Digital signal processing using waveguide networks

1 335~40 BACKGROUND OF THE IN~ENTION This invention relates to the field of digital signal processing and particularly to signal processing useful in digital music synthesis and other applications.

Digital music synthesis has attracted increased interest as data processors have undergone new developments which provide increased performance capabilities. Digital music synthesis has many applications such as the synthesis of stringed, reed and other instruments and such as the synthesis of reverberation.

In actual practice, it has been difficult to provide satisfactory models of music instruments, based upon quantitative physical models, which can ~e practically synthesized on a real-time basis using present-day computers and digital circuitry.

Most traditional musical instruments, such as woodwinds and strings, have been simulated by additive synthesis which consists of summing together sinusoidal harmonics of appropriate amplitude, or e~uivalently by repeatedly reading from a table consisting of one period of a tone ~scaled by an ~amplitude function~) to ~play a note.~ Another method consists of digitally sampling a real musical sound, storing the samples in digital memory, and thereafter playing back the samples under digital control.

FM synthesis as described, for example, in U.S. patent 4,018,121, has also been successful in synthesizing many musical sounds including brasses, woodwinds, bells, gongs, and some strings. A few instruments have been simulated by ~subtractive synthesis~ which shapes the spectrum of primitive input signals using digital filters.

All of the foregoing methods (with the occasional exception of subtractive synthesis) have the disadvantage of STAN13/006 -2- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 - 1 335~40 not being closely related to the underlying physics of sound production. Physically accurate simulations are expensive to compute when general finite-element modeling techniques are used.

Digital reverberation has also been difficult to achieve. Although digital music synthesis has employed digital reverberation as a post-processing function for many years, there still remains a need to be able to simulate with digital signal processing the quality of reverberation which exists in natural listening-space environments. The basic acoustics of reverberation in natural listening-space environments, such as concert halls, has a long history with many different design theories.

The goal of digital reverberation is to produce digital signal processing methods which simulate the effect that a good concert hall or other good n listening space~ has on sound. This goal is made difficult because typical good listening spaces are inherently large-order, complex acoustical systems which cannot be precisely simulated in real-time using commonly available computing techniques.

In architectural acoustics, an understAnding of digital reverberation is important in the design of concert halls with good acoustical qualities. In digitally synthesized music, reverberation is a part of the synthesized instrumental ensemble and provides enrichment to the sound quality.

For these reasons, there have been many attempts to capture the musically important qualities of natural reverberation in digital music synthesis.

Digital room simulation (reverberation) has been implemented by simulating specular reflection in actual or approximate concert-hall geometries.

The diffusive scattering of sound in such natural listening environments must be considered in order to obtain high-quality reverberation models. However, practical models which accommodate diffusing reflections have been beyond the reach of present computing power when applied to listening spaces of nominal size over the audio frequency band.

STAN13/006 -3- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 ` 1 335~40 In another implementation of digital reverberation, an approximation to the impulse response between two spatial points in a real concert hall has been recorded. The effect of the hall on sound between these two points can ~e accurately simulated by convolving the measured impulse response with the desired source signal. Again, this imple~entation leads to a prohibitive computational burden which is two to three orders of magnitude beyond the real-time capability of typical present-day mainframe computers.

The current state of high-quality digital reverberation based upon large ~concert hall) spaces, although well understood, is too expensive to synthesize by computation. Because there is much detail in natural reverberation that is not important perceptually, models for reverberation need to be simplified so as to become computationally practical.

One example of a computationally simple model relies upon convolving unreverberated sound with exponentially decaying white noise thereby producing the heretofore best known artificial reverberation. The digital reverberator designs based upon quantitative physical models need to be replaced by models based upon simple computations which retain the qualitative behavior of natural listening space reverberation.

Some basic building blocks of presently known digital reverberators include cascaded and nested allpass networks, recursive and non-recursive comb filters, tapped delay lines, and lowpass filters. The early reflections can be exactly matched for a fixed source and listener position using a tapped delay line, and the late reverberation can be qualitatively matched using a combination of allpass chains, comb filters, and lowpass filters. Using a lowpass filter in the feedback loop of a comb filter simulates air absorption and nonspecular reflection. These known techniques for reverberation have been the basis for reverberation design for more than a decade. Although these elements do provide some essential aspects of STAN13/006 -4- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 3~`5~40 reverberation, especially for smoothly varying sounds at low reverberation levels, they do not provide reverberation on a par with excellent natural listening-space environments.

In accordance with the above background, there is a need for techniques for synthesizing strings, winds, and other musical instruments including reverberators in a manner which is both physically meaningful and computationally efficient. There is a need for the achievement of natural and expressive computer-controlled performance in ways which are readily comprehensible and easy to use.

SUMMARY OF THE 1NV 1~ ION The present invention is a signal processor formed using digital waveguide networks. The digital waveguide networks have signal scattering junctions. A junction connects two waveguide sections together or terminates a waveguide. The junctions are constructed from conventional digital components such as multipliers, adders, and delay elements. The number of multiplies and additions determines the number of signal-scattering junctions that can be implemented in the waveguide network, and the number of delays determines the total delay which can be distributed among the waveguides interconnecting the junctions in the waveguide network.

The signal processor of the present invention is typically used for digital reverberation and for synthesis of reed, string or other instruments.

The waveguides of the present invention include a first rail for conducting signals from stage to stage in one direction and a second rail for conducting signals from stage to stage in the opposite direction. The accumulated delay along the first rail is substantially equal to the accumulated delay along the second rail so that the waveguide is balanced. The first rail is connected to the second rail at junctions so that signals conducted by one rail are also conducted in part by the other rail.

STAN13/006 -5- 86/10117-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 t 335~40 Lossless waveguides used in the present invention are bi-directional delay lines which sometimes include embedded allpass filters. Losses are introduced as pure attenuation or lowpass filtering in one or both directions.

The signal processor in some applications includes a non-linear junction-connected to provide an input signal to the first rail of the waveguide and to receive an output signal from the second rail of the waveguide. The non-linear junction in some embodiments receives a control variable for controlling the non-linear junction and the signals to and from the waveguide.

In one embodiment, a digital reverberator is formed by a multi-branch network of lossless digital waveguides.

In another embodiment, a reed instrument is synthesized by a non-linear junction terminating a digital waveguide. A primary control variable, representing mouth pressure, is input to the non-linear junction (also controlled secondarily by embouchure variables). The ~unction simulates the reed while the digital waveguide simulates the bore of the reed instrument.

In another embodiment, a string instrument is synthesized. A primary control variable, representing the bow velocity, is input to the non-linear junction. The non-linear junction represents the bow-string interface (including secondary controls such as bow force, bow angle, bow position, and friction characteristics). In the stringed instrument embodiment, two digital lossless waveguides are connected to the non-linear junction. The first waveguide represents the long string portion (from the bow to the nut) and the other waveguide simulates the short string portion (from the bow to the bridge). A series of waveguides can also be used to implement the body of, for example, a violin, although in such a case there is normally no direct physical interpretation of the waveguide variables.

In particular embodiments, the reflection signal or signal coefficients introduced into the waveguides from the STAN13/006 -6- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 nonlinear junction are obtained from a table. ln one embodiment, the nonlinearity to be introduced into the waveguides is f(x) where x is the table address and also the incominq signal sample in the waveguide (a travelling wave sample). In another embodiment, the values g(x)-f(x)/x are stored in the table and the ta~le is addressed by x. Each value of g~x) addressed by x from the compressed table (where g(x) is called a coefficient) is then multiplied by x, x~g(x) which thereby produces the desired value of f(x).

$n accordance with the above ~ummary, the present invention captures the musically important qualities of natural instruments in digital music synthesis with digital processing techniques employing digital waveguides which are computationally efficient and therefore capable of inexpensive real-time operation.

The foregoing and other objects, features and advantages of the invention will be apparent from the followinq detailed description in conjunction with the drawings.

In another aspect the present invention provides a real time tone generation system comprising means for providing a control signal; wave transmission means for transmitting wave signals, the wave transmission means including an input and an output, a first signal path for receiving signals from the input, a second signal path for providing signals to the output, the first signal path being coupled to the second signal path, and delay means in at least one of the signal paths for delaying signals; junction means having a first input for receiving the control signal, a second input for receiving a signal from the output of the wave transmission means and an output for providing a signal as the input to the wave transmission means which is a function of at least the value of the control signal and the value of the signal received from the output of the 1 ~35840 wave transmission means so as to cause a signal to propagate in the wave transmission means; and tone signal extracting means for extracting a tone signal from at least one of the wave transmission means and junction means.

In another aspect the present invention provides a real time tone generation system comprising means for providing a control signal whose value is substantially independent of the pitch of a tone to be generated; wave transmission means for receiving the control signal and electronically simulating wave transmission which occurs in a natural musical instrument so as to create at least one wave signal in the wave transmission means in response to the control signal, said wave signal interacting with the control signal so as to be sustained; and means for extracting a signal from the wave transmission means as a musical tone signal.

In another aspect the invention provides a real time tone generation system comprising control means for providing a control signal; at least first and second wave transmission means, each including an input and an output, a first signal path for receiving signals from the input, a second signal path for providing signals to the output, coupling means for coupling signals from the first path to the second path, and delay means in at least one of the signal paths for delaying signals propagating therethrough; junction means, having a first input for receiving the control signal, a plurality of second inputs each of which is connected to the output of a wave transmission means, and a plurality of outputs each of which is connected to the input of a wave transmission means, the junction means providing outputs whose values are functions of the values of the control signal and the outputs of the wave transmission means, said control signal causing periodic signals to be -7a 1 335840 generated and propagate in the wave transmission means;

and musical tone extracting means for extracting a musical tone signal from at least one of the junction means and wave transmission means.

In another aspect the invention provides an electronic musical instrument for synthesizing musical tones comprising control signal generating means for generating a control signal for controlling the generation of a musical tone; a signal processing unit including wave transmission means and converting means for processing a musical tone signal, said wave transmission means for conducting said tone signal, including a first rail in one direction, a second rail in the opposite direction of said first direction, and a plurality of delays connected to at least either of said rails and selectively interconnectable, said converting means for determining a conversion characteristic on the basis of said control signal and for converting said signal transmitted from said wave transmission means in accordance with said conversion characteristic and transmitting the converted signal to the wave transmission means; controlling means for controlling the interconnection of said delays to be connected in response to a selected tone pitch of said musical tone, and output means for extracting a signal from the signal processing unit as a synthesized musical tone.

In a further aspect the invention provides a tone generation system comprising control means for providing a control signal, wave transmission means for initially creating a wave signal in response to the control signal and thereafter sustaining the wave signals by interacting the control signal with the wave signal, -said wave transmission means including a signal path and means for delaying signals propagating therethrough; and means for 1 335840 providing at least one wave signal from the wave transmission means as an output tone signal, wherein the pitch of the output tone signal is a function of the amount of delay imparted by the wave transmission means.

In a further aspect the invention provides a real ti~e tone generation system comprising a wave transmission section having first and second ends, a first signal path for propagating signals from the first end to the second end, and a second signal path for propagating signals from the second end to the first end;

a first junction connected to the second end of the wave transmission section, said first junction receiving a signal from the first path and transmitting signal to the second path; wherein `at least one of the first path, second path and first junction has at least one delay element therein; a second junction connected to the first end of the wave transmission section, said second junction receiving at least a control signal and a signal from the second path and providing a signal to the first path which is a function of said received signals, wherein a periodic wave signal is created in the wave transmission section as a result of the interaction of the control signal and the signal received from the second path; and an output for providing an output signal from at least one of the wave transmission section or junctions as a tone signal.

In a further aspect the invention provides a method of generating tones in real time, comprising the steps of providing a signal propagation network having an input for receiving signals, an output for providing signals and a signal propagation path coupling the input and output and including a delay therein; introducing a control signal to the input of the network to initiate signal propagation in the network; repeatedly performing processing of the control signal and a signal from the -7c - 1 3J5840 _ 7d_ output of the network and providing the result to the input to cause a periodic signal to be created which is propagated through the network; and extracting a signal from the network as a musical tone signal.

In a further embodiment the present invention provides a digital reverberation system comprising a branched network including a plurality of branches formed of digital waveguides and a plurality of junctions interconnecting the waveguides, wherein each waveguide includes two digital delay lines running parallel to each other for propagating signals in opposite directions and having a first end and a second end, said first end having an input to a first delay line and an output from a second delay line and said second end having an input to the second delay line and an output from the first delay line, each waveguide having at least one of its ends connected to a junction; at least one of the junctions has at least three waveguide ends connected to it and signals arriving at each junction from a particular waveguide end are partially transmitted to every other waveguide end connected to the junction and partially reflected back to said particular waveguide end; means for introducing losses into signals propagating in the network; input means for providing an audio input signal to be reverberated to the network; and output means for providing at least one reverberation output signal from the network.

In another aspect the present invention provides a reverberation system comprising a branched network including a plurality of branches formed of waveguides and a plurality of junctions interconnecting the waveguides, wherein each waveguide includes two signa paths running parallel to each other for propagating signals in opposite directions wherein at least one of the paths includes a delay, each waveguide having a first _ 7e 1 335840 end and a second end, said first end having an input to a first path and an output from a second path and said second end having an input to the second path and an output from the first path, each waveguide having at least one of its ends connected to a junction; at least one of the junctions has at least three waveguide ends connected to it and signals arriving at each junction from a particular waveguide end are transmitted by a predetermined amount whichmay include zero to other waveguide ends connected to the junction and reflected back by a predetermined amount which may include zero to said particular waveguide end: means for introducing losses into signals propagating in the network; input means for providing an audio input signal to be reverberated to the network; and output means for providing at least one reverberation output signal from the network.

BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 depicts a simple closed waveguide network.

FIG. 2 depicts a 3-port waveguide network.

FIG. 3 depicts a junction of two waveguides.

FIG. 4 depicts a cascade waveguide network in accordance with the present invention.

FIG. 5 depicts one embodiment of a cascade waveguide network section.

FIG. 6 depicts another embodiment of a cascade waveguide network section.

FIG. 7 depicts a third embodiment of a cascade waveguide network section.

FIG. 8 depicts a pipelined embodiment of a waveguide filter.

FIG. 9 depicts a travelling pressure wave 'at a general point within a waveguide section.

1 335~40 FIG. 10 depicts a normalized-waveguide digital filter.

FIG. 11 depicts a wave-normalized waveguide junction.

FIG. 12 depicts a transformer junction.

FIG. 13 depicts transformer-coupled waveguide junction.

- FIG. 14 depicts a non-linear junction, controlled by a control variable, and connected through a plurality of ports to a plurality of waveguides.

FIG. 15 depicts a terminating non-linear junction controlled by a control variable and connected to a waveguide network.

FIG. 16 depicts further details of the non-linear junction of FIG. 9.

FIG. 17 depicts a block diagram representation of the waveguide of FIG. 9.

FIG. 18 depicts a non-linear junction connected to first and second waveguides.

FIG. 19 depicts a waveguide reverberator.

FIG. 20 depicts a typical waveguide employed in the FIG. 19 reverberator.

FIG. 21 depicts details of the FIG. 20 waveguide.

FIG. 22 is a signal processor forming a music instrument using digital waveguides.

FIG. 23 is a graph of a waveform representing the data stored in the table of FIG. 16 for a reed instrument.

FIG. 24 is a graph of a waveform representing the data stored in the table of FIG. 16 for a string instrument.

DETAILED DESCRIPTION Lossless Networks - FIG. 1 In FIG. 1 a network 10 is a closed interconnection of bi-directional signal paths 11. The signal paths 11 are called branches or waveguides, designated 11-1, 11-2, 11-3, 11-4, and 11-5 and the interconnection points are called nodes or junctions, designated 12-1, 12-2, 12-3, and 12-4.

STAN13/006 -8- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 An example of a simple network is shown in FIG. 1 where each signal path is bi-directional, meaning that in each waveguide there is a signal propagating in one direction and an independent signal propagating in the other direction. When a signal reaches a junction, one component is partially reflected back along the same waveguide, and other components are partially transmitted into the other waveguides connected to the junction. The relative strengths of the components of the transmitted or n scattered" signals at each junction are determined by the relative characteristic impedances of the waveguides at the junction. In FIG. 1, the waveguides 11 intersect at the junctions 12.

A lossless waveguide, such as each of the waveguides in FIG. 1, is defined specifically as a lossless bi-directional signal branch. In the simplest case, each branch or waveguide 11 in a waveguide network 10 is merely a bi-directional delay line. The only computations in the network take place at the branch intersection points (nodes or junctions). More generally, a lossless waveguide branch may contain a chain of cascaded allpass filters. For practical reverberator and other designs, losses are introduced in the form of factors less than 1 and/or low pass filters with a frequency response strictly bounded above by 1 in magnitude.

A closed lossless network preserves total stored signal energy. Energy is preserved if, at each time instant, the total energy stored in the network is the same as at any other time instant. The total energy at any time instant is found by summing the instantaneous power throughout the network waveguides 11. Each signal sample within the network contributes to instantaneous power. The instantaneous power of a stored sample is the squared amplitude times a scale factor, g. If the signal is in units of ~pressure~, "force~, or equivalent, then g = 1/Z, where Z is the characteristic impedance of the waveguide 11 medium.

If the signal sample instead represents a ~flow~ variable, STAN13/006 -9- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 - 1 335840 such as volume-velocity, then g = Z. In either case, the stored energy is a weighted sum of squared values of all samples stored in the digital network 10.

N-Port Network - FIG. 2 In FIG. 2, an N-port network 14 is shown in which for N=3, three waveguides, called ports, leave the network with one port 15 designated for input and two ports 16-1 and 16-2 designated for output.

Such a structure is suitable, for example, for providing stereo reverberation of a single channel of sound. Note, however, that really in FIG. 2 there are three inputs(15, 16-1, 16-2) and three outputs(l5, 16-1, 16-2) because in an N-port, each waveguide connected to the network provides both an input and an output since each waveguide is bi-directional.

An N-port network 14 of FIG. 2 is lossless if at any time instant, the energy lost through the outputs, equals the total energy supplied through the inputs, plus the total stored energy. A lossless digital filter is obtained from a lossless N-port by using every port as both an input and an output. This filter is the general multi-input, multi-output allpass filter.

An N-port network 14 is linear if superposition holds.

Superposition holds when the output in response to the sum of two input signals equals the sum of the outputs in response to each individual input signal. A network is linear if every N-port derived from it is linear. Only linear networks can be restricted to a large and well-understood class of energy conserving systems.

Lossless Scattering - FIG. 3 Consider a parallel junction of N lossless waveguides of characteristic impedance Zi (characteristic admittance ri = l/Zi) as depicted in FIG. 3 for Nz2.

If in FIG. 3 the incoming traveling pressure waves are denoted by Pi, where i = l,...,N, the outgoing pressure waves are given by Eq.(l) as follows:

STAN13/006 -10- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 3358~0 Pi Pj Pi Eq.(l) where Pj in Eq.(1) is the resultant junction pressure given as follows:

Eqs.(2) N where ai = (2ri)/(Qr1rQ) For N=2, pj ~1Pl + 2P2 ~1 = (2rl) / (rl + r a2 = 2 ~ a1 Define the reflection coefficient by k=1-1, then from Eq. 1, j (~1 - 1) Pl + ~2P2 P1 = kP~ k)P2 P2 ~1Pl ~2 1)P2 2 (k + l)Pl - kP+2 Thus, we have, for N=2, Pl = P2 + k(Pl - P2) P2 = P1 + k(Pl - P2) Eqs. (3) which is the one-multiplier lattice filter section (minus its unit delay). More generally, an N-way intersection requires N multiplies and N-1 additions to obtain Pj, and one addition for each outgoing wave, for a total of N multiplies and 2N-1 additions.

The series flow-junction is equivalent to the parallel pressure-junction. The series pressure-junction or the parallel flow-junction can be found by use of duality.

STAN13/006 -11- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 Cascade Waveguide Chains - FIG. 4 The basic waveguide chain 2S is shown in FIG.4. Each junction 26-1, 26-2, . . ., 26-i , . . ., 26-M enclosing the sy~mbol ki(t) denotes a scattering junction characterized by ki(t). In FIG. 4, the junction 26-i typically utilizes multipliers(M) 8 and adders(~) 7 to form the junction. In FIG. 4, the multipliers 8-1, 8-2, 8-3 and 8-4 multiply by the factors ~l+k(i)], [-ki(t)], [l-~i(t)], and [ki(t)], respectively. An alternative junction implementation 26 ' -i of FIG. 13 requires only one multiply. The junction 26-2 in FIG. 4 corresponds, for example, to the ~unction 12 in FIG. 3. Similarly, the delays 27-1 and 27-2 in FIG. 4 correspond to the branches 15 and 16, respectively, in FIG. 3.

The Xelly-Lochbaum junctions 26-i and one-multiply junction 26'-i (see FIG. 13) or any other type of lossless junction may be used for junction 26.

In particular, the two-multiply lattice (not shown) and normalized ladder (FTG. 11) scattering junctions can be employed. The waveguide 25 employs delays 27 between each scattering junction 26 along both the top and bottom signal paths, unlike conventional ladder and lattice filters. Note that the junction 26-i of FIG. 4 employs four multipliers and two adds while junction 26 ' -i of FIG. 13 employs one multiply and three adds.

Waveguide Variations - FIGS. 4-14 Reduction of junction 26 to other forms is merely a matter of pushing delays 27 along the top rail around to the bottom rai~, so that each bottom-rail delay becomes 2T seconds (z 2T~ instead of T seconds z T. Such an operation is possible because of the termination at the right by an infinite (or zero) characteristic impedance 6 in FIG. 4.

In the time-varying case, pushing a delay through a multiply results in a corresponding time advance of the multiplier coefficient.

Imagine each delay element 27 in FIG. 4 being divided into halves, denoted by a delay of Tl2 seconds. Then any STAN13/006 -12- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 3~5~`0 waveguide can be built from sections such as shown in FIG.

5.

By a series of transformations, the two input-signal delays are pushed through the junction to the two output delays. A similar sequence of moves pushes the two output delays into the two input branches. Consequently, we can replace any waveguide section of the form shown in FIG. 5 by a section of the form shown in FIG. 6 or FIG. 7.

By alternately choosing the structure of FIG. 6 and 7, the structure of FIG. 8 is obtained. This structure has some advantages worth considering: (1) it consolidates delays to length 2T as do conventional lattice/ladder structures, (2) it does not require a termination by an infinite characteristic impedance, allowing it to be extended to networks of arbitrary topology (e.g., multiport branching, intersection, and looping), and (3) there is no long delay-free signal path along the upper rail as in conventional structures - a pipeline segment is only two sections long. This structure, termed the "half-rate waveguide filter", appears to have better overall characteristics than any other digital filter structure for many applications.

Advantage ! 2) makes it especially valuable for modeling physical systems.

Finally, successive substitutions of the section of FIG. 6 and reapplication of the delay consolidation transformation lead to the conventional ladder or lattice filter structure. The termination at the right by a total reflection (shown as 6 in FIG. 4) is required to obtain this structure.

Consequently, conventional lattice filters cannot be extended on the right in a physically meaningful way. Also, creating network topologies more complex than a simple series (or acyclic tree) of waveguide sections is not immediately possible because of the delay-free path along the top rail. For example, the output of a conventional structure cannot be fed back to the input.

STAN13/006 -13- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 Energy and Power The instantaneous power in a waveguide containing instantaneous pressure P and flow U is defined as the product of pressure and flow as follows:

P = PU = (P + P )(U + U ) = P + P Eq.(4) where, P+ = P+ U+ = Z(U+)2 = r(p+)~ P~ = P~ U~ = -Z(U~)~ = _r(p-)2 Eqs.(S) define the right-going and left-going power, respectively.

