Piezoelectric driver using resonant energy transfer.

<b>Background of the Invention</b>

This invention relates to a drive circuit for driving a capacitive load such as a piezoelectric element.

In applications where a piezoelectric element or similar capacitive-type load is coupled to a drive circuit, it is desirable to produce a high output to the load without wasting a great amount of energy. Piezoelectric elements are commonly used to generate an audible alarm by driving them with an AC voltage, which causes the piezoelectric elements to vibrate at their natural oscillation frequency and in time with the voltage, producing a sound. This is especially useful where it is important that the circuit elements not take up much space, such as in a heart pacemaker. A piezoelectric element is smaller and requires less energy to drive than an electromagnetic device, and can be supplied with energy from very compact batteries. The piezoelectric element also can be used in an implanted drug pump, the vibrations of the element being used to initiate the flow of a drug into the body.

The efficiency of the drive circuit can be increased, and the amount of energy dissipated as heat or otherwise lost can be decreased, by using a resonant drive circuit where the piezoelectric element, or capacitive load, is connected in series with an inductive element. The two form what is known as an L-C circuit, in which an inductor (L) and capacitor (C) comprise reactive elements whose impedances change with the frequency of an applied voltage. An L-C circuit has a resonant frequency at which the reactive impedances of the inductor and capacitor exactly cancel each other, and at which maximum energy transfer occurs. As a consequence, the L-C circuit comprises a resonant energy transfer system that can produce an instantaneous output voltage to the capacitor many times larger than the supply voltage with minimal energy lost as heat. The frequency at which resonance occurs will depend on the inductance and capacitance values.

In an L-C resonant drive circuit, if the piezoelectric element is to be used to produce an audible signal, the element must vibrate in the audible frequency range, preferably at approximately 1 kHz. That is, the supply voltage must be applied at this frequency. Typical piezoelectric elements that vibrate in this frequency range and that are suitable for implantation have capacitance values for which corresponding inductors are unfortunately too large to be implanted. Moreover, an inductor small enough to be implanted, when combined with a typical piezoelectric element, would correspond to a resonant frequency on the order of 100 kHz, well above the frequency range of human hearing.

A drive circuit in accordance with the preamble of claim 1 is known from US-A-4,763,789. In the known drive circuit the frequency of switching between the supply voltage and the reference potential is controllable, so that a desired frequence of the L-C circuit is obtained. The voltage across the capacitive load, however, is not controllable. The invention as claimed is intended to remedy this drawback.

<b>Summary of the Invention</b>

The present invention as defined in the claims provides a resonant energy transfer system, for transferring energy from a supply voltage source to a capacitive load, comprising a drive circuit that makes use of otherwise lost energy stored in the load and returns it back to the load, that operates under a wide range of drive frequencies, and that cyclically produces peak voltages at the capacitive load that are substantially greater than the supply voltage. In accordance with the present invention, the supply voltage charges the load to the supply voltage level during the first quarter of the drive circuit voltage cycle while a current flows through the inductive element. When the capacitive load reaches a voltage level equal to the supply voltage, the current through the inductive element peaks and the inductive element reaches its maximum energy storage level. It then delivers its stored energy back to the load in the form of a decreasing current. As the inductive element augments the load's charge after the current peak, the current in the inductive element decreases to zero as the load voltage swings about the supply voltage and increases to its peak value.

After a predetermined waiting time interval, the second half of the voltage cycle is started when the supply voltage is removed from the circuit and the capacitive load is discharged and, in doing so, transfers energy back to the inductive element while current in the circuit flows in the opposite or negative direction from before. When the load voltage reaches zero, the current through the inductive element reaches its peak negative value and then delivers its stored energy back to the load. That is, the energy from the inductive element induces a charge on the capacitive load symmetric about a reference voltage, such as ground or zero, until the current through the inductive element again reaches zero, ending the cycle with the load having its peak negative voltage.

After a predetermined waiting time interval, the process can be resumed with the application of the supply voltage to the capacitive load and the discharging of the load. The capacitive load, for example, can comprise a piezoelectric element for providing an audible warning signal or for driving a drug pump. The augmented charging and discharging, which theoretically could continue indefinitely, is limited by system losses but nevertheless can produce an instantaneous output voltage many times the supply voltage. The output is advantageously controlled by the energy limiting means that limits the voltage produced at the capacitive load.