For the N-way waveguide junction, we have, using Rirchoff's node equations, Eq.(6) as follows:

N N N j ~ i-l i i i-l j i j i-l i Eq.(6~ Thus, the N-way junction is lossless; no net power, active or reactive, flows into or away from the junction.

Quantization Effects While the ideal waveguide junction is lossless, finite digital wordlength effects can make exactly lossless networks unrealizable. In fixed-point arithmetic, the product of two numbers requires more bits (in general) for exact representation than either of the multiplicands. If there is a feedback loop around a product, the number of bits needed to represent exactly a circulating signal grows without bound. Therefore, some round-off rule must be included in a finite-precision implementation. The guaranteed absence of limit cycles and overflow oscillations is tantamount to ensuring that all finite-wordlength effects result in power absorption at each junction, and never power creation. If magnitude truncation is used on all STAN13/006 -14- 86/lOtl7-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335~0 outgoing waves, then limit cycles and overflow oscillations are suppressed. Magnitude truncation results in greater losses than necessary to suppress quantization effects.

More refined schemes are possible. In particular, by saving and accumulating the low-order half of each multiply at a junction, energy can be exactly preserved in spite of finite precision computations.

Signal Power in Time-Varying Waveguides The convention is adopted that the time variation of the characteristic impedance does not alter the traveling pressure waves Pi. In this case, the power represented by a traveling pressure wave is modulated by the changing characteristic impedance as it propagates. The actual power becomes inversely proportional to characteristic impedance:

EP+i(x,t)]2_lp-i(x,t)l2 Pi(x,t)=Pi(x,t)+Pi(x,t)= Eq.(7) zi(t) This power modulation causes no difficulties in the Lyapunov theory which proves absence of limit cycles and overflow oscillations because it occurs identically in both the finite-precision and infinite-precision filters. However, in some applications it may be desirable to compensate for the power modulation so that changes in the characteristic impedances of the waveguides do not affect the power of the signals propagating within.

Consider an arbitrary point in the ith waveguide at time t and distance x=ct measured from the left boundary, as shown in FIG. 9. The right-going pressure is Pi(x,t) and the left-going pressure is Pi(x,t). In the absence of scaling, the waveguide section behaves (according to our definition of the propagation medium properties) as a pressure delay line, and we have Pi(x,t)=Pi(O,t-T) and Pilx,t)=Pi~O,t+T)=Pi(cT,t-T+T). The left-going and right STAN13/006 -15- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 - 1 3358~0 going components of the signal power are [Pi(x,t~l2/Zi(t) and tPi(x,t)12/Zi(t), respectively.

Below, three methods are discussed for making signal power invariant with respect to time-varying branch impedances.

Normalized Waveguides Suppose the traveling waves are scaled as the characteristic impedance changes in order to hold signal power fixed. Any level can be chosen as a reference, but perhaps it is most natural to fix the power of each wave to that which it had upon entry to the section. Ir. this case, it is quickly verified that the proper scaling is:

i i ))/(Zi(t T ) ) ] Pi ( ~ t - T ) ~ X=C T Eqs.(8) Pi(X,t)=[ (Zi(t) ) / (Zi(t-T+T) ) ] ~ Pi (cT,t-T+T) In practice, there is no need to perform the scaling until the signal actually reaches a junction. Thus, we implement Pi (cT, t)=gi(t)Pi(O,t-T) Eqs.(9) ~ Pi(O,t)=gi(t)Pi(cT,t-T) where gi(t) I(Zi(t))/(Zi(t-T))]~ STAN13/006 -16- 86/10/17-14 Atty.

Docket No.: STAN4983-2DELStan Ref: S85-043 1 335~40 This normalization is depicted in FIG. 10. In FIG. 10, each of the multipliers 8 multiplies the signal by gi(t) as given by Eqs.(9). In the single-argument notation used earlier, Eqs.(9) become _ i(t T) gi(t)Pi(t-T) Eqs.(10) i(t)=gi(t~Pi(t) This normalization strategy has the property that the time-varying waveguides (as well as the junctions) conserve signal power. If the scattering junctions are implemented with one-multiply structures, then the number of multiplies per section rises to three when power is normalized. There are three additions as in the unnormalized case. In some situations (such as in the two-stage structure) it may be acceptable to normalize at fewer points; the normalizing multiplies can be pushed through the scattering junctions and combined with other normalizing multiplies, much in the same way delays were pushed through the junctions to obtain st~n~rd ladder/lattice forms. In physical modeling applications, normalizations can be limited to opposite ends of a long cascade of sections with no interior output "taps. n To ensure passivity of a normalized-waveguide with finite-precision calculations, it suffices to perform magnitude truncation after multiplication by gi(t). Alternatively, extended precision can be used within the scattering junction.

Normalized Waves Another approach to normalization is to propagate rms-normalized waves in the waveguide. In this case, each delay-line contains STAN13/006 -17- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 Pi(X,t)=Pi(x~t)~[zi(t)]~ Eqs.(ll) Pi(x,t)=Pi(x,t)/[Zi(t)]~ We now consider P~(instead of P~) to be invariant with respect to the characteristic impedance. In this case, i )tlzi(t)] = Pi(0~t-T)/[Zi(t-T)3~= P+(t T) The scattering equations become [Zi(t)]~ Pi(O,t) = _+ ~ i( )I[ i-l(t)] Pi_l(CT,t)-ki(t)lZi(t)l~ Pi(0 t) ~ Eqs.(12) [Zi-l(t)] Pi_l(CT~t)~ ki(t) [Zi_l(t)]~ Pi_l(ct,T)+ll-ki(t)l [Zi(t)] Pi(t) or, solving for Pi, P.(O,t) = i [( i_l(t))/(Zi(t))] Pi l(cT,t)-ki(t)p-(o t) ~ Eqs.(13) ki(t)Pi_l(ct,T)+[l-ki(t)] [(Zi(t))/(Zi-l(t))] Pi(t) But, (Zi-l(t))/(Zi(t)) = (l-ki(t))/(l+ki(t)) Eq.(14) whence STAN13/006 -18- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 [l+ki(t)] I(Zi-l(t))/(zi(t))li = ~1 ki(t)] [(Zi(t))/(Zi-1(t))] = [l-ki(t)]~ Eq.(15) The final scattering equations for normalized waves are p+i(ort)=ci(t)pi-l(cT~t) Si~t~Pi~ ' Eqs.(16) Pi_l(CT~t)=si(t)Pi_1(Ct,T)+Ci(t)Pi(t) where si(t) _ ki(t) Eqs.(17) ci(t) ~ [l-ki(t)3~ can be viewed as the sine and cosine, respectively, of a single angle ~i(t)=sin 1tki(t)] which characterizes the junction. FIG. 11 illustrates the Relly-Lochbaum junction as it applies to normalized waves. In FIG. 11, the multipliers 8-1, 8-2, 8-3, and 8-4 multiply by the factors [l-ki(t)]~, -ki(t), [l-ki(t)]~, and ki(t), respectively.

In FIG. 11, ki(t) cannot be factored out to obtain a one-multiply structure. The four-multiply structure of FIG. 11 is used in the normalized ladder filter (NLF).

Note that normalizing the outputs of the delay lines saves one multiply relative to the NLF which propagates normalized waves. However, there are other differences to consider.

In the case of normalized waves, duals are easier, that is, changing the propagation variable from pressure to velocity or vice versa in the ith section requires no signal normalization, and the forward and reverse reflection coefficients are unchanged. Only sign-reversal is STAN13/006 -19- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 - . 1 33~0 required for the reverse path. Also, in the case of normalized waves, the rms signal level is the same whether or not pressure or velocity is used. While appealing from a "balance of power~ standpoint, normalizing all signals by their rms level can be a disadvantage. In the case of normalized delay-line outputs, dynamic range can be minimized by choosing the smaller of pressure and velocity as the variable of propagation.

Transformer-Coupled Waveguides Still another approach to the normalization of time-varying waveguide filters is perhaps the most convenient of all. So far, the least expensive normalization technique is the normalized-waveguide structure, requiring only three multiplies per section rather than four in the normalized-wave case. Unfortunately, in the normalized-waveguide case, changing the characteristic impedance of section i results in a changing of the reflection coeficients in both adjacent scattering junctions. Of course, a single junction can be modulated in isolation by changing all downstream characteristic impedances by the same ratio. But this does not help if the filtering network is not a cascade chain or acyclic tree of waveguide sections. A more convenient local variation in characteristic impedance can be obtained using transformer coupling. A transformer joins two waveguide sections of differing characteristic impedance in such a way that signal power is preserved and no scattering occurs. It turns out that filter structures built using the transformer-coupled waveguide are equivalent to those using the normalized-wave junction described in the previous subsection, but one of the four multiplies can be traded for an addition.

From Ohm's Law and the power equation, an impedance discontinuity can be bridged with no power change and no scattering using the following relations:

STAN13/006 -20- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 ~ 1 335840 ~P+i~ /[Zi(t)] = rp~ Zi_l( )] Eqs.(18) [Pi] /[zi(t)~ = [Pi_l] /[Zi-l(t)] Therefore, the junction equations for a transformer can be cho$en as i gi(t)Pi_l Eqs.(l9) Pi-l gi ( ) i where, from Eq. (14) i ~ [( i(t))/(Zi_l(t))] = [(l+ki(t))/(l-ki(t)]~ Eq.(20) The choice of a negative square root corresponds to a gyrator. The gyrator is equivalent to a transformer in cascade with a dualizer. A dualizer is a direct implementation of Ohm's law (to within a scale factor) where the forward path is unchanged while the reverse path is negated. On one side of the dualizer there are pressure waves, and on the other side there are velocity waves. Ohm's law is a gyrator in cascade with a transformer whose scale factor equals the characteristic admittance.

The transformer-coupled junction is shown in FIG. 12.

In FIG. 12, the multipliers 8-1 and 8-2 multiply by gi(t) and l/gi(t) where gi(t) equals [Zi(t)/Zi-l(t)~ . A sing junction can be modulated, even in arbitrary network topologies, by inserting a transformer immediately to the left (or right) of the junction. Conceptually, the characteristic impedance is not changed over the delay-line STAN13/006 -21- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 portion of the waveguide section; instead it is changed to the new time-varying value just before (or after) it meets the junction. When velocity is the wave variable, the coefficients gi(t) and gi (t) in FIG. 12 are swapped (or inverted).

So, as in the normalized waveguide case, the two extra multipliers 8-1 and 8-2 of FIG. 12 provide two extra multiplies per section relating to the unnormalized (one-multiply) case, thereby achieving time-varying digital filters which do not modulate stored signal energy. Moreove~, transformers enable the scattering junctions to be varied independently, without having to propagate time-varying impedance ratios throughout the waveguide network.

In FIG. 13, the one-multiply junction 26'-i includes three adders 7-1, 7-2, and 7-3, where adder 7-3 functions to subtract the second rail signal, Pi(t), from the first rail signal, [Pi_l(t-T)]~gi(t)]. Junction 26'-i also includes the multiplier 8 which multiplies the output from adder 7-3 by ki(t). FIG. 13 utilizes the junction of FIG.

12 in the form of multipliers 8-1 and 8-2 which multiply the first and second rail signals by gi(t) and l/gi(t), respectively, where gi(t) equals [(1-ki(t))/(l~ki(t))]~.

It is interesting to note that the transformer-coupled waveguide of FIG. 13 and the wave-normalized waveguide (shown in FIG. 11) are equivalent. One simple proof is to start with a transformer and a Relly-Lochbaum junction, move the transformer scale factors inside the junction, combine terms, and arrive at FIG. 11. The practical importance of this equivalence is that the normalized ladder filter (NLF) can be implemented with only three multiplies and three additions instead of four multiplies and two additions.

The limit cycles and overflow oscillations are easily eliminated in a waveguide structure, which precisely simulates a sampled interconnection of ideal transmissions line sections. Furthermore, the waveguide can be transformed STAN13/006 -22- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 - 1 3~584~ into all well-known ladder and lattice filter structures simply by pushing delays around to the bottom rail in the special case of a cascade, reflectively terminated waveguide network.

Therefore, aside from specific round-off error and time skew in the signal and filter coefficients, the samples computed in the waveguide and the samples computed in other ladder/lattice filters are identical (between junctions).

The waveguide structure gives a precise implementation of physical wave phenomena in time-varying media. This property is valuable in its own right for simulation purposes. The present invention permits the delay or advance of time-varying coefficient streams in order to obtain physically correct time-varying waveguide (or acoustic tube) simulations using st~ rd lattice/ladder structures.

Also, the necessary time corrections for the traveling waves, needed to output a simulated pressure or velocity, are achieved.

Waveguide Networks with Non-Linear Junction - FIG. 14 In FIG. 14, a plurality of waveguides 53 are interconnected by a non-linear junction 52. In the particular embodiment of FIG. 14, the junction 52 has three ports, one for each of the waveguide networks 53-1, 53-2, and 53-3.

However, junction 52 can be an N-port junction interconnecting N waveguides or waveguide networks 53. The control variable register 51 provides one or more control variables as inputs to the junction 52. In FIG. 14 when only a single waveguide is utilized, the single waveguide becomes a special case, single-port embodiment of FIG. 14. Single port examples of the FIG. 14 structure are described hereinafter in connection with reed instruments such as clarinets or saxophones. Multi-port embodiments of the FIG. 14 structure are described hereinafter in connection with stringed instruments such as violins. A multi-port variation of the FIG. 14 structure is also described hereinafter in connection with a reverberator. Many other STAN13/006 -23- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 , 1 335840 instruments not described in detail can also be simulated in accordance with the present invention. For example, flutes, organs, recorders, basoons, oboes, all brasses, and percussion instruments can be simulated by single or multi-port, linear or non-linear junctions in combination with one or more waveguides or waveguide networks.

Waveguide with Non-Linear Terminating Junction - FIG. 15 In FIG. 15, a block diagram representation of a waveguide 53 driven by a non-linear junction 52 is shown.

The non-linear junction 52 provides the input on the first rail 54 to the waveguide 53 and receives the waveguide output from the second rail on lines 55. A control variable unit 51 provides a control variable to the non-linear junction 52. The FIG. 15 structure can be used as a musical instrument for simulating a reed instrument in which case the control variable unit 51 simulates mouth pressure, that is the pressure drop across a reed. The non-linear junction 52 simulates the reed and the waveguide 53 simulates the bore of the reed instrument.

Non-Linear Junction - FIG. 16 FIG. 16 depicts further details of a non-linear junction useful in connection with the FTG. 15 instrument for simulating a reed. The control register input on lines 56 is a control variable, such as mouth pressure. The control variable forms one input ~negative) to a subtractor 57 which receives another input (negative) directly from the most significant bits of the waveguide second rail on lines 55. The subtractor 56 subtracts the waveguide output on lines 55 and the control variable on lines 56 to provide a 9-bit address on lines 69 to the coefficient store 70 and specifically the address register 58. The address in register 58 provides the address on lines 68 to a table 59 and to a multiplier 62. The table 59 is addressed by the address, x, from address register 58 to provide the data, g(x), in a data register 61. The contents, g(x), in the STAN13/006 -24- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335~40 ~, data register 61 are multiplied by the address, x, from address register 58 in multiplier 62 to provide an output, x*g(x), in the multiplier register 63 which is equal to f(x). The output from the multiplier register 63 is added in adder 64 to the control variable to provide the first rail input on lines 54 to the waveguide 53 of FIG. 15.

In FIG. 16, table 59 in one embodiment stores 512 bytes of data and provides an 8-bit output to the data register 61. The multiplier 62 provides a 16-bit output to the register 63. The high order 8 bits in register 63 are added in saturating adder 64 to the 8 bits from the variable register 51' to provide a 16-bit output on lines 54.

Similarly, the hiqh order 8-bits from the 16-bit lines 55 are subtracted in subtractor 57.

The contents of the table 59 in FIG. 16 represent compressed data. If the coefficients required are f(x) from the compressed table 70, only a fewer number of values, g(x), are stored in the table 59. The values stored in table 59 are f(x)/x which are equal to g(x). If x is a 16-bit binary number, and each value of x represents one 8-bit byte of data for f(x), table 59 is materially reduced in size to 512 bytes when addressed by the high-order 9 bits of x. The output is then expanded to a full 16 bits by multiplication in the multiplier 62.

Further compression is possible by interpolating values in the table 59. Many table interpolation techniques are well known. For example, linear interpolation could ~e used. Interpolation can also be used to compress a table of f(x) values directly, thus saving a multiply while increasing the needed table size, for a given level of relative error.

Other examples include a double look-up, address normalization, root-power factorization, address and value quantization, address mapping to histogram. Other compression techniques can be employed.

The manner in which the data values for a reed instrument are generated is set forth in APPENDIX A.

STAN13/006 -25- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 t 37`5~40 In FIG. 17, further details of a schematic representation of the waveguide 53 are shown. The waveguide 53 includes a first rail receiving the input on lines 54 and comprising a delay 65. A terminator 67 connects the delay 65 to the second rail delay 66 which in turn provides the second rail output on lines 55.

In an embodiment where the FIG. 16 signal processor of FIGS. 16 and 17 simulates a reed instrument, the terminator 67 is typically a single pole low-pass filter. Various details of a clarinet reed instrument in accordance with the signal processor of FIGS. 16 and 17 appear in APPENDIX B.

To simulate clarinet tone holes, a three-port scattering junction is introduced into the waveguide. Typically, the first three or four adjacent open tone holes participate in the termination of the bore.

In FIG. 17, the terminator 67 includes a multiplier 74, an inverting low-pass filter 72 and a DC blocking circuit 73. The multiplier 74 multiplies the signal on line 75 from the delay 65 by a loss factor gl where gl is typically 1-2 4 = 0.9375 for a clarinet. The output from the multiplier 74 is designated yl(n) where n is the sampled time index. The output from the low-pass filter 72 is designated y2(n)~ and the output from the DC blocking unit 73 is designated y3(n).

For a clarinet, the low-pass filter 72 has a transfer fun¢tion H12(Z) as follows:

H12(Z) = -(l-g)/(l-gZ Therefore the signal Y2(n) output from the low-pass filter 72 is given as follows:

Y2(n) = (g-l)Yl(n) + gy2(n-1) In the above equations, g is a coefficient which is typically determined as equal to 1-2 k where k can be any selected value. For example, if k is 3, g is equal to .875 STAN13/006 -26- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335~40 and g equal to 0.9 is a typical value. As another example, 1-2 +2 = 0.90625.

In FIG. 17, the transfer function, H23(Z), of the DC blocking circuit 73 is given as follows:

H23(Z) = (1-Z l)/(l-rZ 1) ;

With such a transfer function, the output signal y3(n) is given as follows:

3 Y2(n) - y2(n-1) + ry3(n-1) In simulations, the value of r has been set to zero.

In actual instruments, DC drift can cause unwanted numerical overflow which can be blocked by using the DC block unit 73. Furthermore, when using the compressed table 70 of FIG. 16, the error terms which are produced are relative and therefore are desirably DC centered. If a DC drift occurs, the drift has the effect of emphasizing unwanted error components. Relative signal error means that the ratio of the signal error to signal amplitude tends to remain constant. Therefore, small signal values tend to have small errors whi~h do not significantly disturb the intended operation.

In FIG. 17, for a clarinet, the delays 65 and 66 are typically selected in the following manner. One half the desired pitch period less the delay of the low-pass filter 72 r less the delay of the DC block in unit 73, less the delay encountered in the non-linear junction 52 of FIG. 16.

When a saxophone is the reed instrument to be simulated by the FIG. 16 and FIG. 17 devices, a number of changes are made. The non-linear junction of FIG. 16 remains the same as for a clarinet. However, the waveguide network 53 of FIG. 15 becomes a series of cascaded waveguide sections, for example, of the FIG. 4 type. Each waveguide section represents a portion of the bore of the saxophone. Since the bore of a saxophone has a linearly increasing diameter, STAN13/006 -27- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 each waveguide section simulates a cylindrical section of the saxophone bore, with the waveguide sections representing linearly increasing diameters.

For a saxophone and other instruments, it is useful to have a non-linear bore simulation. Non-linearity results in excess absorption and pressure-dependent phase velocity.

In order to achieve such non-linear simulation in accordance with the present invention, one method is to modify the delays in the waveguide structure of FIG. 8. In FIG.

8, each of the delays, z 2T, includes two units of delay.

In order to introduce a non-linearity, one of the two units of delay is replaced by an all-pass filter so that the delay D changes from Z to the following:

-T -T -T D = [Z ][(h+Z )/(l+hZ )] With such a delay, the output signal, Y2(n) is given in terms of the input signal, y1(n) as follows:

Y2(n) = h*yl(n-1) + yl(n-2) - h*y2(n-1) In the above equations, in order to introduce the non-linearity, the term h is calculated as a function of the instantaneous pressure in the waveguide, which is the sum of the travelling-wave components in the first rail and the second rail. For example, the first rail signal input to the delay, yl+~n) is added to second rail signal yl(n) and then utilized by table look up or otherwise to generate some function for representing h as follows:

h = f[yl(n) + y1(n)~ The delay of the first-order all-pass as a function of h can be approximated by (l-h)/(l+h) at low frequencies relative to the sampling rate. Typically, h is between 1-E and 0 for some small positive E (the stability margin).

STAN13/006 -28- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 3~5~40 Using the principles described, simulation of a nonlinear waveguide medium (such as air in a clarinet bore) is achieved. For clarinet and other instruments, the bore which is modeled by the waveguides of the present invention, includes tone holes that are blocked and unblocked to change the pitch of the tone being played. In order to create the equivalent of such tone holes in the instruments using waveguides in accordance with the present invention, a three-port junction can be inserted between cascaded waveguide sections. One port connects to one waveguide section, another port connects to another waveguide section, and the third port is unconnected and hence acts as a hole. The signal into the third port is represented as P3 and this signal is equal to zero. The radiated signal from the third port, that is the radiated pressure, is denoted by P3. The three-port structure for the tone hole simulator is essentially that of FIG. 14 without the waveguide 53-3 and without-any control variable 51 input as indicated by junction 52 in FIG. 14. The junction 52 is placed as one of the junctions, such as junction 26-i in FIG. 4.

With such a configuration, the junctions pressure, PJ, is given as follows:

3 + pJ = ~ aip where, ai = 2ri/(r1 + r2 + 3)' r i = characteristic admittance in ith waveguide Pi PJ Pi PJ lPl + 2P2 = a1Pl + (2 - a1 - a3)P2 + + + P1 = PJ - P1 = (al~1)P1 + 2P2 + + a _ P+ p = p - P2 = lPl + ( 2 1) 2 STAN13/006 -29- 86/10/17-14 Atty.

Docket No.: STAN4983-2DE~Stan Ref: S85-043 I 335840 P3 = PJ - P+3 = PJ (tone hole output) (rl + r2)/2, open hole Let, r3 = 0, closed hole Then, _ ¦1, open hole ; a3 ~ ¦, closed hole 1-1, open hole a2 = 2-al, closed hole Then with P+ = P+ - P2, we obtain the one multiply tone-hole simulation:

+ _ _ + 2 1 ~ Pl P2 ~ P~, (open hole) In a smooth bore, r 1 = r 2 = r and r 3 = B r, where B is -the cross-sectional area of the tone hole divided by the cross-sectional area of the bore. For a clarinet, g=0.102 and for a saxophone, g=0.436, typically. So we have:

B r, open r3 ~ Br = = 0, closed Then, al = a2 = 2r/(2r+gr) = 2/(2+g) a a3 = 2B/(2+B) = Ba, There is now a single parameter STAN13/006 -30- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 375~40 2/(2+B), open 1, closed So, the tone hole simulation is given by PJ a(Pl + P2) (if open) 1 J P2 P2 + (-l)Pl = P2 (if closed) 2 J Pl QPl + ~-l~P2 = Pl (if closed) Summary:

0.95, clarinet 0.821, saxophone 3 B~ PJ ~(Pl + P2) l J 2 J 2 2/~2+B), open 1, closed a = bore radius b = hole radius STAN13/006 -31- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 ~ 3 ~ 4 0 ¦0.102, clarinet B = b~/a~ = I ¦0.436, saxophone = (2a2)/(2a2+b~) - hole open ~ = 1 - hole closed PJ is radiated away spherically from the open hole with a (1/R~ amplitude attenuation.

Reed Simulation In FIG. 23, a graph is shown representing the data that is typically stored in the table 59 of FIG. 16 for a reed instrument. The output signal R (n) on line 54 is as foll~ws:

R (n) = k*P~/2 + Pm(n)/2 The control variable input on line 56 is Pm(n)/2 and the input on line 68 to the table 59 is (P~)/2 = (R (n) - Pm(n)/2) where R (n) is the signal sample on line 55 of FIG. 16.

The table 59 is loaded with values which, when graphed, appear as in FIG. 23. The curve 92 in FIG. 23 has a maximum value of one and then trails off to a minimum value of zero. The maximum value of one occurs between (PL min)/2 and (P~ c)/2. The value (P~ c)/2 corresponds to the closure of the reed. From (P~ c)/2 to (P~ maX)/2 the curve 92 decays gradually to zero. The equation for the curve 92 is given as follows, Curve ~(P~,max P~)/(P~,maX P~,c)] STAN13/006 -32- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 ~ 3 ~ 5840 where ~ = 1, 2, 3, ...

The output from the table 59 is the variable k as given in FIG. 23, that is, k = k[(PQ)/2] Bowed-String Simulation In FIG. 24, a graph is shown representing the data that is typically stored in the coefficient table 59 of the signal table 70 (see FIG. 16) of FIG. 18. The output signals Vs 1 on line 54 and Vs r on line 49 are as follows:

V~ k(V+) ~ V+ + V+ Vs r = k(VQ) * VQ + Vs 1 The control variable input on line 56 is bow velocity, Vb, and the input on line 68 to the table 59 is V~, = Vb - (Vs ,1 + Vs, r) where Vs 1 is the signal sample on line 55 and Vs r is signal sample on line 50 of FIG. 18.

The table 59 is loaded with values which, when graphed, appear as in FIG. 24. The curve 93 in FIG. 24 has a maximum value of one and then trails off to a minimum value of zero to the left and right symmetrically. The maximum value of one occurs between -VQ c and +VQ c From (V~ c) to (V~ max) the curve 93 decays gradually to zero.

The equation for the curve 93 is given as follows, Curve = [(V~ max ~ VQ)t(V~,max ~ VQ,C)] where Q = 1, 2, 3, ...

The output from the table 59 is the reflection coeEficient k as given in FIG. 24, that is, STAN13/006 -33- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 3 ~ 5 ~ 4 0 k = k~(V~l] Compressed Table Variations The compressed table 59 of FIG. 16 containing g(x)=f(x)tx is preferable in that quantization errors are relative. However, alternatives are possible. The entire table compressor 70 of FIG. 16 can be replaced with a simple table. In such an embodiment, the round off error is linear and not relative. For linear errors, the error-tosignal ratio tends not to be constant. Therefore, for small signal amplitudes, the error tends to be significant so that the error may interfere with the intended operation. In either the table compressor embodiment 70 of FIG. 16 or a simple table previously described, the tables can employ compression techniques such as linear, Lagrange and quadratic interpolation with satisfactory results. In a linear interpolation example, the curve 92 of FIG. 23 would be replaced by a series of straight line segments thereby reducing the amount of data required to be maintained in the table.

Also table 59, address register 58 and data register 61 of FIG. 16 each have inputs 94, 95 and 96 from processor 85 (FIG. 22).

The inputs from processor 85 function to control the data or the access of data from the table 59.

Modifications to the data in the table can be employed, for example, for embouchure control for reed synthesis.

Similarly, articulation control for bowed-string synthesis is possible. In one example, the address register 58 has high order address bits, bits 10 and 11, which are supplied by lines 95 from the processor. In this manner, the high order bits can be used to switch effectively to different subtables within the table 59. This switching among subtables is one form of table modification which can be used to achieve the embouchure and articulation modîfications.

ST~13/006 -34- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 - 1 335840 Non-Linear Junction with Plural Waveguides - FIG. 18 In FIG. 18, further details of another embodiment of a non-linear junction is shown connected between a first waveguide 76 and a second waveguide 77. The non-linear junction 78 receives an input from the control variable register 51' and provides inputs to the waveguide 76 on lines 54 and receives an output on lines 55. Also the non-linear junction 78 provides an output to the waveguide 77 on lines 49 and receives an input on lines 50.

In FIG. 18, the non-linear junction 78 includès an adder 57 receiving as one input the control variable from the control variable register 51' on lines 56. The other input to the subtractor 57 is from the difference register 79 which in turn receives an output from an adder 80. The adder 80 adds the inputs on lines 55 from the waveguide 76 and lines 50 from the waveguide 77.

The output from the subtractor 57 on lines 68 is input to the table compressor 70. The table compressor 70 of FIG. 12 is like the table compressor 70 of FIG. 10 and provides an output on lines 69. The output on lines 69 connects as one input to each of the adders 81 and 82. The adder 81 receives as the other input the input from lines 50 rom the waveguide 77 to form the input on lines 54 to the first waveguide 76. The second adder 82 receives the table compressor signal on lines 69 and adds it to the input from the first waveguide 76 on lines 55. The output from adder 82 connects on lines 49 as the input to the second waveguide 77.

In FIG. 18, the waveguide 76 includes the top rail delay 65-1 and the bottom rail delay 66-1 and a terminator 67-1.

Similarly, the second waveguide 77 includes a top rail delay 65-2 and a bottom rail delay 66-2 and a terminator 67-2.

In the case of a violin in which the long string portion is approximately one foot and the short string portion is one-fifth of a foot, the waveguides of FIG. 18 are as STAN13tO06 -35- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 follows. The terminator 67-1 is merely an inverter which changes the sign of the first rail value from delay 65-1 going into the delay 66-1. For example, the changing the sign is a 2's complement operation in digital arithmetic.

Each of the delays 65-1 and 66-1 is the equivalent of about fifty samples in length for samples at a 50 RHz frequency.

The terminator 67-2 in the waveguide 77 is typically ten samples of delay at the 50 RHz sampling rate. The terminator 67-2 can be a single pole low-pass filter. Alternatively, the terminator can be a filter having the empirically measured bridge reflectance cascaded with all sources of attenuation and dispersions for one round trip on the string. Various details of a violin appear in APPENDIX C.

Reverberator - FIG. 19 One lossless reverberator is augmented as sh~wn in FIG. 19 by one or more simple loss factors (typically of the form 1-2 n) in waveguides 30 to set the reverberation decay times to any desired values. The time, T60, over which the reverberation decays 60 dB is arbitrary. This decoupling of reverberation time from structure incurs no loss of generality in the present invention.

Some of the waveguides 30 of the network are determined to give specific early reflections, while others are chosen to provide a desirable texture in the late reverberation. An optimality criterion for the late reverberation is to maximize homogeneity of the impulse response by making it look li~e exponentially decaying white noise.

The waveguide networks of the present invention allow every signal path to appear as a feedback branch around every other signal path. This connectivity richness facilitates development of dense late reverberation. Furthermore, the energy conserving properties of the waveguide networks can be maintained in the time-varying case which allows the breaking up of unwanted patterns in the late STAN13/006 -36- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 reverberation by subtly changing the reverberator in a way that does not modulate the reverberation decay profile.

Finally, the explicit conservation of signal energy provides an easy way to completely suppress limit cycles and overflow oscillations.

In FIG. 19, one typical waveguide reverberator is shown including five waveguides (branches) formed by the waveguides 30-1, 30-2, ..., 30-5. The waveguides 30 are connected to junctions 31 and 32. The waveguides 30-1 through 30-5 have first rail inputs 33-1 through 33-5, respectively, have first rail outputs 35-1 through 35-5, respectively, have second rail inputs 36-l through 36-5, respectively, and have second rail outputs 34-1 through 34-5, respectively. The first rail outputs 35-i, where i has values from 1 to 5, includes the output signals aiP+i, for i = 1 through 5. The outputs 35-i each connect to the summing node 31. Summing node 31 is an adder which adds all of the ~iPi signals to form the junction pressure signal PI. The PI signal connects in common to each of the second rail inputs 36-1 through 36-5. The PI signal at terminal is typically used to provide an output from the reverberator of FIG. 19. In FIG. 19, the input 18 is typically connected to at least one of the waveguides 30 such as waveguide 30-5.

In FIG. 19, the waveguides 30-1 through 30-5 provide the second rail outputs 34-i for i = 1 to 5. The outputs 34-i provide the signals aiRi which in turn connect as inputs to the summing node 32. The summing node 32 sums all of the signals aiRi to form the node signal RI at terminal 19. A second output is typically taken from terminal 19.

Additionally, the RI signal from summing node 32 connects in common to all of the first rail inputs 33-1 through 33-5.

Reverberator Waveguide - FIGS. 20 and 21 In FIG. 20, further details of the waveguides 30 of FIG. 19 are shown. Typically, each of the waveguides 30 in STAN13/006 -37- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 FIG. 19 includes an R junction 37, a lossless waveguide 38, a loss unit 39 and a P junction 40.

In FIG. 21, further details of the typical waveguide of FIG. 20 are shown.

The R junction 37 includes a subtractor 41 and a multiplier 42. The subtractor 41 subtracts Ri from the RI signal to provide the Ri signal on line 43. The multiplier 42 multiplies the Ri times a gain factor, ~i' to provide the signal iR+i signal at output terminal 34-i.

The lossless waveguide 38 includes a lossless delay 45 and a lossless delay 46. The delay 45 delays by a delay, N. With the signal input to the delay on line 43 equal to Ri(t), the delayed output signal on line 47 is equal to Ri(t-N). Similarly the delay 46 delays the input signal Pi(t) by N to form the delayed signal on line 44 equal by definition to Pi(t-N), which is equal to the R+i(t) signal.

In FIG. 21, the loss unit 39, in one particular embodiment, includes a multiplier 24. Multiplier 24 multiplies the signal on line 47 by ~ to provide on the output the Pi(t) signal equal to ~Ri(t-N). While the loss circuit in the form of multiplier 24 has been inserted in the line 47, the loss circuit may alternatively be placed also in any one or more of the lines 43, 44, 47 or 48.

In FIG. 21, the P junction 40 typically includes a subtractor 21 and a multiplier 22. The subtractor 21 receives the Pi signal and subtracts it from the junction pressure signal PI to produce the Pi signal. Multiplier 22 multiplies the P+i signal by ai to form the ~iPi signal.

In summary, the reverberator of FIGS. 19-21 consists of waveguides 30-1 through 30-5 connected together to form an arbitrary network. The waveguides 30-1 through 30-5 can be referred to as "branches" and their points of intersection 31 and 32 as n junctions" or ~nodes".

Reflections are created by a mismatch between the admittances r i of the intersecting waveguides. The admittance is the inverse of the characteristic impedance Zi Setting the waveg~ide admittances all equal is acceptable STAN13/006 -38- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335~0 as long as the waveguide delays Ni are different. Equal characteristic admittances means that when a signal comes into a junction of waveguides, it will be split equally into all outgoing waveguides. In the reverberator of FIG.

19, equal characteristic admittances result in i=2/5 for all i. Choosing a power of Z for the number of branches means ai is a power of Z and can therefore be implemented in binary arithmetic by means of a shift operation.

If a waveguide with small admittance connects to a waveguide of much higher admittance, the pressure wave will be partially reflected with a sign reversal. In the limit:

a pressure wave is completely reflected with a sign reversal when it encounters an admittance which is infinitely larger than the one in which it was traveling;

a pressure wave is completely reflected with no sign reversal when it encounters an admittance which is infinitely smaller than the one in which it was traveling;

a pressure wave is not reflected at all (complete transmission) when it encounters an admittance which is the same as the one in which it was traveling in, the "matched-impedance~ case.

Time-Varying Reverberation - The effect of amplitude modulation of a waveguide admittance is to vary the admittance away from its original value. In order for the network to remain lossless, the sum of incoming scattering coefficients [i of Eq.(2)] must equal 2. Let ri(t) denote the time-varying branch admittances. Then from Eq.(2) )=(2ri(t) ) / ( ~ r i=l N and ~ ~i(t)=2 at all times.

i=l The objective is to vary ~i(t) in a complex waveguide network such that STAN13/006 -39- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335~40 N N ~ ~i(t)=2 and ~i(t)=2ri(t)/1 ri(t) for some waveguide admittance values ri(t).

The easiest case is the two-junction network such as shown in FIG. 19. In this case, the ~i(t) are identical at the two junctions.

One time-varying reverberation technique in the two-junction case is to vary the ri such that r i=c for some constant c. Then N i ) i(t)/C~ andi~ ~i(t)=2 as c- Then i(t)=2ri(t)/c~ andi~l i(t) as required for losslessness of the network. A special case is where ri~rj=ci in pairs. Another method for the time varying case is, at each junction, to provide one "reflection-free port~ (RFP). Such a port is created when the admittance of one waveguide (that connected to the RFP) is equal to the sum of the admittances of all other waveguides meeting at that junction. In this implementation, the waveguide of the RFP has admittance 1, and it does not vary with time. We call this a n special~ waveguide. Since every waveguide must connect to exactly two junctions, a special waveguide provides a RFP at two different junctions simultaneously. (A special waveguide is not very useful as a self-loop at some junction due to the next constraint.) Given a reflection-free port caused by a special waveguide of admittance 1, the sum of the remaining waveguide admittances is 1. Since the waveguide connected to the reflection-free port is time-invariant, the sum of all time-varying admittances will be 1.

STAN13/006 -40- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 3358~0 A simple method for time-varying reverberation using a RFP is to pair off the time-varying waveguides 50 that their admittances sum to 1 in pairs. This pairing is handy because a pair is the smallest number of mutually constrained waveguides that can be arranged. When there are more than two nodes (junctions), simple complementary pairing of time-varying junctions may be difficult.

Musical Instrument - F~G. 22 In FIG. 22, a typical musical instrument, that is signal processor, employing the waveguide units of the present invention is shown. In FIG. 22, a processor 85, such as a special purpose or general purpose computer, generates a digital signal representing the sound to be produced or a control variable for a synthesizer. Typically, the processor 85 provides an address for a random access memory such as memory 86. Memory 86 is addressed and periodically provides a digital output representing the sound or control variable to be generated. The digital sample from the memory 86, typically at a sampling rate Ts (usually near 50RHz), is connected to the waveguide unit 87. Waveguide unit 87 processes the digital signal in accordance with the present invention and provides an output to the digital-to-analog (D/A) converter 88. The converter 88 in turn provides an analog output signal through a filter 89 which connects to a speaker 90 and produces the desired sound.

When the signal processor of FIG. 22 is a reed instrument, the structure of FIGS. 15, 16 and 17 is typically employed for waveguide unit 87. In FIG. 15, the control variable 51 is derived from the processor 85 and the memory 86 of FIG. 22. The structure of FIGS. 15, 16 and 17 for a clarinet uses the FIG. 17 structure for waveguide 53 with a simple inverter (-1) for terminator 67. For a saxophone, the waveguide 53 is more complex, like FIG. 4.

When the signal processor of FIG. 22 is a bowed-string instrument, the waveguide unit 87 in FIG. 22 typically employs the structure of FIG. 18. The control variable input STAN13/006 -41- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 ~35840 to register 51' of FIG. 18 comes from the memory 86 of FIG.

22. The output from the waveguide unit of FIG. 18 is derived from a number of different points, for example, from the terminals 54 and 55 for the waveguide 76 or from the terminals 49 and 50 from the waveguide 77 of FIG. 18.

In one typical output operation, an adder 71 adds the signals appearing at terminals 49 and 50 to provide an input at terminal 20 to the D/A converter 88 of FIG. 22. The sum of the signals in adder 71 corresponds to the string velocity at the location of the bow on the instrument.

When reed and other instruments are employed, it has been found useful to introduce white noise summed with the control variable input to register 51' of FIG. 16. Additionally, the introduction of tremolo and other musical effects into the control variable enhances the quality of the sound produced.

When the waveguide unit 87 of FIG. 22 is a digital reverberator, the waveguide of FIG. 19 is typical with the parameters of TABLE 1.

STAN13/006 -42- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 3J584~ TABLE 1 NlT = 5 ms.

N2Ts = 17 ms.

N3TS = 23 ms.

N4T = 67 ms.

N5T = 113 ms.

Ts ~ 20 microseconds E = O 9 where ¦ E ¦ ~i = 2 (lossless condition) where Osis2 For time-varying reverberation:

~1 = 1 ~2 B1/2 = (1-B )/2 SBl a4 = B2/2 Osg sl ~ = (l-B )/2 What is claimed is:

STAN13/006 -43- 86/10/17-14 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 APPENDIX A COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 1 335~40 ~ Bct 1986i 15 ~2 REOF S~IONSF JOS~ P~GE 1-l C~nnENT Plot recd flou v~r~u~ di~f-r-ntial pr~uraS COnnENT Ver~ion ~ V3 uith ~outh-pr-~ut--in~ r~ t t~bl-;

BEGIN R--dF' C~nnENT Cl tin-t ~tructuta O P (n~ o------ ----->1~)----~ P (nl --->I Uav-guid L-ngth N l---~o--~ Out t o O I ~ O _____I I I 2 0------0 1 l l RC IRC(n)l ~ ~ O O Tablc ~ *) Output aignal <---1~)<------1~-) ~oupa~ I I t ~ (tuo ton--holo~) t t 1-LP O I O O--t--- ¦ P (n)~2 (thi~ xa~pl-) I I out I LP out o< o d l l 0------- ~ ~ O O ~ <---- P (n) ~---¦ Uav-guido L-ngth N l<---o - ~ b O O O P- - nouth pre~ure (con~tant) O Loua~ Ga;n i~ clo~e to (-1) at all frequencie~ uith increa~ing attenuation at high fr-quencie~ 0 5ell output ;~ co-ple~-ntary hi9hp~.

If H(z) i~ the loupa ~tran~for function beil output i~ 1-H k) (Gell i~ ~ ~requenc1-dc~cnd~nt b~au ~piitt-r ) O ~hon ton~ hol~(~) opencd dela~ Iine get~ a r-f~oction at ~ach open tone hole Con~eauentl~ ~uch 1-~- nerg~ got- to b-il In hig~ rogi~ter~ ~ot~ hol-~ and b-ll g-t a good--i~-d ~ignal l-vel O R~fl~ction coefficient RC i~ 1 fro- 2~Pbp-P- betue-n -1 and - 1 or ~o then fall- to 9 around 2 and decrea~-- ther~after pretty !oul~ .

RECUIRE 'Il<> OELlnlTERS OEFINE ~- COnrENT RE3U R JOSLI R O LIB JOS) SDURCE!F'LE:

REW R~ RECORn R atLlB JOSl' SOURCE!F LE RECU R 'nYlO lEO LIB JOS~ SOURCE!FIL-:

REW Rt OlSPLA R-O[LlB JDSI SOUR~E!F LE:

INTEGER PROCEDURE Sign(REAL Val) RETURN(IF V~ THEN 0 EL _ IF Val>G THEN 1 ELSE -1) B~OLEAN PROCEDURE FindZ~ro(nEFER3 ~~ REAL Z REAL PRCCEOURE F REAL X-in Xna~ XB dX) WnnEN- Find fir-i 2ero of F~X) ~tarting at XS t-pping dX BEGIN FindZero INTEOER c~ o~ RE~L X x~xe:

c~ Sign(F(X)) C~ E (c~+l) Of BEGIN 1 GEGIN Z~X ~ETLRN(TRUE) END ~1 ~HILE (X X~dX) LEO X-ax AND ~--1 00 c~Sign(FlX)) ~] UHILE (X~X-dX) OE a X-in AND c~-1 W c~ Sign(F(X));

ELSE ~RINT(' Findzcro Proc~aure Sign i~ bro~on ) END 2 ~ X IF NOT (X-in LEC X LEO X-ax) THEN BEGIN z ~ (xnin nAX x nlN xna~ RETURN(F~LSE) END RETURN(TRUE);

ENC 'FindZero ;

-4't S~AN13/000 Al. 86/09/30-5 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 APPENDIX A COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFOR~ JUNIOR UNIVERSITY 1 335~4~ 7 Oct 19D6 15:~2 REEDf SAlnNSF.JOSl PAOE 1-2 J Configurat;or~ const~nt~ and d-claration OEFINE NPd. 1e24 # Nu-b r o outh-to-oor- dift r-ntial pr-~ur-~ OEFINE NPdp- 1824 J Nu-O-r o inco-ing pr-~-ur- uav- valu~ to tr~ OEFINE NE-3- 2 ; J Nu-o-r ot Oouchure- to tr~ ~EF NE R-alBot ~ 38 INT GER Tr ce DEF NE D buglx~ - ~ (Tr~c- LAND 2-x) ~ OEF NE u^p~Edl - I IF O-bug(1) THEN Dp~Ed 1:

OEF NE Op~Ed2 - I IF Oebug(2) THEN Op~Ed 1 REAL ARRAY Garr Y3rr ACarr~l NPd~NE-~ RE~L ARRAY RCarr PdArr ~l:NFm tr~] STRING P-tr Xstr INTEGER iPd j iE-o l REAL P Pdc Pd dPd U-lou A-p Alpha Pd in Pd-ax E-b x0 x0- E-in E-ax dE EF-ax REAL C Zc Rho A8 Pi Ro Sr Pdr Bet~ APdc Pdpnin Pdpnay StepReduce BOOLEAN T-~ tnode IF Tr ce.~ THEN ~race~7 IF StepReduc--O T~EN StepReduc-~ 81 Sti~U~T(0 2);

IF Pi LEG 0 T~EN BEGIN SetUp p; ~ 4eATAN(1) C ~ 1B90* 2*2 a4 # Air spe-d in c-/~ec Oru 20 d-gr--- C 1 atRho ~ 0 ~ 129; # Air den~it~ in gJc-t3 ~a-e condition~ Ro ~ Q 7~ ~ Radiu~ ot clarinet bore in cU~lou ~ 3 # Reed flou a-plitude Ic-t3t~ec) for Pd-x-1 9r t 1 4 -6 ~ Reed ~tiffne~ in dune/c-t3 (d~ne-g*c-/~ec-2 # xQ t 8 06 ~ Reed opening (c-) at r-~t (Backu~) X0 t 0 15 # Reed opening (c-) at re~t (-~ ea~ure-entI Pdr t 1--8 ~ Fraction of pres~ure drop felt bu reed (!1 Ph4~ic~ the valu- her- ie o;zarr-;

# It ha~ been ~et to give the de~ired Oehavior EF-ax ~ 88*5r ~ Pressure applied to reed at axi-u- e-Oouchure END SetUp ;

A2 ~ PitF~t2 J Cro~ ectional area o- clarinet oore in c-t2 2b t RhoJC~8 ~ Characteri~tic i~ ce of clarin~t bore Alpha t Pdr/Sr # Alpha~Pd - Change in reed po~ition (c-) v~ pr urop Beta ~ EF-axtSr J Beta~Pd - Change in reed po~ition at a~ e o 1.1 Pdc~ /Alpha ~ Reed clo~ure pr~ure (d~ne/c-t2) APdc ~ UE~i(Pdc) # Ue gue~ti-ate pre~ure in unit~ o re-d-ciosure pressuro J A-p ZbJUflou ~ Convert reed-apertur- flou into trav-ling bore prersure IF A~p CE~ 0 rHEN Aop AinR-al(A-p Scaie f_- ReedAd~ittanc-t8OreAd-ittance (- for reristor test) ) IF A-p<8 THEN BEGI~ MlNT( Replacing reed b~ fixed aperture of rpecific ad itt~nce- J~ ~ Cr~f) Te~tnod-~TRUE IF A-p>l THEN PalNT( You h~ve ~ t reed ~deittanc- gr~at-r than bor- ~!! CrLf) PRINT( Solution i~ CrLf CrL Pb- - (1-A p~ op) * Pbp Aop~ A-p) ~ Pn CrLf CrLf) PRINT( Reflection coefficiont i~ RC - (1-A p)~ A p) CrLt) END ELSE Tc~tnode~FALSE Pdoin ~ -S*x2~1 pha; # Reed clo~ur- pres~u?- ir -xa/Alpha Pd-~x ~ -Pd-ins ~ na~ diff r-nti~l pr-~ur- (Shouldn t 9O po-itive oft-n?):Pdpnin ~ 2~Pdc ~ nini-u- inco-ing pre~-ur- uav- ic tuic- r- d clo~urPdpna~ ~ -Pdpnin ~ naxi-u- inco-in~ prer~ur- c~n ~e ~ r-tlection of in ST~13/000 A2. 86/09/30-5 Att:y.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 APPENDIX A 1 3 J 5 8 ~ O COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY Oct 1986 15 ~2 QEE~F S~l0NSF J~S) PAGiE 1-3 E-in~O E-ax~l: J E-Douchur- 18~ > liC~t e~ouchur- 1 .~ ti~ht~ tE (E--~-E-in)/(NE-b-1) Fu^R iE-~ l STEP 1 UNTIL NE-D DO 8EGIN Eloop Eeo E~in~(iE b-1)~dE J Curr-nt bouchure dPd~(Pd ax-Pd in)/(NPd-1) FOR iPd 1 STEP 1 UNTIL NPd DO 8EGIN lloop RE~L G x:

I iPd~(iEeo-1)*NPd Pd ~ Pd in ~ (iPd-1)~dPd ~ Pr---ur- drop acro-a r--d bor- to outh x ~0 ~ Alpha*Pd: ~ R--d po-ition du- to pr---ur- drop x . x - B-ta*E-b: ~ E bouchur- i- n add-d forc- on reed rpring x - x r~x S ~ O ie r--d cloeure x~ i- r--d po- at re~t Xarrtll ~ x IF T--tnod- T~EN G - A-p~E~CitPd) ~ Plain reeiotor ELSE G A~p*(AES(Pd)~xt2)t 67s ~ 7~ ne- ~louGi~Jnrre~ ~oOrop.Pd Garr[l~ ~ (If Pd~S THEN G flSE -G) END lloop END Eloop P-tr Alph~. ~Cvf~(Alph~)~ Pdc- 6C~ J(Pdc)~ P- ~C~f~(P)~ XS. ~C~t~lXS)~ - Pd (du~e/ --2) IF NOT Te~t~ode THN DpyEd1(Xarr NPd P~tr X po~ition (c-i Pd-in Pd-ax) DpuEd1(G~rr NPd P~tr Pre~we G (dune/c-t2) Pdein Pdnax Pdnin Pdnaxi;

WnrENT Plot AC re lection gain v~ Pn FOR i-~1 STEP 1 UNTIL NE-D 00 ôEGlN fOR iPd-2 SrEP 1 UNTIL NPd DO BGIN REAL Gp ~ E~ti-ate of derivative of G RAL ~Cgain # ~C gai n i~ Gp~ Gp):

INTEGER 1 Pd ~ Pd-in ~ (iPd-1}*dPd ~ Current oper at ing point l-iPd~(iE-b-1)~NPd Gp ~ (Garrtll-Garr~ )/dPd:

ACga;n (1-Gpl~ Gp) ~ AC re lection oef icient at current op pt ~Carrll~ ~ ACgain END;

~Carrtl~(iE-b-1)~NPd~ ~Carrt2~(iE-o-l)JNPd~ ~ Extrapolate 1 ~aeple l~ft END;

Dp~JEdl(~ca-r.Npd.-Acgain(pd)-u~t-.-ptDe~ptbp-.pdein~pdnax) 8EGIN OpyAC INTEGER Id ;E~b:

STRING T~ REAL Y-in Y-ax R~L ARRAY Bu 11 NPd~ Y-in ~ ninArr(NPd NE b AC~rr) Y-in Yn~x ~ nax~rr(NPd~NE~ ACarr) IF Y-in GEO Yuax THEN 8GIN PRINT( AC gain PLOT IS CONSTANT Y-in CrLf)s CALL(S EXIT ) NO OPYOVL(AC~rr.NPd.ld~.- AC Pb-/PDp ~.

Pd- -AC RlC'.Yoin.Y-~x.idllin.Pdn~x.FALSE.TRUE.K-~NPd~11~80);

FOR i E-~2 STEP 1 UN~ I L NE~ DO EIEGIN O~Loop' ARflE~L~(Bu-~l~ .AC~rr~(;E~1)~NPd~l].lNPd) OPYOVL (Bu f . NPd . I d . NULL . ~ . Y~ i n . Y-~x .

Pd~l i n, Pd~l~x, TRUE . FAL ):

ENO ûp~Loop';

STAN13/000 A3. 86/09/30-5 Atty.

Doc~et No.: STAN4983-2DELStan Ref: S85-043 1 3358~ APPENDIX A . . ...CQPYRIGHT.1986.- THE BOARD--OF--TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct 19~6 15~2 RfFDf S~IONSf J06I PAGE 1 UH ~E TRUE OD ~EI N (t~lNCHUL). ~ OR T~. U THEN Op~Urt(Id ACRC PLT ~:CiE IF T-- R OR T-- r THEN ~EGIN oUIC~!COOE PGIOT 2 END ~urit-(ld.8) END _SE WNE END Or-l-(ld) END Opu~C C~rnENT Touard the ~olltion ot G(Fd) ~ Pd - Pdp . 8 Repl~c- C(Pd) b~ G(Pd) ~ Pd (uhich i~ approxi oa tel~ Pd ~inc- G-~Zb/Z-)*Pd ~nd Zb< Z-) FOR iE-b~l STEP 1 UNTIL NE-D OC fOR iPd~1 STEP i UNTIL NPd 00 G~rrll~iPd~(iE-b~ NPd~ ~ Garrtl~ ~ (Pd ~ Pd-in ~ (iPd-1)*dPd);

Dp~Ed1(C~rr NPd P-tr G~Pd Pdoin Pd-~x) CDrnENT hbu ol~e for apertur~ r~ ction co-ftici-nt FOR iE-o~1 STEP 1 UNTIL NE~D W DEGIN Sol~ REAL PRDCEDURE U dpPd(REAL Pd INTE OE R iE-c) Roturn G(Pd)~Pd u~ing Garr~1:NPd~ for ~ coar~- r- wlt and u-~ lin~ar intcrpolation bct~-en ~-pleIf R~turn G~rr~1~tNpd-1)~t(Pd-Pdnin)/(Pdn~x-Pdnin))~liE-b-1~sNpdl;

aEGlN GPdpPd INTEGER il i2 io~;

OUN BOOLE~N Initcd OUN REAL ,D RE~L g rndx ri1;

IF NOt Initcd THEN SEGIN Init Init~d~TRUE ~ (Npd-l)i(Pd~ax-Pdnin) D ~ 1-(Npd-l)sPd~in/(Pdnax-Pdnin):

END Init rndx ~ a~Pd~b ~ Oc~ired loo~up index;

# Oo lin-~rl~ int-rpol~t-d loo~up:

i1 ~ rndx IF Trac- ~NO NDT (1 LEO il LEO Npd) rHEN PRINT( 2*Pdp-Pn exc~ed~ Pdnin or Pdnax CrLf For Pd- Pd. indx . il CrLf) ril ~ il:

g ~ rndx - ri1 (1 rux il nIN Npd~;

i2 ~ 1) nlN Npd;

iof ~ (iE b-1)*Npd iof:

i2 ~ i2 ~ io';

RErURN(G rr~ g~(Garr~i21-G~rrli11)):

END GPdpPd J U nou tind the solution Pd of th- ~u~tion G(Pd) ~ Pd - Pdp 8.

~or th~ co pl~t~ r~ng- of Pdp v~lu-~ to ~ ~upport d in op r~tion u~ing a geneo~l local zero inde- For -tabl- op-r~tion o~ th- reed th~ u~ve-i - .- lin~ ~hould int-r--ct t~ n-g~tive-ro~i~t~nco portion ot th rccd i-~ c~ curvo in onl~ on- pl c- Thi~ ~n~ G(Pdl~Pd ~hould De ~trictl~ incr-~ino uhich i pli-- th ~ t-nco onl~ on- 2 ro RE~L Pdp PD- Pd dP~p rc -4~STAN13/000 A4. 86/09/30-5 Atty.

Docket No.: S~AN4983-2DELStan Ref: S85-043 APPENDIX A l 3~ J - -- - COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 1 Oct 198E 15 ~2 RfEDF SAltNSF JOS~ PAGE l-S INTEGER iPdp l REAL PROCDURE GPdpPd~Pdp(RE}ERENC REAL Pd): RETURN(GPdpPd(Pd iE b)-Pdp);

E b - E-in~iE o-l)~dE J Curr-nt bou~hura PRINTI Solving ixed-point probl-a for bouchur~ E-b CrLf) dPdp (Pdp-ax-Pdp-in~/(NPdp-l) X~tr ~ E-b- 6Cvt~(E-o)6 Pdc- ~Cvt~(Pdcl~' Pd (d~n-~c-t2) Pd (Pdnin n~X B nlN Pd~ax) ~ Fir-t ~-arch ~-t to idpoint in r~ n ca~e Pdp ~ Pdpnin-dPdp;

- fQR ipdp~l STEP 1 UNtlL NPdp OO BEGIN PdpLoop Pdp ~ Pdp ~ dPdp Searc~ fro- pre~iou~ ~olution tor nou ~olution IF NQT Find2 ro(Pd GPdpPd Pdp Pdnin Pdnax.Pd dPd~ THEN PRINT(' No zerc CrLf) # Rcpeat at reduccd ~tep ~iz~ (a~-u-e~ interpol-tion in GPdpPd) IF NOT FindZero(Pd GPa~r~ ~dy Pdnin Pdnax Pd dPd~Sitc~n~ e) THEN PRINT( No 2ero CrLt) I ~ iPdp~(iE-b-l)~NPdp;

PdArr~l~ Pd rc ~ (IF ABB(idp) OEû dPd~StopReduc- THEN 2*(Pd/Pdp)-1 ELSE rc) RC rr~ rc IF Oeoug(3) ANO ABSlPdp) LE0 (Pdp~ax-Pdpnin)/2Q THEN aEGlN ~oeG REAL ARRUY TupArr~1 NPd*NEub~ INTEGER jE-b jPd l FûR jE-o~l STEP 1 UNTIL NE-o DQ ~EGI~ INTEGER ndK iof FOR jPd~1 STEP 1 UNTIL NPd OO T-pArrtl~(jPd+~jE-b-1)~NPd)~ Garr~l~ - Pdp ndx~1~(Npd-1)~((Pd-Pdnin)/iPdnax-Pd~in)) IF NOT (1 LEO ndx LEO Npd~ nHEN 8EGIN PRINT( REALITY fAI W RE );

ndx ~ (1 nAX ndx nIN Npd) ENO iof~(jE-b-l)~Npd - TxpArr~ndx~iot]~T-pArrtl~iof~ # nar~ found 2ero-cro~ing END:

Op~Ed(T-pArr.NPd.-G(Pd)~Pd-Pdp V5.

Pd or Pdp- &CvF~(Pdp)~ ~X~tr G~Pd-Pdp Pdnin Pdnax) ENO ~ceG END PdpEoop ErD Solv-:

0pyEd2tPdArr NPdp Pd(Pdp) '-X-tr Pd Pdpnin Pdpnax Pdpnin Pdpn~x) DpuEd2(RCarr NPdp Reflection co-ff v~ Pdp for ~X~tr RC Pdpnin Pdpnax) ~ WnrENT PRACTICAL NOTE RCarr i~ uritten out (u~ing tho uritc-filo option o Op~Ed) to a di~k filc uhich i~ u~rltHJ road b~ JCLA laft-r ~uitablo for-~t conver~ion~ and u~od for tho clarin t i-ul~tion r--d t~bl OEGIN DPyAII INTEGER Id i STRI~G l~ X~tr RE~L Y-in Y-ax REAL ~RRAY Buf~1 NPdp~ X~tr ~ Exb- U v ~(E-o)~ Pd~c. U vf~(Pdc)- Pdp (dun-/c-t2) Y-in ~ n in~rr(NPdp~NE-o Pd~rr) Yna~ ~ n~xArr(NPdp NE-o Pd~rr) Ycin ~ Pdpnin STAN13/000 A5. 86/09/30-5 A1:ty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 33~840 APPENDIX A C~PYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct 19~6 15~2 REEDf.~l oYSF,JOSl P~GE 1 4 y~x ~ Pdpn~s IF Y-in OE C Y-~x THEN BECIN PRlNT(X-tr,CrL~,- PLOT IS C~NST~NT - ,Y-in,CrL-): C~LLlO,-fXlT') END aPYOVL(Pd~rr,NPdp,ld_0.

Pd(Pdp): ~X-tr,-Pd-,Y-in,Y-~x,Pdpnin,Pdpn-x,F~L,TRUE.NE-~NPdp lB00);

FOR i~2 STEP l UNTIL NE-o OO 9EGIN Op~Loop ARRBLT(8u-~1~,Pd~rrl(i-l)sNPdp~1],NPdp) OpyovL(But~Npdp~ld.NuLL.NuLL~yoin~y~x.pdpnin~pdpnax.TRuE~F~L ):

END Op~Loop-:

UH-LE TRUE 00 BE IN f (T-_lNCH~L).-u- OR T-~-U- THEN D w Urt(ld~-po-~cys(iE-b)~-.pLT-) LSE IF T--'R- OR T---r- THEN BEGIN-OUICK!C~OE PGIOT 2, END: nurito(ld~0) END LSE DONE END:

Or-l-(ld);

Y-in ~ nin~rr(NPdpsNE-b,RC~rr3 ax~rr(Npdp~NE-b.R~rr) -F Y-in GEO Yoax THEN EGIN PRlNT(X-tr,CrLf PLOT IS C~NSTANT .Y-in.CrL-)- CALL(0,-EXIT-~ ENDPyGvL(RcArr~Npdp.ld-8~-po-~pdp:-6x~tr~-R.c~-~y-in~yu~x Pdpnin~Pdpnax.R~LSE TRUE.NE-~NPdp~ FOR i 2 STEP l UNTIL NE-b DO BEGIN Dp~Loop ARRBLT(Buf[1~,RC~rr~(i-1)sNPdp~1l,NPdp) DPYOVL(Bu~Npdp~ld~NuLL~NuLL.y-in~y-ax~pdpnin~pdpnax;nRuE.F~LciE):

END DpyLoop-:

UH LE TRUE 00 F (T~INCHUL).-~- OR T~.-U- THEN DpyUrt(ld RC-~CVS(iE-c)~-.PLT-) LSE IF T~.-R' OR T5--r- THEN BEGIN OUICK!C W E PGIOT 2, END; nUrite(ld,8) END L9E OoNE END:

Orel~(ld):

ENO Op~AI~' END ReedF -4q STAN13/000 A6. 86/09/30-5 Atl:y.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 APPENDIX B 1 3 ~ 5 8 t ~ COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIO~? UNIVERSITY ~ ûc~ 19~6i 15 -5 JCL~ NFF~S~n JOSl PAGiE 1-1 Cu^nnEN- E~p- i--nt~l Cl~rin-t ~od~tic~tior~ hi~tor~ 3_ruA_J~ v r~ion i~ ir~t toot lu~-d ~ith JCLA E- ~t th~t tie-) I -r~R- Ei - ~dd-d D~ I I ùutput hig~p~ ilt-r ~nd ch ng d Li e~nir~ I -rUR- E - Pl~c-d ûC bloc~ng c~p- in oor2~-nUR- S - Add~d ~i r or~point control of RC t~ole Rf TO 00 - ~dd clipp-r T~ run R JETS~n ~cl~Cl ~CALL~ EX Jcl~ RE~D JE-SU~ ~or eo~e infor~ation Rel~ant file~ ~i~O JET ~nto JET NS~ JE~n ~AItLlB BILl UOP INS S~ltLI~ 91Li ncCLS T5LtLlB 81LI LoUER OEF~NE~ nv'il S~LIB/O r REOUIRE 'C~K> OELlnlTER'i;

REDEFI~E ~. COnnENr R~lt~lNE Ttru c step I until ~ ALT c'l75~ CR c'1S~ CRLF-c('lra~'12)~ ~B-c('11~ )~ Rtlt~lNE C~-c~lF Tr nHEN Repc t ELSE Null!n-~age)~ oEFINE ~ itenod- - UritelO~t~Gl!einu~!GO~Sine ;

INTEGER -;

REoUIRE Need OPYENV REL~i~n JOS1 nESS~GE REoUlRE OPYENV REL~S~n JQS~ Lû~O!nOOULE PqOCEDURE wclr; ouick~coo pgiot 2 nd COrrENT cl~r ~11 pi c~ o~ 91 ?ROCEOURE Uh-re(SrRING ~rg(NU~L)I 3EGIN U~ r~ IF ~rg-NULL nHEN aEGlN H~rINTEGER i~ oEFlNE N -~- 6G' j. i~ SrRlNG ~RRUY Ut1 N a~I OUN INrEGER S--d IF S -c - O rHEN 3EGIN S-ed - ~EnoRY~'17] 6-~d~ 9~nU~l(Sced) END i ~0 U ;~ ;n th oorning P~D r ;

U ~ ~n th~ b-t~roo Ll -'up5-~ir~-:

U '~ nn t~ bu p r' U ~ in th- ~ nt of r-~ult~ U J ~-~r- ~ou l-~t ~ct itU ~ D-tu ~n s- 41-U , ~ on tt~ to O~tonU , ~'in th~ ui2~rd~ -5~ STAN13/006 Bl. 86/09/30-;

n,~ Ot ~ T~N49R3-2DEI, Stan Re~: S85-043 APPENDIX B 1 ~ 5 .~ ~ O COPYRIGHT 1986 - ,THE 80ARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY Oct 19~Ei 15:-5 JCU.NFFISAn, QS~ PAGE 1-2 U~ I- in tho ooitu ri~ ;

Ul l ~n t~- bottlU~ di~cl~ r Ul I~ -ncruptcd ~ithout ~ p~uord U ~ -uh-rU . loo--lu ~p-~ing U ~ - i t u r-U ~ in th- corr du p U ~ on uo~r or-h- d U . in th- fortun- coo~iU ~ ~long uith flo~ting undoru- r 'C-' ;

ur,~ uh-r- it uill n-v r b- r-~d U ~ ~o-~uherU . ~oo-uh-r- r-~on~bl~ U ~ to~-n ot our ~Dpr-ci~tion U ~ ~ littlc ~it to th~ lo~t ;

U ~ a~ ~ rc-inder ot J ~eb-llU I- und-r thc bo~rdual~ ;

U I~ in tribute to the bit buc~-t~;

U ] in ~n ~rtitici~llu int~llio-nt plac- ;

U ~ on ~our U2 tor-~ :

U ~ in uour credit ~ilU ~ in uour letter~ ho a U ~ in t~e Icnc ~tr~ct-:

U ~ und-r con~id-r~tion U ~ in P~tte ~ ~il tile U ~ in ~ bug-report to BIL-:

U ~ in DAJ ~ tloor ~p~cU ~ in ~crou ;

U i~ ~nd than unplaced U I~ ~h~r- 40u ui~ PR NT(U ~N(0)~i-.45 nux 1~1;

END Uher~ ELSE PRlNt(- Uhere ~l~e? ) E~ Uh r-COnnENt t~Loo~ - t~ol~ loo~up obj-ct iNTEGE~ OBJECT TbLoo~ArgStr);

9ELilN INTEGE~ i.Dl4~dr~sc~l 014Port ~odl InLoc OutLoc~ol~Lcn;

300LE~N GotP-- GotOut GotAdr POI~TER CurArg;

REAL OuitTilu~port~nodl~lnLoc-outLoc~ol~Adr~lnv-lid-p<;

I~Len_OuitTi~;otP--~TRUE;

CotOut-rALSE;

~;o tAdr~FALsE;

oR i~l SrEP 1 UNTIL ArgNu- 00 OEGIN CurArgrG tArg;

IF CurArgdNULL_RECORO TUEh C~SE I nt~-g n~glCurArgl OF BGIN '~-por t~ ~ull n~.-~s-~ JUddrc~l 0l4Adr-lntn~g V~l ~urArgl J5c~ Sc~l~lntn~g V~l ~urArgl;

~InputA~ InLoc-lntll g:V~I [CurArg~ JOutputl OutLoc-lntn~g:V~I lCur~g~:

Jl on1 OI~L~lntn~4:~l ICurArgl tchl E~EGII~ P~tchIF P-Tu~p- ~spcn-g i 1 'CurArgl ) -rbd i ~ i r _po -51 STAN13/006 B2. 86/09/30-5 ~ttv.

Docket ~o.: STAN4983-2DELStan Re~: S85-04~ 1 375~40 APPENDIX 8 COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct l9U6 15~5 JCL~ NFFtS~n JOS~ PAOE 1-3 T~EN BECIN nod1-Spc~-g ilt~ur~r9~ Ol~Por ~Spcn-g i21CurAr91s END ELSE BEGIN nodl~Spcn~g 12tCur~rg~;

OI~Port Spcn~o:ilCCurArg~ END - F P-Tw-(Ol~Port)~0~ p~ r~EN Bo~rror~ P~tch li-t d 1~4 i- inv-lid') F P-Tgp-(nod1t~nodi~i-r_p~ TUEN Bo~Error( P~tch li-t odif; r ie ;nv~l;d '~CVtts(nodl) otPcs FALSE;

ND P-tch^ ~Ouit~t~ OuitTi- ~RIn~g V~l~CurArg~ #DurJtionI OuitTi e-Rln~g V~loCurArgl~p~-~/sr~te ~L Bo~Error('T~loo~ c~nnot h~ndle '~Getn-th6d~- ~[lntn-g ~-glCurArg~)) EL O~hE;

END;

~F P~Ch c~lOlyPortl~in~lid-pJ rHFN OI~Port-G-t(D-l~_p- -1 T~101~') IF P Ch c~lnod1)-in~l;d_pe nHEN nod1~G t(~od;ti~r_p- -1 tblnod ) IF P-Chee~(OutLocl inv~lid_pe nHEN ~EGIN GotOut-TRUE; OutLoc~G-t(nbC6u~_Pe -l 'TblOutLoc') EN0 IF Ol~dr-in~lid_pe THEN IF OI~L-n>8 THEN ~IN Jl~dr~GettD-Addr_pe DI~Len 'Tblne- );

otAdr~tRUE;

:~0 ELSE Boxrrorl'Tbioo~ got n-ither ~ ~lid d~ ddr~s~ nor ~ del~ Icngth');

Sa D14(U--(DlyPort) ~ddre~(Ol~dr) node(Rounded_Loot~up) Scal-(Sc~l));

6 ~ bd(Us tnodl),lnputAtlr~oc),nod~(O la~_Unit),O-l ~ (Ol~Port),Output(LutLoc));If OuitTie>0 n~N ~G'N F t;ott'-- THEN Fr~eAll(OuitTin~ Dl~Part.~odl);

F ~atA~r nHEN Fr--(OuitTi-~ Olu,~dr~;

IF CotOut T~EN Fr--(OuitTi-- OutLoc);

END:

RETURN(OutLoc) EN~;

ConnENT l pul--.

Con~t~nt Noi~o CDnnENT l~pulr- In~trur~nt;

PROCEDUR Ipul~e(RE~L Seo Dur A p; INTE~Eq OutLoc):

BEGIN I pul-StopUntil(Be~;

~ On- 2-ro r ~ Ll-nl ~ Labn8! LO . L1! L1 . ~;

S~-rod (nbd-( n- Z--o) Ouit~t(B g~Our) T~r~8 (~-p 1~1 LS~ 19)-1))) G~inS l)~Output(OutL~c).Etc);

END I pul-- ;

C3nrENT St-p In-tru ent;

PROCEDURE Con-t nt(REAL B-g Dur A p: IN~E OE R OutLoc) BEGIN Con-t nt StopUntil(e o);

IF P-Typ-(OutLoc).lodSv P- THEN L-tchSig(OuitAt(Beg~Dur).T-r~ AJF l(l LS~ 19)-1))) O4tputlOutLoc) Etc) EL IF ~T~p~lOutLoci-G nSun_~- nHEN STA~13/00 6 B 3 8 6 /0 9/ 30 ~S ~ , n~k~ ~AN~r~ nFT. ~tan R~f ~-043 1 3 ~ 8 ~ ~ APPENDIX B COPYRIGHT 1986 - THE ~OARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 ûet 1986 1$:4S JCL~.NFF ~i4n.JOs~ P~GE 1 4 Sa GEN(Ouit~t(8cg~0ur~.~ plitud-(2 A~p),OutputloutLoel.

Pha--196).Fr eu nc~(O).Ete) ELSE PRlNt(- Con~t~nt: OutLoe i- not ~ u --org loc~tion!

FND Con-t~nt-:

C~rnENT Noi~- In-truo~nt PROCEu^URE Noi--~RE~L B-g.Our,~-p: INrEGER OutLoe, S -d~S~)~ 9EGIN ~oi~ INTE OER R~nSu StopUnti1(8eg):

RanSu- ~ (IF Acp.l T~EN OutLoe ELSE G<tnlodSu !Pc.-t.-Noi~ Out-i):

Sa~nod(Quit~t(8eg~0ur). ~od-(Uni~o~- noi~ Input~(Z~ro).lnputB(~-ro).Output(RanSuo~.

Coct-~( 1Z54635 LS~ 18).

Co-tfl(O .

Sesl-S(2~,Scal-l~6~.

Tor~S(-6~B6Z3).T-roll-l777777-RUN(S--d)), Ete):

IF ~op NE~ l THEN ~ i~Sig(auit~t(8eg~0ur),0utput(0utLoe).lnput~(RanSu-~.Gain(~ o~.Ete~:

END Noi~ ;

C~nnENT ~ooduind Bor- ~it~ output at bell nd intern l OC bloc~ing INTEGER PRCCEDURE Bore(REUL Beg,Dur,Lg.Fg.Rp.R2 INTE OE R Ll.PbpS~ .Rb~Su ):

8EGIN BoroOEFINE O-e QuitAt(Beg~Our) I~TEGER Fltln,FltOut.C~pl.C~p2.Cap3.DolL-n,~utSuo.Out D lL n ~ (Ll-5)/2: ~ Ll d-l-~ froo PboSuo to PbpSuo;

StopUntil(B-g):

Fltln DI~Lin(C.lnput~(Pb Su ),L-n(D IL-~-3).Etc~ Rg~P- ~ G t(D-Iav-p-) Fltln ~ 31~Lin(... U--(RguPo FltOut ~ On Pole(a,Gainl-Lg~ BS(Fg))).Co ft~F~).lnput8(Fltlni,~tcl r.,p~ Z.rolq.Cor~f (R2) G~in(l~ R2)J.lnput~lFltOut).Etc);

:ap2 ~ n Pol-(a.G~in(l~Rp~.Co-~ Rp).lnput~(C~pl).Etc) I~Lin( .In~utA(C~p2).L n(~-lLrn-:).Output~ bpSu~).Etc) utl ~ ero~O.Cocff~ in~G.~).lnputA~:ltln).Etc) JUtSu ~ OnePol~ta.G~in(Fo .Co--f Fg).lnput'(Outl).Etc~: J B ~1 RETUR~(OutSu ):

END Bor-- C~nrENT Rrrd nout~D; ecI~TEGER Pfi^uCEDURE R--dlREAL B-g.Dur: INTEGER Tbl~dr.TolpLr2.pn2sun.pbcsu~) BEGIN RecdINTEGER Tblln.Tblûut.TblL~n.~idsu-.pdpsu-~pdpK~u-.pn2dsuo.T~psun.pt~sun.n~ln~ninln RE~L EndT: EndT~3eg~0ur:

StopUntil(Seg) IclL-n ~ 2tTblPYr2: ~ T~ oo~uD lonot~ ;n ~aupl--:

PdpSu~ ni~Sig~OuitAt(EndT),lnputA(PboSu ),G~inO(l).

Input8(P-25u-~ Gainl(-l) Etc) J Input i~ P-nPdpdSu~ ~ D!~Lin(OuitAt(EndT),inputAtPdpSu ).; n(4-3),Etc): iip- corr-ction If nidSu ~ Sa GE~(Ouit~t(EndT),Fo~Qve ~(O~.Pha~-(98).

A p~ itud-(2~(TDlG-noa.S)/(2t28)).Et~):

ni~S w ~ L~tcbSio(OuitAt(End ) T r-1(TblL~n~.2) Etc)n xl n ~ n i ~S i g (Ou i t~ t (EndT) . r nputA (n i dSu~ i n~ (l ) Input8(PdPS~),Co ~ blE nS2 LSH 8).Etc); ~ lB-OX I n;

J InputB(PqpSu ),G-in1((TblL n~2)'2-1~) Etc)ninln - n~x8i9(oui t~t ( ndT).lnputA(zoro).lnputB(n-~lnl.Gainl(l).Etc):

TDIIn ~ ninSig(Oui Ut( ndt),lnpu U lnidSu-).Ga;nO12-2t(1-TblP~r2)), InputB(ninln) ~inl (l) Etc) I~lOut ~ Lool~(Ouit~tlEnar),lnlputA(~blln).

Sc~ l e (O) . ~cdr --- (Tb l ~ ~ (Tb l Lon) );

~ Su- ~ nulSi~(Oui t~t (EndT~ . lnput~(TblDut) . lnputB(pdpdsu-) ~ inl (l) .Etc):

OI~LinlQuit~t(EndT).Output( ~ ).ln~utA(f ~ ).E-n(~-3).Ete);

RETURN (F~l:

STAN13/006 B4. 86/09/30-5 Atty. ~ocket No.: STAN4983-2~EL Stan Ref: S85-043 APPEN~I~ B l ~J 5 8 ~ O COPYRIGHT 1986 - THE BOARD OF TR~STEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct 13J6 15 ~5 JCU NFF~SAn J~5~ P~G_ I-S END ~--d ;

WnnENT Pip lin~ c not countinq u- or~ int conn-ct ~ti~Sig DI~Lin 3 Ro~Siq Tbl_oolL '~ ~tulSig 1 ~PolO~ ro 1 ndlinctruuent~ C0nnENT Glob~l vari~ble~;

INTFGER PbpSu-~ Pb Suu Ll RcT RE~L 8cg~0u Lg f9 T~ P~F-~Ep-~Rp R~Rn~Ng~E-b 8t;f A~a ~rf eCOLEAN Rt lt Ud STRING Uh~t .s~r~ i, .

EXtERNUL INTEGER NcCVOS INTEGER blAdr P-2Su OEFINLF TblPur2. 1~ Nrc- 2~TblPur2 INtEGER ARRU~ RC~O:~rc~; ~ E~tr~ l~t ~d uscd b4 Dol~rr~ for uc~a DEFINE RT l~o IIF Rt THEN Re~lTi-- ELSE Null!ne~s~g~) OEFINE StdOpen-cS-tSr-te(F-) RTtlao ;h~nn-l~tZ) Opti-i~-(Co-bineeit) ~vStop E~c~ OEFINE UD ile~i Y ~IF ~d ~NO NOr Rt THEN ~ itdDataF;I-(~) ELSE NULLI~ESSAGE)~ OEFINE RTrePcrt-c(lF NOT Rt THEN Report cLSE NULL!nEiS~GE)~ OEFINE û-c Chit~t(8eg~0ur~ o POINTER Pt Rt PROCEDURE C~Env: IF E-b NEC 2 THEN R~na~Env(-B 1 ~C~F(E~b~10Q)~- 1 10~ ~C~F(Stif)):

CDnrENn GetRCt7~1e - Load R~flection-Co-~ici~nt T~DIPR2CEDURE GetRCta~l-(lNTE OER ARR~r RC: INTEG~R N):

3EGIN G~tRCta~ INTEOER i,Ch n,Br~,Eof:

IR RcT.1 THEN 3EGIN FOR i~1 S~EP 1 UNTIL N 00 RC~ Ta~(2~19~ Ep-ilon;

PRINT(-~C t~ol- i~ con~t~nt ,T~,CrL-):

ENO ELSE If RcT.2 THEN BEGIN STRING T~ IF SATfil-,NULL T~EN BEGIN PRlNT~-Longt~ .N,- inout S~T til~ SAt~ INChUL:

ENO ELSE aEGlN PRlNTl-U~in~ pr-~iou- t-~l- SAT~il- . ,SATfil-,CrL-, (S-t NULL to ov-rrid )-,CrLf);

RETURN E~:

OPEN~8~7n~G~tC~ n,-05~-, 17,8, ,8,Br~,Eo-~: IF Eof THEN PRlNT(-op n f~il d-);

LOO~UP(C~n.S~Tfii-,Eof); IF Eof nHEN PRlNT(-~OOnUP t~ d-):

URR~lN(Ch n,RC~0~,~h1):

~,LE~SE (Ch~n~ ~RINT(-Fil- ,S~T~ii-, io-dod .CrLf):

~0 ELSE ~y S~13/006 B5. 86/09,~30-5 Atty.

Doc~et No.: STAN4983-2DEL Stan Ref: S85-043 APPENDIX B COPYRIGHT 1986 - THE BOARD OF ~RUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 1 335~0 ?

Oct 198S lSt~S JC U.NFF~S~.JQ51 P~GE ~-6 EGIN RcT~ FOR i~ SrEP 1 UNTIL ~ OO RCtil ~ (2-19~ En~Yl(i~ 8~(N-lJ.Rtl nux S PRlNt(-R~ t~ol- -t to curr nt Rt tunction.-.C L-):

E~O:

ND G tRCt~ol- ;

CornENT PutRCt~ol- - G-n-r-t- P-~l-ction-Coe~tici nt T~bl-s PROOEDURE PutRCt blBEGI~ PutRCt~ole NTE OER i.Ch-n,ar~.Eo-:

TRING ^un~-e:

~tRCt~ole~RC.Nrcl:

~INT~-Dutput S~T fil~ . ) On~n- ~ INCHUL:

OPEN(Ch~n~GetChan.-DS~ .2.5.~r~.Eof): IF Eo- W PRINT~ open f~il-d-):

ENTER~ChJn.On-oe.Eof): If Eo- W PRlNt( ent r ~ d-):

URRYOUt(Ch~n.RCt0~,Nrc~ RELEASE(Ch~n) PRlNt(-Fil~ ,u^na-c,- 4r;tten.-,CrLf) E~O Putf~:t~l~-:

COnnENT Ot--t - Obla~-line te~t PR~WlE Ot--t:

BEGIN Ote~tSt~rtS~-(StdOpen,Fi'-(-Ot--t.S--~ Dfil-(-Dt-~t.~,r~-)) PRlNT(CrLt):

8ind(sa-oo~sctpa~(8eg~srate));

Pb~Su- ~ OACnodSu-t l: PbpSu- ~ OUCnodSu t11:

OlyLin(O.Len(LI-3), npu U (PD4Su ).Output(Pb Su-~.Etc);

OI~LinlO.L n(LI-~l, nput~(Pb-Su J,Output(PbpSuel,Etc) IF It THEN lepult (~eglEp-.O~r.T~.PbpSuu) asE Noi~e~Beg~Ep~.Beg~2~Ll~Sr~t-,T~,PDpSu-) IF ~d THEN ~riteSig O.lnputA(PbpSu-).Etc) StopSa-(O.RTreport):

END Ote~t-:

COnnENT 8te~t - Bor- te~t;

P~OCEDUR Bte-t;

8EG1N Bte~tSt~rtS~ (StdOp n.Fil-(-Bt-~t.S~ -).UOfil-(-8t-~t. nd )~: PRINT(CrLt);

Bind~S~ox.S-tP-~(B-g~Sr~t-)) Pc-6v - ~AC~odSu~l; PboSu- D~C~odSu tll IF Ud THEN Ur;t~Sig(O.lnputA(Rx~ ).Etc) Ol~Lin(o.Len(6-3).lnput~(pbpsu ~.Output(Pb Su ).Etc);

aor-(B-g.Dur.Lg.Fg.Rp.Rz.LI.P~p~4-,Pb Sua1;

lF ~t THEN l-pul--(8eg~Ep-.3ur.~-.PbpSu~ QSE Noi~(Beg~Ep~.Beg~2~LI/S~t~.~a.PbpSu~);StopS~ (a~RTr-port);

END Bt~t-:

COnnENT Rt--t - R--d t--t PROCEDURE Rt~t:

aEClN Rt~t INTEOER i 3utSu~.NoiSu~. n i ~su. P~25u~ ~-9su. P t su.St~rtS~ (StdO4-n,Fil-(-Rt--t.S~ ).UDfil-~-Ri-~t.S~d-).HogSa ): PRINTlCrLt) TDlAdr~G~tF(8-g~Dur.D-Addr_p~.Nr .-RCt~DI--):

IF R- THEN 8ECIN ~tRCt~DI-(R~,Nrc):

,~l~rr~(Rc.TDlAdr.Nrc):

END LSE PRINT( TD lAdr-.c~o-(P~v otr(Tol~dr)l.CrLt):

Gind'S~ ~ox.s-tp~ Be9*sr~t-l) PDPSU- - QAClod_u~ Sl'AN13/006 B6. 86/09/30-5 Atty.

Docket No.: STAN4983-2DELStan Ref: S85-043 APPENDIX B f 3 7 5 ~ 4 o COPYRIGHT 1986 - THE 30A~D OF TRUSTEES OF THE LELAN~ STANFORD JUNIOR UNIVE~SITY Oct 1986 lS:~S JCLA.NFF~SAn,JOSl P~GE ~~' ûut~u- ~ u^Ao~odSu~ Pt- u ~ S- GENlO.A-pEn~(SclEn~P~.PJ)),Fr-Qu-~c~(0),P~- ~9 ~,G~hift~g-_o--~,Etc~ Noi~u- ~ ~n Pol-(5.GJin(Nc-(l Rn)).Co~tf(Rn),lnputB(NoiS;g(0,-tc)),Etc~ u- ~ ni~Sigl~.lnputA~P~J6J ~,G~in~l),ln~utB(NoiSu 1,G in,~l),Etc) ~-g u- ~ Sa GE~O.~-DIituob~An~),Fr-~u-nc~(Anf),G-~ift(9-_o~ ,Etc~;

pO2cu ~ S~nOO~O,~od-(A-),C~inl (2-An~), nputA (n; ~su ), InputB(AagSun),Etc~:

P~ u- ~ ~ dlB 9,D~r,TblAdr.TolPur2,P~2Cuo,PboSu ) Out u- ~ aor-lB-g.Dur.Lg.Fg,Rp,R~,Ll,Pbp 4-,Pb Suu)~ IF Ud THE~ Urit-sig(o~ln4utA(pb u-~,Etc~:

lF TJ>0 THEN lF It THEN lupul~ g~ED~,~ur,TJ,PbpSuo) EL Con-tant B-g+Ep-,Dur,T~,~ix5u ):

St~pS~ (0,RTrc~ort) END ate~s-;

C~nnENT ~e~Te~t - Te~t playing ro- t~ ~c~bo~rd P~OCEDURE ~-~T~-t:

EEGI~ ~e~T-~tINTEGER i,ûut5u-.NoiSu-.ni~Su ,P~25ua,AogSuo,PfaSu ;

StartSJ-(stdoprn.Fi~ rr~t~sa-~)~uDfil-(~ T--t.snd~)~Hogsa~); PRlNT(CrLf);T~lAdr~GetF(Beg~Our.D Addr_pe,Nrc, RCtaole );

IF R- THEN 8EGlN ctRCt~bl~(RC,Nrc);

)e l ;~rr J~ Tb l Adr ~ Nr c);

ENO LSE PRlNT(~TblAdr~ o~(PeNuue-r(TblAdr)),CrLf);

Bin (Sa-bnx,SetPa~Ceg~Sr~te));

Pb~u . ~4onodSuo~0I;

Out~u ~ ACnodSuo~ Pf~ u ~ - oEN(L,A-pEn~SelEnv(Pf P~)),Fr-qw ncu(0),Pha~a(90 ,Gshift(g~_o~f~,Ete);

Noi'u ~ n Polola~G~in(Nga(l-Rn))~co-ff(Rn)~lnputB(Noisig(a~ te)),Ete);

nix"u . n;xSig(C~lnput~(PfaSu-) G~in0(1)~1nputB(NoiSu ),G~;n'(1)~Etc);

Au; ur ~ S~-GEN~C,~rpl;tud-(An~),Fr-euenc~(Anf),G-hitt(g-_o~f~,Ete):

P~2~u- ~ S~-nOG(a~nod- O-),G~inl(2-Ana)~ npu~(nixSu-),lnpu~B(~agSu-),Etcl;

Pb- u ~ R--d(8eg,0ur TbiA~r,tblP~r2,P~2ru-,PbpSu-) ûut~uu ~ Bor~(B-g,Our,Lg,Fg,Rp,R~,Ll,Pbp u-,Pb~Su-);

ff Ud THEN Lritesig(G~lnputA(pb Suu)~Etc);

IF T~>a rHEN IF It tHEN Irpul~-(B-g~Ep-~our~T~pbpsu-) Q Con~t nt(8-g~Ep~,Dur,Ta,nixSur);

PRlNT( Ent--ing pl~ loop CrLf) U~ILE rRUE 00 BEGIN StopSa-(û. RTraport) EhO ~-~To~t ;

C3rnENt ~ho 5~ PROCEOURE Uho; ConrENt Print glo~al~ EGIN 'U~o REDEFINE Se-iCrLf.e( 6 1~a~ 12~;

PRlNt(~ab Rt~ (IF Rt nHEN TRUE asE F~LSE ),Se~iCrLf);

IF Rt THEN Ud-FALSE:

PRINT(~ , Ud~ (IF ~d t~EN rRUE ELSE F~LSE ),S-~iCrL~);

PRlNT(~b~-pf~a~En~ PrtEnv(Pf)~---)-~S~-iCrL~) PRlNT(T b,-Rf~l~i~Env(---,PrtEnv(Rf~,---)-,Se~iCrLf):

IF ReT.2 tHEN PRlNT(Tao SATfil-~ '',SAttil-,'' ,S--iCrL~) PR N~(CrL~);

PR N~(tao ReT~' RcT Se-iCrLf);

S PR N~(Tao 8 9- B~o,SrriCrLf);

PR NT(T O4r~ Ohr S~iCrLt~;

PR NT(taD Ul~ Ll, ; COnnENT Pitch ~ '~CYF(F-/LI~ ;' CrL~);

PR NT(t 'P~_ ,P~, iCrL~ PR-NT(T,'~-- t~, ~ iCrLf);

PR Nt(taD Lg- Lg ~--iCrLf);

PRlN~lTaD Fg- fg 'e-iCrLf) STAN13i006 B7. 86/09/30-5 5~ . C'r!~N~qS21_0r~FT. C~an ~ s~s-043 APPENDIX B 1 3 3 5 8 4 0 COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY Oct 19~6 15:-5 JCLA.NFF~SAn.J~SI P~LE 1-~ PR NT(T~o,-Rp~-.Rp,~e-iCrLf)~ PR NtlT~o,'R2--,R2,'~-iCrL-~;

PR~Nt(TD~ N~ --iCrLf1 PR NtlT~o~ Rn~-,Rn,''--iCrL~);

PR NTlT~-Tr~-~Tr~ -iCrLf);

PR NTlT~o.-~ iCrL-);

PR'NT(t~D,-~nt.-,A1-.'-n;CrL~);

PR Nt(t~b.-E-o~-.E-o.~ -iCtL-~;

PR~Nt(T~o.-St;f--,Sti-.S- iCrLf);

PR NT(t~-F~ cys(F~)~s- iCrLt) IF T~>4 tHEN 9EGIN PRlNtlt~o.Tao.-lt~-.(lF It T~EN 'TRUE' E~SE 'FALSE-).S--iCrLt) PRlNTlT~c.t~ p~.-.Ep~.Se-iCrLt) ~D;

END Ho-;

PRCCEDURE S~v-{STRlNG Fna--l-JC U -)) CDnnENT Sav- gloc~ 8EGIN 'S~r~ IF Fn~- ~NULL rHE~ 8EGIN Print('Output JET til-:'); Fn~ lNCHUL ENO;

IF Fn~ e.NULL tHEN RETURN:

SETPRI~t(Fn- -.'8'): Uho: SEtPRlNT(NULL,'T-) END S~v--:

COrnENT S-t up d~t~ult~ ~nd tr~ ;t:

PROCEDURE E(STRING F(NULL)): Ev~lF(-DS~-.(lF F THEN F ELSE JCL~.JET'~): E:

REDEFIHE r.-Rte~t'; ~ I h~te to t~pe;

~tflNE dr - dprvenv~rt)-;

fftlt~lNE d~ . dp~env(pt) PRlNT~CrLt.- CL~: .

C0rPlLER!BANNER LENGTHlSC~NC(COnPlLER'8ANNER,'11~--,--.--in2-))~11 FOR 17~,CrLt):

x I~U~. T ~0,3) NoCYQS . TRUE; CDltENT 1 Evaluator doe~n't r-cogniz- t~ n't print;T~ 8;

It . fALsE;

Ep~ O 01:

Tr ~ 8 Rct.3;

~;

~11 f ~8;

U~at .

Uho.~ at.': -~CrLf~-Openfile(na-c).Clo~efile.Bt-~t.Rte~t-:

~HILE nRUE 00 S~lLError(2,-Uho.~hat.Uhero. or :'-,--):

S~v~:

f~O J- ~S STAN13/006 B8. 86/09/30-5 a R t _ ? r~ ~ T C t ~ ~ C R C~ 1 37`5~40 APPENDIX B COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY ~0ctl986 lS:41 ~5.~il 2 21 PAGE ~5-1 ~L~ O-tor-in- i~ PiP- corr-ction- ~r- needed ~outo g-t ProD-r clipping?

~oi~ a~ n-~d lpol- loulp~ or ~o S~ould ~ound noro~l Fi~ u^C on~et ~lap in JCLA Tr~ oigger t~le Fl~r- D-l Su output correctl~ or tono hole~ Future tuo ~orec ~28-n,--86 1839 Jo~i CliC and del~u-change control Re~on tor ~ign~l h<~t u ~c-a t rir~ht ~t ~ ~ignal e~tre-e all ot outh pre~ur~ g-t~ gated in ~nd ~ince outh pre~ur- ;~ a~aep thl~ ~ield~ l~rge~t po-~ibl- r-tl-ction ~ign l P-rh~p~ thing i- uhether ~lope xce-d~ -1 or ~o e ~uch ~Z2-l~r-86 0819 J06 JCLA C~nrENT T1 ~akc c!-rin-t do~OI~ toot P ~na~Env( ~ 8 25 1 50 8 75 1 la6 8 );

Rt~n~kEnv(~O 1 25 1 65 0 a8 18B a2 ) L1~91 Beg 0 Our~ 5 80: P-~ l B8 ta~ 8; Lg- 998; Fg_ 78a Rp~ 0R~ 1 80; Ng~ 0 Rn~ 9 Tr-O F~ ~88aQ CIrnENT T2 T1 ~cept reduc- R t right ~nd d~-p-n hor Pt_~a~Env( 0 0 25 1 S8 0 75 1 108 0 Rt~na~Env( O 1 2a 1 18a 8 ) Ll 91 aeg- o Dur 5 0 P~ 1 0 T~_ 0 Lg~ 95 Fg_ 786 Rp 0 R2~1 0 Ngr O Rn 0: Tr~4 F~ oOnnENT ~utSu- ~b ll output) U~Y too aint ~l~o it ~ not uch ~rig~t r ore cignal i~ ~trong ~ut too ~a~u 'ignal i~ v-r~ ~-n-itive to ~reaA~oint loc~ ~oving l-tt or right uor~en~ rea~ing right-o~t rc in Rt ~Ae~ th- not- louder' Ue can :~ ~n~te ~ d-crea~ing Lg ~- u- have don- here No;~e added to outh prc~ure didn't ch~ng an~thing tulndaeental (Ng~Q) Oddl~ th- noic- I-v-l g t~ odul~t-d ~o ehou h~ th- not- ~ plitudb Br;ghtne~s: S t Fg tro~ 7 to Fg- 7 i~ not Dright ~nough F p- 1 giv-~ highpa~ in looo L--- th~n th;~ doo~ not ~ound CornENT T3 (uou1 T2 xc-pt 1-~ loupa-- ~ott-r ~or- Po rci--;

Rt~TRUE Uo~F~LSE;

Pt~na~Env( O 0 25 1 53 0 75 1 1~e 8') Rt~nakEnv~ 8 1 25 1 1e4 ) L1~91 B~gr Lur~ S O P-- 1 8; T-^ J; Lg_ 970; Fg_ SBe Rp- O;

R2~1 0; Ng- 85; Rn O; Tr_O; F~ U 0~0;

STAN13/006 B9. 86/09/30-~ ~ t 1- ~ ~ n ~ t Y -~ ~ C 'T` ~ N ~l q R ~ - ~ n F` r . ~ r- CRS-04 1 335~0 APPENDIX B COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY ~ Oct 19J6 15 ~1 JOS nSCI 2 2I P~GE ~S-2 COr~ENT In t~i~ c~ inglu t~e fir~t not- ~I-o~t ov-rblo~ to Ji~l~ t~ 3rd h~r onic la ~itth upi Th- tuo not-- ar- id ntic~l but ~or ~t th noi~ i~ doin9 u-t th- -cond not- ha- ~ olid und~- nt~l ~nd ound~ co pl-t~lu ~ift~r~nt ~rt ti b- 8/29/~6 1it ~ ~ -n ~ uhil-!) Lrot~ GENSAT SAl to tru ~o-- oth r RC tunctionFir-t r-pe-t-d th- ~unction in ~ou j-t nd got id ntic~l re-ult- N-~t tri-d oro r 2 Found th t t~r-~old blouing pr-~-ur- iTSP) dropp-d to ~Dout P~ 8 6 ~nd ~t P--2 8 th- not- ~ur~tion ~ out th ~ b-for~ ~x~--p I Q1-n r-86 a151 JOS CornENT n-~- cl rinet doubl- toot Rt-TRLE ~d_F~L;

Pf~naLEnv( O 8ZS 1 raO 8 75 1 188 O ) Rf~na~Envl O 125 1 65 0 a~ lB8 t2 ) Ll~lB8 ~-9~ 8 Our~ s.æ P~ I B8 Ta. 8 Lg~ 99 Fc~ 788 Rp_ 8 R2 1 oa Tr-4 F-_~8a~t8 ~inning i-pul~- t-~t of re~d ~nd boro RT ~ F~L UD ~ TRUE 8-9 ^ ~ Our ~ .1:

P F ~ na~En~l O 8 1 0 2 1 1B8 1 ) Rcf ~ na~En~( 8 1 25 1 65 U 1~a 82 ) F- 3B88B:

LoopL n ~ 18 P-~ p - 8:

T~-tA p ~ 81 I-pT--t ~ TF~E Ep- ~ 0 01 Tr x- ~ 0:

LoopG~in ~ 1 FoG~in ~ a Uinning St p tn~t RT . FALSE UD ^ TRUE 49 ~ 0;

"Jr ^ . 1:

f ~ n~En~l O O 1 0 2 1 1~0 1 ):

~cf ~ n kEnYI O 1 25 1 65 U l~B a2 F~ ~ 3DeaO LoopL-n ^ 18 P~ r~t~ l pT--t ~ F~LSE Ep- 81 Tr c- ~ LoopG~in ~ 1 FbG-in 9t-~ to~t u~ing ~oo n~ S~AN13/006 B10. 86/09/30-5 .~ttv.

Docket ~o.: STAN4983-2DEL Stan Ref: S85-043 APPENDIX B 1 3 ~ 5 8 ~ O COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct lg~6 15~ 2. 2l P~GE ~5-3 RT ~ f ALSE . T~;

~- 0:

P F ~ n~Env ( ' 8 0 i 0 2 1 1~ 1- ~:

R~ ~ Env ~ 0 1 25 1 65 ~ 1 851 ~2 );

F~ ~ 388~ ~wpL-n ~ 10:

P~ p ~ T--tA p ~ a;

I pl--t ~ F~ Ep- 8 ~1 Tr ~ O:

~oop~;a i n ~ l;

F~Cain ~ ~ Fir-t or~ing toot t-rt, 3~1~86 11ain pro~ i- Dig Oc top F ~ ~ 3t~0 Rl ~ TRUE ~0 ~ FALSEPcF ~ ll~Envl-0 8 20 1 80 1 188 8-):

RcF ~ Env ( O 1 25 1 65 U 188 82- ) 8eg ~ O D~ - 1:

LoopL n ~ 35 P,,~p ~ 1:

LoopG~in ~ 99 F~G~in ~ 7;

ST~13/006 Bll. 86/09/30-5 ~ . C ~ ~ ~ A ~ Q ~ n ~ T C ~- ~ n ~ ~ C C~ O ~ APPENDIX B 1 3 ~ 5 8` 4 0 COPYRIGHT 1986 - THE BOARD OF $RUSTEES OF THE LELAND STANFORD JUNIOR UNIVERS~TY 7 ~t1~ 21:~ ~L.IET(~.~5l P~El-l Filn_ E~t PPN Si2~ ~ritt~n Ti-o Pro Urit r R~-r~rc---S Ou-pcd Ot~SEl JET SArJOS l'S :'-Scp-~6 a927 OBB lJOS JCLA 7-Oct-hO ~ P~7 JCL~ JET SAlJOS Z~6 .. -l~r_06 BaS5 o~a lJOS E 7-Oct- ~ a6 P.7 ICrU 6 JET SArJOS ~' ~q-Au~-~6 23~9 ~8 lJOS JETS~n ~7-Oct-_ lS P~b~ e*lGHT JET S~nJOS '~ pr-J6 1223 R88 TX- ~N JCLA 7-Oct-A 01 P7r TEST JET S41JO' 2~ 2 -n~r ~6 B ~ ~ l QS E 7 4ct~ 7'1 BASSAX .~T SAnJO~ ~ 7q-Aug S6 2316 eo lJOS JCLA ~-Ckt- ~ 7 P2 ~ SE2 T ~AlJOr ~- -S-p-56 ~931 SS lJOS JCLA , '-Cct_~ 4 P7 ~. >

SE~ _ T ~ '; --S-p-J6 ~S W l~S JCLA7~ct-~s ~ P~ 7 TOOT2 ~-T ~WnJOr 12~ - -n~r-~6 ~a~2 e~8 _~S E ~ -~ct- ~ 1 P- ~ UOU -T WnJO~ 17 ~7-n~r-56 '2 B80 _~S E ? ~ct-~6 BS P~~~>

NCLOSS JET ~lJOC ~ -Aug 6 ~':S 88B l_JS JETsAl1 7-Oct-86 22 P- ;>

strPc JET SA~JO~ '2 5 -Aug-86 P74 BaO _OS JETS~n 7-oct-a~ ~2 P2 ~ SE~ JET ~WnJOr 1 2-S-p-t6 ~ 7 B08 lJ~S JCLA7-Ckt-5~ 4 P2, >

SE5 JET ~UnJo~ '1 12-5 P-56 J~ a 880 lJ06 ~ A 7 4ct-J~ ~4 P2~7 Tot~l- 3 3 SEl JET SA~105 115 12-Sep-56 B~27 B08 lJOS JCLA B7-akt-56 04 P287 Rt.nR~_ Pf~ 'nv(' .9888880 .B888808 12.5808000 1.B888800 37.50Qa280 1.0098888 59.80888a9 .B82e800 62.5~98828 1. 88B889 87.500QBEO l . B9oa888 180.8QBQRBO .8383Ba8' );

Rt~na~',nv~- . 88808a8 1.0880888 25. 88B80BO 1. B8908~8 109. B088809 .8808988 ' );

SATtile--o4.~t';

RcT-2:

Dur~ S.a892'`8 Ll~91 CnnnENT Pitch ~ ~39.s6a448a;

p~, .~ :i~ .' ;

r., .

Lp . 7 Fg. .'~~~~ Rp~ '~ '' ~ ;

Ng. 1~ c-2 ;

Rn. .8 "~h~ ;

Tr 2;

Arb~ .0B989B8 ~ so0sa Fs_4Beaa:

JCLA JET S~nJOS 256 22-nar-b6 0056 0B8 lJQS E 07-Oct-56 a5 P273 - COnrENT n~ ~ clarin-t dr~uDI- t30t, r-duc- Rt at right and da p-n ~or-;

REDEF NE r.-Rtc~tF'NE dr . 'dpyan~(r~ REL_F'NE da . 'dp~en~( Rt~lRUE;

~AL5E R~a~Envt-8 8 25 1 90 8 75 1 198 O'):

R~.na~Env(-0 1 25 1 180 8' ~:

_1~91: ConrENT Pitc~ appro~ ~4~:

ep .8;

v~ 5.88;

'~ 1.88T~ . B:

Lg~ Fp .288;

R~ .8;

R2~ 1.80;

Rn~ 8 Tr~ :

F~_48888:

IC~W6 ET S~UQS 91 29-~9 J6 2349 880 lJDS ETSAn 8~et~8 18 P286COtENT ûutSu- (~l l outputl U,~'~ too ~int. ~1 o, i t' - not uc~ t r.

ecr- oign~ tronC but too b--s~.

ST~N.13~006 B12. 86~09/30-5 l~tl-v nr~k ~ t ~ T AN 4 98 ~--~n EI. St~n R~: S85-043 APPENDI~ B 1 3J58~0 COPYRIGHT 19 8 6 - THE ~OARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oet 1986 21 39 4LL JET~SAn JOSl PAGE 1-2 Signal ~ v-r~ ~-n~itiv- to Dr-~point loe noving I- t or right ~or~en~Oecre~ ng r ght-oct e In Rf ~ th- note Ioud-r~ U- c n ~ n~te Du deer~ing Lg ~ ~ bave don h-re Noi~- dd-d to outh Dre~ ur- didn't ch~ng- ~nuthing und~-ental (Ng>~ Oddl~ the noi-e level g t~ odut~ted o-ehou D~ th- note acplitude 3rig~tne~ S-t Fg fro- 7 to Fg. 7 i~ not bright enou~h F~_- 1 give~ highp~ in loop Le~- than thi- do-~ not ~ound Rt~TRUE Ud~F~L~E Pf~lal~Env(' 0 ~ Bæ 12.508 l.B88 ~7.508 1.5B0 52.808 .~8 62.588 1.082 87.5Q8 1.;~2 1 0 . ~0' ) Rt~la~Env~' 0~ S0 25.888 1.099 lB0.089 .089-):

_1~91 COnrENT Pitch 439 560 eg~ 081 'v ~ 'i ~ '~ . ~ :

T~ .~ :

~p . 7 F p 1 ~ R~ . 8~ ;

R2~ 1 ~ Np 1 ~--2:

Rn ~0 Tr~2E-b~ 0ae S t i t . . 08~ :

F~_4ZBB0;

BRlGHT JET S ~ i 78 03-~pr ~;1223 8~0 Tl~T~NJCLA 07~ct-86 01 P27~>

Rt~TFUE Ud_FALSE;

Pf~ Env(' .080 .000 25.088 1.888 58.888 .~O0 75.088 1.888 1B0.080 .0a8');

Rt~n~Env(' .880 1.888 25.8QQ 1.088 188.888 .888'1 I~9l; COrnENT Pitc~ . 43~.568;

ag- .8~8 ~r~ 5.88 '~ 1.0~8 T~ .808 Lp .995 F p .3ao RD~ .808 R2~ .888 N9~ .528~-2 ;

Rn~ .808 Tr~8;

F~-4oaZ8;

TEST JET SAnJOS 256 21-n~ -86 B~38 B88 lJQS E a7-Oct-JS 01 n73, ConrENT I pui~e-in-lo~ci-~--loop te~t F~ ~ 38OEOa;

RT ~ nRUE:

UD ~ F~L :

Pf - n~Env('O O 20 1 U 1 180 8'):

RF ~ n~En~'O 1 25 1 65 . U 180 . U ):

D~r ~ .1:

~L - 35:

P~ . 0:

TA ~ l.O LG ~ 1:

FC ~ ~:

Rp_R2~0:

BASS~X JET SAnJQS ~5 29-Aug-a6 2316 890 lJQS JCLA 87-Oct-S6 87 P2S6>

STANl 3 /006 Bl 3 . 86 /09 / 30 ~5 . . . n ~ _ b ~ ~ T ~ ~ Q '~ ~ r ~ ~ c . .~ APPENDIX B 1 3 ~ 5 ~ ~ O COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 ~t1~ 21:39 ~L.~Tl~,~Xl P~ 1-3 R t~TR Pf~n~I' .~ .~ 12.~ l.o~ ~7.~ 50.~ .o~ ~.~0 1.~ ~7.

O. ~ .

R f ~l~En~ ( ' . ~1 1 . 3B11 25 . ~08 1 . ~8P 1 8S. ~ .

1~150: orn~T Pi t~ - 2~.~7:

4r ~ .. . SSO ;

T~ . ~ ~9- 7~ ;

Fg .~111 Rp~ R2~ 1. 8S -2 Rn_ . 88P Tr. 2F .~41180~1;

2 JET S~S gO 12-SCP-~6 8931 ~8~1 lJOS JCLA ~7-Oct~S6 ~ P287>

Rt- TRIJE:

Pf_n~nv( .~ .~æ 12.~B 1.~ 37.~ ~ l. o~ so. ~ 62.~ 1. o~ ~7.~ 1.~ 11 0.0~0 .08~-):

Rf_nb~Env(- .88a 1.~2Q 25.8aa 1.8B0 1~8.8a8 .a28-):

SAT~ 4.

RcT~2:

Dur~ 5.2~ :

Ll-91 COnnENT Pitch 439.56S:

p~ t~ . 2e Lg~ .`7S Fg~ .'88 Rp~ . 8a Ng~ .1 æe-2 ;

Rn~ .8B0 Tr~2:

~n-. s.

F--4a8aO:

- ` 3 JET BUnJOS 90 12-S-p-86 ag35 ~80 1JOS JC U 87-Oct-J6 ~ P287>

Rt~TRI F Ud~F~L :

Pf~n~nv(' .o~a .0~8 12.5B8 1.0eO 37.588 1.888 sO.0e8 .za8 62.5~8 1.88S ~7.58a 1.0 t .800 .0a8-):

Rt~n~Envl- .oaa 1.0aB 25.B80 1.888 10~.80B .88S-):

S~T~ -o4.~tRcT~2:

Dur~ 5.~ Ll~91: ConnENT Pitc~ ~ 439.s6e:

P~_ .8~ :

T~ e8 Lg~ .97- ;

Fg~ .100 Rp~ .800 Ncr .180<-2:

Rn~ . 80 Tr~2:

Ar~ 1.~ ;

~t~ 0 F-_;

TOOT2 ~ET SAtLlDS 12~ 21~6 81132 880 lJOB E ~-Oct-J6 n P256 C~T ~ ~ D~-iC toot, thi- tin U-il~ OC D~ in loopS STAN13/006 B14. 86t09/30-5 ~tty.

Docket No.: STAN4983-2DEL Stan Ref: S85-043 1 335840 APPENDIX B COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 3ct 1986 21 39 ~LL ETlSAn JOS~ PAGE 1-~ Rt-nRUE Ud-F~LSE Pf~ En~ 098 -08 28 088 1 Ba8 U 880 1 Ba8 188 ~08 800 ) Rf~nb~n~( 880 1 088 25 060 l O~O 65 88 U8 188 808 a28 )~ l~18J COnnENt Pi tch - ~88 808:

~9~ 888:

ur~ 1 88 '~ 1 08:

t~ 88~ 0:

fcr 700 Rp~ 008 Rz~ 1 8~ r,~:

F~-~0aOO UOU JET SArJOS 12~ 22-n~r-86 0122 000 lJOS E 07-Oct-~6 85 P273>

COrnENT na~- cl-rin-t dcuOI- toot rcduc- R t ri~t nd da-pen ~orc Rt~TRUE:

Pf~n~En~(- O 8 25 1 50 o 7ra 1 180 8 ) Rf~n~En~( 0 1 25 1 100 0');

l~9n COnnENt Pi tch ~ ~39. 560 0:

ur~ 5 '~ 1 . ~:

T~ ~ Lg- 978;

fcr S~;

Rp- 8 R2~ l O:

N9~ .oe;

Rn~ O:

tr~O F- ~8880 hOLCSS JEt SAnJO5 92 38-Aug-66 8815 B80 1JOS JETSAn 07-Oct-~6 52 P2~6 Rt~TRUE:

Ua-f~LSE:

Pf~n~nv(- .880 .800 12.5~8 1.880 37.580 1.088 50.800 .088 62.sa0 1.888 a7.s08 l.aO 10 -000 .880-) Rf~ Env( .880 1.8B8 25.808 1.8B0 188.088 .808-~:

88 COnnENT Piteh . 188.088 ~9~ .~8B ~r~ 1 . 0 ~ .5'' T~ .88 . 0v Fg~ .80~' ;

Rp- .88~ :

R2~ 1.8~ :

Nc~ 8~-2 :

Rn- .880 Tr~2:

E-t~ .000 Sti~ .808 F-~8808:

0InPC ~Et SAnJOS 92 38-Auq-~6 8QnK 8~8 lJOS ~ETSAn 07-Oct-J6 ~2 P2~6 Rt~tRUE:

Ud-F~LSE;

P-~rJ~En~(- .8e8 .800 12.588 1.8BO 37.5JO 1.0e~ 58.~BO .850 62.5JO l.BOO S7.5JO l.B 11 0 .0~8-):

R~-n~nv(- .80 l.-D~ 25.080 l.~e~ 180.~ea .~QO-);

-64 ST~13/006 B15. 86/09/30-5 1 3 ~3~0 APPENDIX B COPYRIGHT 1986 ~ THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 70ctl9~ 21~39 ~l.~T~,~l P~l-S 1.~; ~n~TPitc~. ~n.~:

ur~2.~ '~ .~ :

T~ .~ ~p 1.00 F p .111~0 :

R~.~ ;

R2~ Np .1#~-2:

R~ .E~ :

r~2;

~~ .080 ;

ti ~.. .

~4~88~;

Rt~T~;

Ud~S~ Pf~n~ 12.~ 1.~ 3~.~ 1.~ ~.~ .~ ~.~ l.E~ ~7.~ I.a~ ~E .#~ .E~-~;

R~ n~l- .~ 1.~ 25.~ 1.~ 1~.~ .~-):

~T~ t~ SE4 ~TS~U~S 9112-S-p-~ ~7 ~ 074ct~ ~ P287>

RcT~2 Dur~ ~.0~ ;

Li~lSe onn~T Pi tch - 266.667;

P~ .~ ;

T~ ._O Lg~ Fg. . ~ Rp- . ~ :

Ng~ . ll!llh-2:

Rn .

El~ Tr~2:

. '~--1:

~f~ 5.

F~88 Rt~TRL:

U~F~LSE:

Pf ~n~ ( - . ~ . EIBP 12 . 5~ 1.1~8il 37 . 5~ 1. 080 5~. 81l0 . ~!18 62 . 508 l . ~SB 87 . 5~8 1. ~ 1 E .~ .8~-):

R f ~ll~Env E ' . ~10 1. ~0 25 . 388 1. 88ll l Elll .1180 . EI~ SAtfi l~ t-:

5 ~T S~IJOS 91 12-Sep~6 OE~38 ~ lJI~S ~ E17-Oct~6 ~ P2a7 RcT~2 Dur~ ~. ~8 ;

L1~3~; Wl~NT Pi tcJl ~ 133.333;

p~ . s50 t~ .`80 Lg~ . 7` Fg~ Rp~ . ~ :

Ng~ .18 e-2;

Rn~ . ~8EI Tr~2;

. S~e- l;

~nf- S.

F~;

STAN13/006 B16. 86/09/30-5 APPENDT~ C 1 ~ 7 ~ OF THE LELAND STANFORD JUNIOR UNIVERSITY ~ ~ct 19~6 21-2S vS.~ Lt~.~S~ P~ C~rrENT Violin Si ulJtion o~tu re ~od~fic~tion ~i~to~ Ori9in~ uac V.5~1 ~5~1,JQS~, C-. OCt. 1~2.

Tr~n ~t b-C~ S.S~IlSlO,JOSl, ~ro~ 2 to Ap~il S3.

No uo~t~nti~l ch~ng-- ~ r- inet~ d over t~ n~t co~pl- ot ~-~r~ 12/11/85 - Ch-ng-d Tr-c- u-~go ln-t~ a oul~ tring r-~toring ~orc Added v-locit~ ~nd bou--tring o~rc- output ~ile ~L~S:

~llpa-~ r-~et or v;br~to i~ not p-rt-ct Yo~ can he~r little glitche~ onc- per period luhen d-l~y Iin- incr-a~-~?) Need ~ caretul r-vieu o t~i- Perhaps r-etolr- old vee~ion to ~ee ;t it ~a wened ~ay ~c~ u~en l t~ought not! (12/11/85) The ~ou friction eurve u--d in HJperBo~ i~ not ~uf~icientl~ reali~tic ~ pur- discontinuity ~hould o- replac-d inite ~lope Th cou-~tring olver ~oe~ not corr-ctly i~pl-eent ~tere~i~ Dehavior Need a ~tic~--lip ~tere~i~ e or~ r~it Currentl~ th- ~-all-rt v-locit~ pe~turbation iJ ~elected uhich c~n b urong in the ~tuc~ e~-- It ~a- o-en o~-erved th~t ur~n neg~tive v~locit~ pul-e return- to oou roe nut. u- e-n to b ju ping to lip~ing uithout getting over th- friction curv- pea~ BGIN VS RfoUlRE (l o OELI~ITERS;

u^EFINE t I COnnENT 1 thru - I STEP 1 UN~IL 1 CnLf - t( 15)~('12)1 Ta~ . 1 116 1 ~It . 1 175~ 1 Cr 1( 15)~ 1 Sa~ .

Il EXTERNUL INTEOE R !S~IP';

INTERNUL INTEGER Trace ûuiet RE5U RE J05L18 REOC 18 JQSI SOUR~E'flLE REOU RE 'RECW REOC 19 ~ Sl~lflCE!FILE;

REOLI RE 'tlYlO P~O~LI JOSi SûUROE!FlL~;

FE~U RE FLTIO RE~L B JO-~' SaRCE'flLE;

REOU RE Ol SPI~ REL LlB JtJS~ SWROE ' ~ I LE E)(TER~L PROOE~E Trplni(lNTEOER COOE); ~ JA11LIB flo~ting-point tra~ O~INE Traccl. (tr-c- U~ Tracc2. (Trac- L~ 2) Trac-3. (Trac- L~ 4) Trac~.-(rrace L~O ~i-.

TraccS.' (Tracc LAN~ 16)' Tracc6. ITrace LArO 32) Fi I ter and Oel~-Line routine~;

Sl~ lNTEGER PR~XEDURE ;nd-x(lNTEGER Ptr Len) RETUlNllF Ptr>Len T~N Ptr-Len ELSE IF Ptr LEO 11 THEN Ptr~en QSE Ptr) REAL PROC~IRE OI~LinlRE~L ~Y O REFERE~eE INTEGER Ptr INTELER L-n; R~L InSigl91);

CtlffNT Place~ InSiig into t~cla~ I ine ot lengt~ Le~n ~nd rctwns cwrent output;BEGIN '~ JL in' STAN13~00 Cl. 86/10/17-1 Att:y.

Docket No.: STAN4983-21)EL Stan Ref: S83-043 APPENDIX C ~ 3 ~ 5 ~ ~ O COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND S~ANFORD JUNIOR UNIVERSITY Oct 190S 21:2~ Vs.NFF[LlB. QSl PAGE 1-2 REAL Output:

IF Ptr LEO S r~EN BECIN ARRCLR(O): Ptr~l; END: ~ Initia Output ~ O~Ptr) O ~trl ~ In'ig Ptr ~ Ind xlPtr~1,Len) J Ptr alu~y- Doint- to end o- dol~-lir-:

REtURNlOutPut):

ND OI~Lin' REAL PROCEDURE Filt~rllNTEoER Ni.No: RE~L ARRAY Ic.Oc.P~.P~ ~t~thcL_~ INtE OE R Iptr.Optr: RE~L X(~)) C~ffNT Pl~cc Input X into ilt r and r-turn output. S-- FLTIO.SAI ~IO,J~Sl for tilt r doc w ent-tion lNi.No,lc,Oc). P~ Ni~l],Pu~l:Nol ~re - hi-tor~ ~rrJ~- for th 1ilt r.

Iptr.

Optr are ue-d int-rn~ RECIN Filter INTEGER i,j ~L Acc:

~e~ DI~Lin(Px.lptr.Ni.X~: J Purh input;

j-lptr ~ Point~ on- pa-t input;

FOR i 1 Thru Ni 00 ~cc ~ ~cc ~ ICli]~Pxlj-lndex(;-1,Nii~ j- Opt~;

FOR i ~ 2 Ihru No W Ace ~ Acc ~ Ocli]~p~ nd-~ oll;

OlyLin(P~.Optr.No.Acc); ~ Output RETURN(Acc);

END 'Filt-r' r-~l proced~r- n~X~8SARR(inte~cr n; real arra~ ~) DC9 in '~axArrreal y ax.~:

intcgcr i. ninX ninX ~ ARRlNFO(~.lJ; Co--cnt Lo~er ~ub~cript Dound;

y a~ ~BS~uSninXl);

tor i~l ~tep 1 untii n-l do i- la~AB5(~ ninX])) > ~-aY then ~-a~-au;

r-turnl~-aY);

end naxArr-;

J V i br~tO;

REAL PRSCEDUR ~ibtato(REAL PcP~.PcR~.P~t~Rvf,F~; tNTE OE R ~iee);

8EGIN v;oratoOEFINE Pl.-3.141Sq~ES3589J9~-;

~UN RcAL Ang.Oang,R~cl.Rr~cl.Cranv.Pranv.Ranv.R;Sel;

oUN INTcGER Rcnt.Ri;

REAL Factor;

IF Ti-c Lc~ I THEN 3EGlN Ang.8;

O~PI 2~Pvf /F~;

R~cl 2~PcRv Rcnt~F~JRvf~0.5: # Period ot randoe vibrato:

Rr~cl.1.~fRcnt;

Ri.8;

~0:

IF ~pcRv~a) AND (pcpv~o) nHEN RErURN(1) F-ctor 1 ~ PcP~ SlN(Ar~) ~ Gr-nv Anq An~ ~ Oang IF Ri.~ rHEN efcGlN Pran~ , R-rv STP~N13/00 C2. 86/10/17-1 Att:y.

Docket No.: STAN4983-2DEL Stan Ref: S83-043 1 3~8~ AP P~ND I X C COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY Oct 19~i 21:2S vS.KF tLl8.J05il PAOE 1-3 R~nv R-cl-(RAN~O~-O S) Cr nv ~ Pr~nv RiSci ~ IR~nv-Pr~nvluRr~cl ENO ELS~ Cr~nv _ Pranv ~ RiJR Sc Ri Ri~I IF Ri OE G Rcnt nhEN Ri_Q RETURN(f~ctor~ END vibr~to ~ 80~ noiae REAL PROC3URE 80uNoi~-(R~AL PcBn 8nf F-; INTE OE R Tioe);

OE GIN 80~Noi ae OUN RE~L R-cl Rr~c~ Cr~nv Pr~nv Ranv RiScl;

OUN INTE OER Rcnt Ri RE~L F~ctor IF PcBn.Q nHEN RETuRN(Q) IF Tioe EO l THEN 8GIN R-cl 2~PcBn Rcnt-F~/8nf~0 5 # Period of r~ndo- Bo~Noi~ Rr~cl~1 8/Rcnt Ri~4 END IF Ri.~ THEN BGIN Pranv ~ Ranv R~nv ~ R-cl~(RAN(~) -a. s~:

Cranv Pranv ; RiScl ~ (Ranv-Pranv1sRr~cl END ELSE Cranv ~ Pranv ~ Ri~RiScl Ri ~ Ri-l IF Ri GEO Rcnt nHEN Ri~a RETURN(Cranv) EYC Bo~Noi~e ~ Fi~-d-point ~inder - INTEGER PROCEDUR FP(INT~GER ARRAY F INTE OE R Nt D Re~ R~L A p(l~ BOOLE~N Su--(FALSE)) C~nnENT Solve F(~ 3 for ~ F i~ declar-d ~l N I Dut con-iderrd c ntered ~Dout ~-8 F~nl i~ u--d po~itiv- for n in ~1 nidLoe~ It S~ TRU F~n~ a~u-ed po~itive ever~u~ere - Oth-rui-e it i- ~--u d n 4~tivo in t~ rig~t h~l~ ~idLoc-I ~tl (S~ TRUE tor cl~rin-t flut- ~nd oog~n FALS to Dou o ~tring ) Re~ i- t~e de~ired acc~r c~ in ~ Not- t~t th- Fri-di~nder in~t~Dilit~ i- not n~c---~rii~ r--ol~-d for the a~- S~-- F~L BGIN FP INTEGER L~ UD i D~ FY INtEGER ~ ~ Thi- (-nd o~ hould o- r-JI ~ut h~r- ~ u~nt ~p d STP.N13/00 C3. 86/10/1?-1 Att.y.

Docket No.: STAN4983-2DELStan Ref: S83-043 1 3358~3 APPENDIX C COPYRIGHT 1986 - THE BOARD O~ TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct l9J6 21:25 VS.NF~ ~18.JO5il PAGE 1-~ INTE OER nidLoc: ~ riddl- point ot F curve dLoc Nt LSIH ~ F ~ould b- di-continuo~- ~t eidloc~-idloc-l it not S~x-;

~D~ ~idLoe-D: ~ Slop- ot lin~ lu~y~ po-itiv~ IF LD~1 THEN P~INTI- FP: ID ' LD.~ Nou -t to '.Lb 1.CrLt):

IF LD~N- THEN PRINT~' FP: uD ' LD 'I No~ -t to ' LD-Nf Cr'f~;

UD IIF S~ THEN ~idLoc~o ELSE ~idLoc~: ~ U~per tiJ~t ot ~e~rc~ IF LD~nidLoc ThEN OEGIN '~u p' i--LD:

Lb (lF Sy-n THEN Ub ELSE nidLoc~11:

U~;:

ENO '~u~p' ~ - ~Ub~LD) LSH -1; ~ ~iddle Ox ~Ub-Lbi LSH -1: ~ Fir-t tep--;2- ti--- 2:

D o - nidLoc ~ vi-u thi~ a- tr~n~lating x to c-nt-r at ~ D-lou:

U~ILE Ox>Re~ OO LEGIN '~i~ect' Ox ~ Ox ~S~ H~lv~ the ~t~p-~i2~ IF A-pJFl~l>x~b THEN ~ G~ nlN Ub ELSE x ~ Y-Ox ~AX Lb: ~ Slope po~itive:

ENO '8i~ect' IF Trace2 THEN 3Glh 'loo~' STRlNG ~ INTFGFR Id~;.Dp~si 2 OUN INTEOE R Nbuait RE~L AFR~Y Dp~8uft1:Nt~ REAL d ax.drin:

IF Nuait LEa 0 THEN 8EGIN FOR i 1 STEP 1 U~tlL Nf DO Op~Butli~ - A-p~F~i~ Id~F;

OpuSi2 ~ 3*Nf~10QZ d~ax, nax~rr(NF.Opy8uf) n~x NF~b drin ninArr(NF.Opu2ufl nlN 1~D:

Dp~OvllOP~But.Nf.ld.-VELOClTy-.~vELoclTy~d in.d ax~-512.512.

FULSE.TRUE.OpySi 2):

FOR i 1 STEP 1 UNtlL N- OO DDYBUf ~ i4b Opyovl(opy8u~.Nf.ld~NuLL.NuLL.dein.d-ax -512.512.FALSE.FALSE):

ARRCLRtOp~8uf):

op~au- W _A psFlx~ Opyovl(oD~But.Nt~ld.NuLL~NuLL~d~in.d-ax~-sl2~sl2 TRUE.FALSE):

F (~lNCHUL)--u- OR T~.`U- THEh Op~Urt(ld.FRIC.P~T-) -L Nu~it ~ INtS~AN(T~.01 F Nuait~0 THEN Trac- ~ Trace XOR Trace2 ~ Turn ott t~i~ trac-:

DRELS(ldl ENO:

IF Nu~it>0 THEN Nu~it Nuait-1:

END loo~-:

RETURN (Y-n idL~c) EN3 FP Bo~-~tring int~r~ction RAL PROCEDURE Bo4Eftcct~l~rEGER U~RAY Friction INTEGER NF.V.~b(25Ei);

RE~L ~b(1)):

CtrrENT Coeput- the ~dditiV - v-locit~ i-p rt-d to t~ tring tro- t~o Dou ~n th- D~ ot curr-nt ~tring v-iocit~ (~).

Dou ~-locity (~b).

~nd ~o~ pr--~ur- (Pb). T~ tuo D~ric tt-ct- u--d to d t r~in~ STi~N13/00 C4. 86/10/17-1 At~y.

Docket No.: STAN4983-2DELStan Ref: S83-043 APPENDIX C 1 3 ~ 5 & 4 0 COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY ~Octl~ Z12~ v5.NfF~IB,~Xi~ P~ 1-5 thi~ ro Do~ triction nd ~t~ing u ~ c i~d~ c- r~ ~".~ F~iction~1 Nfl ~ u d to cont~in riction-~ J~ t~nce tunction o volocitu uith ~-ro v-locitu co-r-~ponding to thC oiddl- o~ th- rr u ~ ~2) 3EGIN ~o~E -ct REAL Vip Vo;

Vip VD - Y. U~v- ~a-itt nc- Iin- i- lu~ through (-Vip.Vip~ If PD.O THfN RETURN(8) J Vo ~ fP(Friction N~ Vip 1~PD)~V;PS ~ Find Vp~Vip int r~oct FrictionlVp) Vo FP~frictior~Nf~Vip~l Pbi Pl~ Ioop ~dd- in Yi RETuRN(vo) fN BouE~fect ;

Si pli~ied ~ou-~tring intcraction - Huper~olic triction curv Rf~L Pf~XEDURE R~per80~(RAL Vi Vb Pb) C~r~ENT Co-putc the ~dditi~ velocitu iup rt-d to th- tring fro- thc bo~ or the D~ of cunren ~tring v-locitu (Vil Dou v-locitu (VD) and oo~ prc~ure (Pb) Thc tuo b~-ic ffect~ u~ed to det---ine tOi~ ~ro bo~ friction ~nd ~tring ~o i-~ c~ Thc ~u~tion~ uhich u~t oo ~i-ult~n~ou~ ti~ficd arc Y t . dV t . F(V-Yb) .

FlVi+dV-vb) uhere Y ;~ the characteni~tic ad ittancc of th- ~tring i~ the torc~ of thc Dou on the ~tring ~nd f(V) i~ the force V velocit4 triction curve for the bou ~no ~tring ~ere ue u~e Y FtV) ~Pb/V a- th- friction curv- noru~li2ed Du Y Thu~ d~ ;~ found a~ the ~olution to dV -Pb~dY~V;-Yb) It i~ rcturned th- ~oount to ~dd to th- incident ~tring velocitu Yi to co-plu ~ith th- ph~ic~l con~tr-int~ ot Dou friction and ~tring u~ve i-pedance 3EGIN ~per~o~ _ RfAL Yib~d~vl Y2 Rad Tcp OUN INTEGER StCnt Slipping Ua~Slipping ViD ~ Vi - VD If Uav- ad-itt nc- Iin i~ ~lu~u- through (-Vbi VDi) If PD-~ THE~ RETURN(Q);

R~d _ ViD~viD - 4~PD IF Rad<O THEN BEGIN Stuc~ dV ~ -ViD S C ncel diffcronti~l v-locitu String i~ ~tuc~ to Oou E~D ` S tuc~ Q S OEGIN `Slip R~d S~RT(R~d)/2 T~p ~ -vib/2~ Y1 ~ T-C ~ R~d: ~ Tuo r~ olution- to t~o qu dr~tic (h~v~ ~ e i~n) V2 - T-p - R~J dV ~ (IF Vl>O THEN Y2 a SE Vl) ~f Alu~u~ t~- th- -~II--t olution Th~ ~DOV- ct~t-- nt i~ ov-r-i plif;-d A Dit hDul~ D ~int~in d uhich indic~t-- ~hcth r th- tring i~ tuc~ or ~1; w ing -l~tiv- to th- De~ Th n u ~lu u- t~- th- olution ~hich 1-~ u- in th- c~ t~t- if po-~iDI- It i- po--ibl- to h v- t~o tuci olution- in uhich c~- th bov- rul- li - choo~- t~ ~-~11 r c~nC- in volocit~) ~Dr~- prop rl~ Tho l-~-t-~ction rul- c n f~il u~ n th- tring i- in th- tuc~ ~t~tt~inC it out of t~t t-t- too oon STP~N13/00 C5. 86/10/17-1 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S83-043 APPENDIX C 3 ~ 5 ~ 4 COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE 'ELAND STANFORD JUNIOR UNIVERSITY 7 Oct ~9U6 21:2B vS.N~F ~IR.J051 PAOE 1-6 END Slip :

IF ~r~ce3 r~N BEGIN U~SliDpingrS'~wing Sliwing ~ (IF ~BS(Vi~dV vt,) ~ a.~88B801 T~EN F~LSE ELSE rRU~) IF U~Slipping ~ND NOT SIlDo~ng THEN BEGIN PRlNT(StCnt,- SLIRS .Cr~fl:

StCnt~B: END ELSE IF Nt3T Ua~Sli win9 ANO S~pDin9 THEN ~EGIN PRlNT(StCnt,- STlC~S-,CrLt) StCnt~O: EN3:

StCnt~StCnt~1:

END:

IF Tr x~2 THEN ôEGlN h I oc~STRING T~ INTEGER Id,i,Op~5i2:

OUN INTEGER N~Jit REAL X~cl, Y-a~, Y- i n,Xni n, X-ax INTEGER ~id:

DEFINE Ndpu,.-512-:

REAL ARR~Y Op~Bu-~1:Ndpul:

IF Nudit LEO 8 THEN BEGI~ plotStuc~: Sc~l~ 11:Ndpul to ~e ~-2-Pb,2-PD3 ~X~cl-(l-lid),X~c~iN~pu-nid)~ ~ Slip: Sc~ :Ndp~ to be 1-2~vib~2~vib~rx~ -nid).x~ Ndp~-nid)~ SlnPLE REAL PROCEDURE ItoV~lNTEGER i): RETURN((X~cl-li-nid3~;

SI~PLE INTEGER PRSCEDURE Vtol~F~AL V) RETURN~V/X c~) ~ nia ~ 0.5 n~X 1 ~IN Ndp~):

n id ~ Ndpy~2~ Yn~x _ ~IF NOT Slipping THEN 2~Pb E SE A85~2~(Vi -Vbl ) ) Y~in ~ -Y-ax Xn~ If NOT Slipping THEH 2~Pb ~LSE ABS(2~Vi-Vb))) X a~ ~ 2~ (~85 (Vb) nAX ABS(Vi~ nux A8S(Vi~dV));

X-in ~ -Xn~ X~cl ~ XoaY/(ll;d-l):

F~R i-1 STEP 1 UNTI.

Ndpu 00 DpuBut[iJ ~ (IF A S(ltov(i)-vb)>a.B8B8Bl T K N -Pb/((l~oV(i)-Vb)) ELSE 8) Op~Siz _ 3~Ndp~lBa Dp~0vl(DpuJBuf.Ndp~. d~B.(IF Sliwin9 THEN SLIP- a SE StUCX-)~- VELOCltY~ vELac l t ~- ~ y~ i n~ y~ . x-; n. x~ . FALsE . tRuE . op~s i z) FOR i-l ST-P 1. WTIE Ndp~l 00 Dp~uf~ ItoV(i)-Vi; ~ U~v- i ~~~ .c- IinDC~OVI(OP9 u-.NdP~.ld.NuLL~NuLL~ n.y~.x-in.xo~.f~LsE.F~LsE):

ARRCLR(DpuJ~u-):

Dp~But~Vto ~d~Vi)~ - dY; ~ Ev~lu~t- ~olution on i-~d~c- Iin :

Op~Ovl (Dpu u-.Ndpu,.ld.NULL.NULL.Y-in.Y--x.X-in.X-~.TRUE.FALSE);

F (T~_INCHUL).-~- OR T~.-U- nHFN Op~Unt(ld.-X.PET-) LSE Nu~it ~ INTS~AN(t~,8);

F Nu~it d THEN Tr co Tr x- XOR Tr-c 2: ~ Tulrn of- t~i~ tr c-:

ORELS(Id):

ENI plot-:

IF N~it>B THEN Nuait ~ Nu~it-1;

RETURN(dY);

p-r~ou-;

D cl~r~tion~;

oEFlNE F~ (u4):

DEFINE ~tn~ 961. n~Friction ~ l~2~):

INlEGE~ URR~Y Friction~l:N-r~ 30~--tring triction cur~ :

REAL ~RRA~ IcSI.OcSl.lcSr.OcSr.lcB.OcB~l:Fltn~x~; ~ Filt-r co-ttici nt~;

STAN13/00 C6. 86/10/17-1 Atty.

Docket No.: STAN4983-2DELStan Ref: S83-043 APPENDIX C 1 ~ 3 ~ ~ 4 ~ COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY Oct 19U6 21 2~ VS NFF ~IB J051 P~ 1-7 INTEGR NiSI NoSl NiSr NoSr~NiB NoB ~ filt-r ord-r~ INTEGER P Pl Pr CPr Ppr Hul ~ur i j~S~ D~N~f.NI,T~PO~8O~POt~N~t~I I.NO1a:

BOOLEAN H~pFric STRlNGi NutFilt-rFil- Bridg F;lt-rFil- 80d~Filt rFile ~oriodFile Frlc2~onFile T~RAL f~ Our Fr~ Eift REAL Boupo~ltion~Bo~v-locit~Boupr-~ulr- BF~Bv~B RAL Bvtc~Bptc~Bvpr~Bppr~Bv~Bpa- J Ti-e con-t~nt~ of attac~ plu~ n~oc var~ REAL BPdtc BPdo~ BPd~ BPfin tBp tBDd 4 Tio~ con~te of d-cau plu~ oc v~r~ REAL Dito SlipF J String di Dl~ce-ent ~nd Slip orcREAL Pdv F_Rv Pv Rvf Apc W r~P~D ~iDr~to p r~eter~ ~E~L PcBn 3n J Bou noi~o p~r~--t-r~ RE~L Stitfne~ Stiffn-re of ten-ion-ood ot tring;

RAL Bul~Force J Re~toring forc- dw to ~tiffn-~ Pc~n i~ the a-ount o~ r~ndo- noite to ~dd to Vb Bnf i~ th~ r~te in H2 ~t uhich neu noi~e ta-ple~ r- goner~ted uith inter edi~tnoi~- v~lue- oot~in-d bu lin ~r int-rpol-tion ;

RC~RD'POlNTER(Sndfile) SndPtr DefPtr;

OEFINE In(~)-lSndfil-:~SndPtr~ OEFINE Oef(Y)-lSn~Fil- ~D-fPtr~i J Input P~raveter~ PR;NT(CrL~ VS (violin Si-u'~tioni COnPlLER'LANNER~LENGTH(S~NC(C~PlLER'B~4NER T~D ein~ ll FOR 17~ CrLt) PRlNT(CrLt Trac- codee (~n~ co-bin~tion c n b add-d tog th r) 1 - Diepl~u Bod~ ~tring-v-locit~ ~ppli-d-torc- u~v-foro2 - Di~pla~ So~-etring ;nt~r~ction gr~phic~l olv-r 4 - Print nu-ber of ~a-ple~ ~tuc~ or tlipping. prin d-l~-line change~ 8 - Print ~tring di-pl~ce-ent 16 - Initializ- ~tring uith i-pul~- if not reading initi~l ~tat- fil~2 - Di~pl-u running overl~ o~ Ood~ output. appli-d force ~nd volocit~ ):

Trplni( 26) # ~11 CYceVt integer overflou (1) ~nd re~l uflo~ SUPCT 4 Adju-t Iin- ~ctiv~tion option-;

SETFORnAr(0 2) IF F~ LE~ ~ nHEN EGIN d f~ult~ # Th~ r- pr-~erv-d xro-~ C~LL ~nd START Net~ S J deoug onl~ Dur~1 Litt~8 4 F~17857 14 Frq~lX ~ Lou 6 on violir;

J F~1B8ae;

Frr~ 0 ~ Lou G on ~iolin ouPorition ~ 17 ~t ~uPo-ition ~ 1;

J ouV~Iocitu~ ~ ~Z ou~-locit~ ~ e~Aeeel ~ 88~1 ~tc ~ ~:

o~Pr-~ur- ~ 1 5 eLPr-~ur- ~ 1 Pt~ ~ 0 01 ePtc. o;

ePdtc ~ Lift/2 in ~ SouPr-~-ulr-~2:

Ouit TRUE;

SlipF . 18 peP~ ~ B~5; J T~ic ti r pite~ i- t~ p rioelie ~i~r~to ~c~r-io~;

STA~113/00 C7. 86/10/17-1 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S83-043 APPENDIX C ~ 3 3 ~ ~ 4 0 COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct ~9S6 21 2~ ~S NfF ~IB QS1 P~GE 1-~ PcR~ it81 ~ Tni~ ti--r pitch ic tho oa~ r-ndon ~iDr~to ~cur~lon P~t _ 5 5; ~ Pe~iodic ~iorato rat- ;n H2 R~ - 1C S R ndo~ r~to rat- in i~2 PcBn ~ 1 J o~ ~oi~ plitud :

Bn ~ o~ ~oi~- fr-quoncu ~40fric ~ rRuE; J ~uit riction cur~- h w rbol;c:

Stiffn~ ItSaa; # orc-~Str;nc~i pl~c-- nt Stitfnr~ fNO 'detauit~ J S t up dc~ault filt r~ ~nd friction cur~ NiSr-NoSr-l IcSr~ Si pl- rigid t-r-in~tion tor d-~ult nut NiSl~2 NoSI~l ScSl~1~-1cSli2~-S 49 # S;-pl- Iowpa~- tor d-tault OridgNiB~1 NoB~2 IcB~13- 81 IcB~2~ 0 99 ~ O-f~ult ~od~ io on--polc lo~pa~c i~l.2 J Should b- 0 5:

Nt ~ 512 FOR i~1 Thru 2S6 W Friction~i~ ilaxFriction~l257_i) # i~p roolic def~ult;

fOR i~257 Thru 512 W Friction~ na~Frict;on~(25Ei-;) UHILE TRUE 00 EEGIN 'O-niLoop UH-iE TRUE 00 3E IN GetP~r~eete-~' 'TRINC Buc~ Arg2 Arg1 C-d.Pro pt N~EGER Boolh~ Br~ Proxpt .

CrLf- Our( ~C~FS(~ur)~ ') Li~t(~C~t~ '~ Pitch('~C~f~(Frq)~ ') Cloc~rat-~'~C~t~lF~)~ ') ~axForce(' Cv~(Slipf)~ ) Trac<( ~C~S(Tr~ce)~ ) UrL ~ V-loci~{ UC~t~(BouV-locit~)~ tau- UC~ ~(BVtc) ) ~ccelbration(--,Cvf~lBo :~cc-l)~ ) ~ouPoo( ~Cv~olBouPooition)~ ti-fne-~( C~ ~(Stiftne-o)~ ) ~Crlf~ Forc-( Cvte(Bo~Pro- ur-)~ tau- ~C~f~(BPtc)~ ; Ulti-~t-Forc nlt('~--(BP-in)~ ' t~u.' Cvt~(aPdtc)~ OEFINE FN(Y) ~(IF x nHEN Y ELSE ~D--~ult> )) ) Cr~ Inout(P riod . ~FN(P riodFilo)~ friction FN(Fr;ctionF;l-)- CrL~ ~ut . ~FN(~utFilt rFil-~' Brid9- FN(Bridg Filt-rfil-)~ .

CrLfBod~ - FN(Bo~Filt rFil-)~'l or Not Sp c R-~d_Co-s~nd (Pro4~t Bud~l~ Arg2.Arg1 C-d) CAgE C-d ûF BCI~ S tP r~-~t~r~ 0 ~ur~RE~LSC~N~rg1 Br~) L Lift~RE~LSC~N(Argl Br~)s P Fr~REALSCAN Urgl.Br~) S Stifl~ rr Sr~ (Argi Br~)~ C F~RE~LSC~N Urgl 8r~) ~ SlipF~PF- SCJU (Arg1 Br~)s 'F CEGIN IF NO~ Argl rHEN AinR--l~r ~ nid4l- Bou Pr~sur- ) Q SE Bo~Pr---ur-~RE~LSCAN(A~g1.8r~J IF NO~ Arg2 n~EN AinR-~ Ptc Att~c~ ti _ con-t~nt ) ELSE BPtc~REULgU N(Arg2 Br~) NC STAN13/00 C8. 86/10/17-1 At ty .

Docket No .: STAN 4 9 8 3 - 2 DEL S tan Re f: 5 8 3 - 0 4 3 1 33~0 APPENDIX C COPYRIGHT 1986 - THE BOARD OF TRUSTE~S OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 Oct 19~6 21 25 VS NFF;LIB J~Sl PAGE 1-9 ~'U'l SiEGlN IF NOT A~rgl THN AinR~ Bp~in~Fin~l So~l Pr-~ur~ Lo~ i ELSE BPfin~REALSCAN(Argl,Br~ IF NT Arg2 rHN AinR~ Bpdtc Oec~l~ ti- con~t nt ) ELSE BPdtc~AEALSCAN(~rg2,8r~ i E~ v~l 8EGIN IF NOT ~rg1 THN ~inRe~1(80uVelocitl~, Fin~l 80u Vclocit~ ) ELSiE 80uY-locit~LSCANl~rgl,E~rl 3 IF NT A~rg2 Tl{3N AinR-~l(Bvtc~ Ti- con~t nt ) ELSE BVtc~RE~LSCAN(Arg2 Brl~) E~O ~'A'l BEGIN IF NDT Argl T~N AinRo~1(80uAccol,'~Con-t~nt) ôo~ Acccler~tion ) ELSE BouAcc-l ~LSCAN(Arg1,~r~ E-~O:

1 8 3 BouPo-ition~LSCAN(Arg1,8r~) EGIN Input IF NT Arg1 THEN OEGIN INTEGER Tt~ PRlNT('P-riod Fr;ction, Nut, Bridg, Bod~ Tt~ . TTYUP(TRUE) Ar91~-lNCllJ_:

TTYUP ITt~ci EtD IF Argl . 'P T)IEN OEGIN PRlNT( Sniti~l String-P-riod ):

SndPtr~;E~ARC( lNPUT SNI ,Nl~L,Oui-t) IF SndPtr NEO NLLIRECI~RO THEN aEGlN F~ln(Cloc~) Frq~F-/lnlN~a-p-) PeriodFil- In(Nauc) EHO:

E~ El_SE IF Arg1.'F' T~N SGIN IF NOT Ainlnt(Nt~512,'5i2- o- friction curv- ) 5R Nt<2 T~EN CIlNTlNUE 'GetP~ra-eter~ ;

8GIN INTEGER ,A p REA~L AfiRAY T-pU Ntl PRSNT( F-;ction cur~ FrictionFil- ~ G tArr(T p.Nt, FRlC SND ,Oui-t) H~pFric IFrictionFil- ~ NL L);

IF NT H,~pFric T~N tlEGlN ~ep ~ xFriction/A851T ptNt/2~; # Nore~1i2~ po~;

F~R i 1 Tilru Nt DO Frictionli~ ~ A-p~T p~il;

EN~:

EN~ ENo Q IF Argl. N THS-N BEGSN PRINT( Nut ) IF NOT G tFltlNiS~,~bSr,lcSr,~cSr,NutFilt~Fil-,Oui-t) THEN C~NTINUE G-tP~r ~ t r- :

~inlnt(ll~r ~ ~bSr-2 nAX E). P~ ~bl~ Oft- t for nut filt-r (l~aopl--i );

E~l ELSE IF EOU(Argl ~1 FOR 21, eR ) THEN I~EGIN IF NOT G tFlt(NiSl,NoSl,lcSl,OcSl,Bridg Filt rFil- Oui-t) THEN BEGIN ~ri* F;itorFil~L ~NTINUE G tP~ t r- E~D -1YST~13/00 C9. 86/10/17-1 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S83-043 APPENDIX C ~ 33 5 8 ~ O COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7 ûct ~9~6 21 21~ V5Ci NFFDLIE~ J06~ PAGE l-lB ~inlnt(~Hul ~ Nc51-2 n~x 0). P~ D-I-v O --t for tlr;d9 tilt r (-- pl~i');

~ND ELSE IF EoUlArgl~1 FOR 21 ~0 ) THEN 3EGIN IF NOT G~tFlt(NiB NoB le8 OcB Bod~filt rF;lo Ou;-t) TNEN 8EGIN 80d~Fi;t rFil-~NULL; CONTINUE G-iP r~ -t r- END E~ EL IF ~rg1- 8 nHEN PRINTI A biguou~ input option CrL~) ELSE PRINT(' No ~UCh ;ncut Dtion CrL~) END Input-:

~'N ~ 8EGIN 'Not Sip c' ~inRoal(PePv." P--iodie vibr~to r-lati~- ~ plitud ') AinR-~l~Pv- ' P riodic ~i~r~o rat- in H2') ~inRo~l(PcRv ' R~ndoo vibr~to r-lativ- a pl;tudb ) AinR-al(R~f ' R~naoo vibr~to r~t- in H~ ) AinR-al(Pc8n 80u noi~o r-l~ti~- ~ plitud ') AinRo~1(8nt 80u noi-- ~t- in H2 ) END Not-Sp-c 'T PRlNT(CrEf TR~C r-t to TR~cE INT8C~N(~ro1~8r~CrLf) '0' ûui~t ~ r~1 ~ Boolh~) 'E'` C~LL~ 'EXST') ' ' # For eo--ent~ or co--and pro~pt r-fr-~h ALT ~NE 'O niLoop':

CRl CNE G-tP r~-t-r~' -LS PRINT(' u~ t?' CrLt) END S~tP~r~-~t~r~' END 'G-tPar~o-tcr~' Our NI~NsLift P_F~Fr~ ~ 8 5 Pl PsBouPo~ition-Nul~O S~ ount ot rtring to l-tt of bou (touard br;dg-):

Pr ~ p _ Pl _ Hur # A-ount ot ~tring to th- r;oht o~ tho bou (tou~rd nutl IF 3Ptc L O THEN 8Ppr ~ 0 ELS~ BPpr ~ ~P -1/(8Ptc~f~)l # t r- r-tio for xpon~ntial ri-- at ti-~-con-ta~t:

IF 8Vtc L O ~ THEN BYpr ~ 0 ELSE eNpr XP -1/(8Vte~F~));

8P~ BouPr---ur-~ BPpr): # Additiv- con~t~nt to achi-vo ptotic v-luBY~ eouY-locity~(1-4Vpr) If BPdtc LE~ O nHEN eiPdpr 8 flSE BPdpr . EXP(-~/(OPdt dF~)) BPd~ Ptin~BouPr~ uro)~(1 SPdDr~;

If SndPtr~NULL!REC3RO THEN OE IN ~Ptr ~ NEU!REC3RD~SndFil-) ~lCloc~ ~ F~ (P C~ 16-D; t SAn ~or-~t ~(Spu~ ~ 2; ~ ~6-~it SAn ~or~t ~f~n~A-p)_ 1 ~ S-c to thi~ o for- ~riting out u t(~ ) 'TEST SND END ELS D-fPtr-SndPtr S t V th od-t eErIN 'AL~R REAL ARRAY aod~Out~l N~ Yinit~1 P~: ~ Output ign~l ~nd init;-l ~tring t~tREAL ARRAY Forc Out V-lOut~l Nl:

ffAL Yil Yl Yol Yir Yr Yr Vr-l Yr~ Yor Yb ~bp # String v-loeitio~ ~ ~ lo~ ~r- t~ d 1~4-l;no~ u~ d or id ~ tring prop~g tion RE~L ARRAY Sdlt1 Pl~ ~ Brid9- to Dou ~nd b~c~:

REAL ARRAY Sdr~l Pr~(l~PcR~PcP~ o~ to nut ~nd O~c~ STAN13/00 C10. 86/10/17-1 Atty.

Docket No.: STAN4983-2DELStan Ref: S83-043 1 335~40 APPENDIX C COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND STANFORD JUNIOR UNIVERSITY 7ûetl~ 21:2S ~.~F~IB,~5~ P~ ~ 8-lou ~- tho d~ -l;n ~ u~ or int rn~l ilt r d l~o~ RE~L ARR~Y Xdsrll N;~r~ dSr _ NoSrl J Nut-oid ~tring ~;ltor rS~to RE~L ~RR~Y Xds~ ],YdSl NoSII Bridc---id~ otrino ~i~t- rt~t-s REAL ~RRAY XdB ~ :Ni ~ da _ NoB 1 ebd~- ilt r ~tJto J B-lou zr- point-r~ to thc ilt-r--t~t- d l~rlin INTEGER SdlPtr,SdrPt- XdSlPtr,Ydslptr Xdsrptr~ydsrptr~xdBptr~ydBptr J Pl~ it:

~1f~ ~(0.5) IF SncPtr NEO NULL!RECORD THEN FOR i-l STEP 1 UNTIL P W Yin;t~il,ln(D~tz)li) ELSE IF Tr c-S t~N rinitll~l ELSI~ ~RRCLR(`rini~) v;l ~ Yl ~ Yol ~ Y;r ~ Yr ~ ~r Vrol - Yr~ ~ Yor ~ O # Z ro rtring ~t~tc dlPtr - SdrPtr XdSlPtr ~ ~dSlPtr XdSrPtr ~ YdSrPir XdOPtr ~ YdBptr ~ 1 P ~ BV ~ Oi~p ~ tBp ~ O: tBpd~l; Nol8 ~ N~l~ n~x l; Ppr~Pr;

J tuc~ ~ TFUE ~ 2~ro int;ti~l bou ~-locit~ .> tie~ing initizll~;

fOR SJ P-1 SnEP 1 UNTIL N 00 BEGIN PI~LooP OUN INTEGER NP~it IF S ~p noo Nol8 . 8 nHE~ PRINT( ~ ) # T~ ~ollouing ~loc~ ~ndl-- ~ibroto5 lEFIK Ep-- 8 Bl ~ Thi- zvoid- pol--z ro c nc-ll-tion in th- ~llp~-ePr ~ Pr~ibrc ~ SP PePv, W eRv,Pv .Rv ,F-,S~ p): # Dc-ir-d curr-nt p-riod pr DcPr-Ep- J Floor to got int-g r p rt o- d--ir d d l-~s p ~ DcPr-Cpr: J Oi t r-nc- in d-lJ~ to got uith ~llp~r~;

~pc ~ P~p)~ P~p); # ~llp~r co- ici-nt;

IF Cpr Ppr~l THEN BEGIN IF Tr c-3 n~EN PRlNrl incr-~ein~ d l-4rlin ~t ti-- ,S~ p~F~,Crl~)s FOR i~Cpr STEP -l UNrlL SdrPtr~l OO Sdrlil~Sdrt;-l~s Sdr~sdrptrl~vr-l # Add ~llp~-r del~J c-ll to nd of d~ -line:

Vrel ~ S: # I- thi- th- b--t po--ib1- r- t h r-?

Ppr .

Cpr;

EhO ELS IF Cp Pp -l THEN BEGIN IF Tr~c~3 n~ PRIN~I d cr-~-ing d l ~ -lin- ~t ti-- ,S~ p/Fr,Crlf) Vr-l Sdr~SdrPtr~: Pop l~-t d la~ I-- nt into ~llp~--;

FOR i~SdrPtr thru Cpr W Sdr~ Sdr~ # Co~ r doun:

Ppr ~ CPr:

E~ flSE IF Cpr NEQ Ppr rHEN PRlNrl O~ -lin- c~ng-d ~ ,Cpr-Ppr,Crlf) h- ~ollouing blOC~ h~ndl-- th- xpon nti~l otion of orc- nd v-locit~:

BV ~ BV~- BVprdV: ~ Expon nti~l ro z ro to fin l;

BV-~ ~ BV~ ~ BouAcc~ Int-gr~t~ ~co-l-r~tion tBp ~ BP~ ~ or~ lB~i ~ Att-c~s tBod ~ ~Pd~- ~ BP~ O~d, # D c~:

~P ~ tBr - B~d~ Nou tor t~ rtrino loop ri ul~tion Ytp ~ Yil ~ Yir # String v-locit~ und r t~o bou;

~p ~ Oi p ~ YDp Curr-nt di pl~c-- nt t th- ~ouing point ,ul~forc- ~ Stif~n--~Di~D # R--toring olre- du- to t n-ion incre-re f ~BS(Bul~foreel>~BS(aPI nHEN PRlNr(S- p. ~-- Bul~ ~orc~ e~c~ed~ bo~ or ~ ~n ~):

F S- C-NI n~EN PRlNTl ~I~Li~ting bo~))) ):

_~_ STA]N13/00 Cll. 86/10/17-1 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S83-043 1 3~5~40 APPENDIX C COPYRIGHT 1986 - THE BOARD OF TRUSTEES OF THE LELAND S,TANFORD JUNIOR UNIVERSITY ~0ct~ 2t-~ Vs.~F~lB~sl P~1-12 IF S- p~NI r~EN YO~ ou i~ li t-d, ~o~ ~Oa~ z ro l~ul~ torc- igncr-d) LS tF ~4sf-ie t~EN Yb .~ \~rl~o~Ybp.llY.I~ul~LForc-do~Noi--~PcSn.8n-,Fc,S~ p)) ~SE Ys~ ct~Friction.Nt,Ybp,BY,~-8ul~LForcei P~51ipF/~SlipF~Oi p~2tNt))) Forc-Out~c~ p]~Y~ ~ Stor- tPo~ orc-s V-IOut[S~ pl ~ YOps- ~nd trin~ ~-locit~5 IF tr c-4 thEN PRlNtlS~ p, ^ocu ~dd- ,Yb, to ,Yil-Yir, Oi p. ,Oi p, ~ul~Forc-. ,~ul~Forc- ;rLt) Yor Yil ~ Yb~ 5 J Outgoing ~-locit~ icn~l to t~e rig~t Yr ûl~Lin~Scr,5drPtr Ccr~yor) Sign-l 90 - cloc~ s t~e tollou;n~ ~llp~oo filt r pro~id c tr~ction-of-~ pl- d 1 Vr ~ Yr - ~pc~Vr-l Yr~ ~Vrel ~ Apc Vrs ~ Firct_order ~llp~o~5 Vr~l ~ Vr Yir ~ FilterlNisr~Nosr~lcsr~ocsr~xdsr~ydsr~xdsrptr~ydsrptr~yr~ Nut;

Yol Yir Yb~2 Outgoing to t~ l~-t IF S~op ~EO P THEN Yol ~ Yol ~ Yin;tC5~ p~ F--d in initi~l t~t-s Yl ~ DI~Lin~5dl.5dlPtr Pl Yol): J 0-1-~ on lo~ ~ I-ft of loop ~il Filt r~NiSI NoSI IeSI OeSI XdSI Y oe I XdSlPtr YdSlptc rl~ J BtidgyOutlS~ - F;lt r~NiB,NoB,lcB.Oc~,XdB Y~.XdBPtr,Yd9Ptr,YI) ~ E~,odu, F Tr~c l THEN IF ~(S~ p noD (NCt~ll~P))-o) THEN F NPu~it EO 0 nHEN BE-IN NTEGER Reod-:

F S~ p NEO N~t~ll P r~EN PTOSTR(8,CVS~S , N~t~ll P~ ,O Cr~, eo~ ~Dp~Ed~Bod~Du~,N-t~ll P, TlnE ~SEC~ , VELOCITY ) F eod->l ~HEN NP~it~aeod :

f ~eod- . T~EN Tr e- Tr e- XOR Tr~e-l ~ Turn otf t~i~ tr eF ~eode-0 HEN CONTINUE OoniLooD F Reode~1 -HEN CONTINUE PI~Loop F Reod<.l THEN PRINT~ Yb- ,Yb~ Yor~ ,Yor Yr. Yr Yir. ,Yir CrLt, Yol~ ,Yol. ~1~ YI Yil~ ,Yil ~od~Out. Bod~OutrS~-pl,CrE~) IF Reod-<-l THEN Tr e- ~ Tr e- XOR Tr eo1; ~ Turn of- t~ie tr~c-:

IF Rcod- -1 THEN CONTINUE PI~Loop ;

IF S~ p-N~t~ P~NL nHEN 8EGIN IF S~ p NEO N~t~ll P THEN PTOSrRl~ CYs~s~-p-N-t~ p)~ O U-);

Reodo~Dp4Ed~Forc Out N~t~ P TlrE ~SC) , FORC ):

F Reod->l rHE~ NP~ it~Reod ~ F Reod- O n~EN CO~TIN~E ObniLoop :

F Rcod->O n~EN CONTINUE PI~LooP F acod- -l ThEN Tr e- Tr e- xoa Tr eol; J Turn otf thi- tr~e-;

F Reod <-l nHEN CONTINUE Pl~yLOOP :

E1~:

IF Sxp NEa N-t-l I P THEN PTQSTR~B,CVSlS~p-N-t~ P)~ ,O-t):

Rcw~,:d~V-lOut,N t~ll P,-TIrE (C)-,-V-Iocit~ f cod > W~ NP~Di t~Rcod:

'f ~cod-- THEN CWTINL~ niLooP-:

f ~cod ~ ThEN C~TlNl~ PI~Loop-F Rcoo~<-l ~N Tr~ ~ Trx- XOR ;rx-l; ~ Turn ott th;C tr~C~ If TrKC6 TI~N 80d~put,Fo--c IDut,V-lOut,5~ , Forc~, V-loci t~ E~ EL NPu~it ~ NP~it-l EL EL:

ENI P I ~Loop-;

OECIN RE~L n,~p. ~c l;

-q1STAN13/00 C12. 86/10/17-1 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S83-043 APPENDIX C 1 3 3 5 ~ 4 û COPYRIGHT 1986 - THE BOARD ~F TRUSTEES - - OF THE LELAND STANFORD JUNIOR UNIVERSITY Oet l~S6 21s2~ V5~llFF~~ oe) P~ 1-13 I N~EOER i ~ r I~l,~Out~;

Sel . 1~ f~ u 11 00 ~put ~ k~Out ~ i l ~Sc l rr (N. F~re-Out ) s SC ~ F~l i~l Tr~ru ~1 00 Forc Outtil ~ Fore-Outlil Selt ~p ~ n ~ rr IN.V-lOut):

Se I ~ 1 ~A~ Fl~ ;~1 Tlru 1~ 00 V-lOutIi~ ~ VelOuttil*sel;

'RINT (- 4~ ' ) ;

~utSnd(~Out.N.D-f ~N~_I .O-tPtr~;

~RIN~ 1- b~r6tr in~ torr.- ) ~utS-d( ore Out.N.O~ tPtr) PRIN~ tr i ngV- l oe i t~tll~ ) s P~tSnd(~lOut.N.D-- (N_) .D-tPtr):

E~O O-n iLooP-;

EJO vs-;

STAN13/00 C13. 86/10/17-1 Atty.

Docket No.: STAN4983-2DEL Stan Ref: S83-043