The charging and discharging of the inductive element and capacitive load, and the transferring of the stored energy from the load and the inductive element back to the inductive element and the load, respectively, can be controlled by a pair of MOSFET-type transistors of opposite polarity that are connected to the inductive element and capacitive load by a pair of diodes. A single square wave voltage source can be connected to each of the transistors' gates to thereby control the transistors, whose drains are connected to the diodes. One of the transistors is connected to the supply voltage and the other is connected to ground. Using one of the transistors to control application of the supply voltage and the other to apply a reference potential or ground, the system transfers energy between the inductive element and the load in symmetric swings about the supply voltage and the reference potential. The diodes help ensure that current is provided to the appropriate transistor. Repeated cyclic transfers of this type can produce an instantaneous output voltage many times the supply voltage, limited in practical terms only by system losses and what is known as the quality factor of the circuit.

Other features and advantages of the present invention will become apparent from the following detailed description, taken in conjunction with the accompanying drawings, which illustrate by way of example, the principles of the invention.

<b>Brief Description of the Drawings</b>

FIG. 1 is a schematic diagram of a drive circuit.

FIG. 2 is a timing diagram for various waveforms of the drive circuit illustrated in FIG. 1.

FIG. 3 is a schematic diagram of a drive circuit of the type illustrated in FIG. 1, further incorporating a peak controller in accordance with the invention.

FIG. 4 is a timing diagram for various waveforms of the drive circuit illustrated in FIG. 3.

<b>Description of the Preferred Embodiment</b>

A resonant energy transfer system in accordance with the present invention, which has utility in an implantable heart pacemaker, drug pump, or the like is illustrated in FIG. 1. The system includes a piezoelectric element 10 connected to a drive circuit 12. As known to those skilled in the art, the piezoelectric element vibrates when it is driven by an AC voltage. This makes the piezoelectric element suitable for audible alarms or implantable drug pumps. An inductor 14 of the drive circuit is connected in series with the piezoelectric element.

A supply voltage source 16 is connected to the circuit 12 and produces a voltage +V that is supplied to the piezoelectric element 10 and inductor 14. Together, the piezoelectric element and inductor comprise an L-C circuit having a resonant frequency f_R at which maximum energy transfer occurs. This decreases the amount of energy that is wasted as heat, which is critical for applications where the system is to be implanted. Unfortunately, an inductor that is small enough to be implanted in a human body typically has a resonant frequency that, along with a typical corresponding piezoelectric element, results in a resonant frequency on the order of 100 kHz. This is well above the frequency range of human hearing. An inductor that would provide a low enough resonant frequency for the circuit, on the order of 1 kHz, is too large to be implanted. The circuit 12 makes it possible to drive the piezoelectric element with a voltage that will produce an audible vibration while producing resonant transfer of energy such that an output voltage much larger than the supply voltage can be produced.

The drive circuit 12 includes a first transistor 18 and a second transistor 20. The transistors advantageously comprise MOSFET-type transistors of opposite polarity whose gate terminals are connected via a line 21 to a square-wave voltage source 22 producing a drive voltage V_A having a predetermined frequency. That is, a single drive voltage controls both transistors. The drain terminals of the first and second transistors 18 and 20 are connected to the inductor 14 by first and second diodes 24 and 26, respectively. The cathode side of the first diode is connected to the first transistor 18, while the anode side of the second diode is connected to the second transistor 20. The diodes are connected at a common junction 27 labeled B. The supply voltage source 16 is connected to the source terminal of the second transistor 20. The source terminal of the first transistor 18 is connected to a reference voltage, such as ground.

The operation of the system illustrated in FIG. 1 is best understood with reference to the timing diagrams of FIG. 2, which illustrate the drive voltage V_A, the voltage V_B of the junction 27, the voltage V_L of the inductor 14, the voltage V_C of the piezoelectric element 10, and the inductor current I_L. As known to those skilled in the art, the piezoelectric element acts like a capacitive load and therefore it stores energy, as does the inductor. In FIG. 2, the piezoelectric element 10 is initially without charge, or is at zero voltage, and the drive voltage V_A is high. The first transistor 18 18 is an n-channel or NMOS-type MOSFET and the second transistor 20 is a p-channel or PMOS-type MOSFET. Therefore, when the drive voltage V_A is high, the first transistor 18 is biased on, or is put in a conducting state, and the second transistor 20 is biased off, or put in a non-conducting state.

At time T1, the drive voltage V_A drops to zero, so that the first transistor 18 is biased off and the second transistor 20 is biased on. Because the second transistor 20 is now conducting, a current flows in the drive circuit 12, creating an inductor current I_L and charging the capacitive load 10 to a voltage level equal to the supply voltage +V in a time period equal to one quarter the cycle time of the resonant frequency f_R. When the voltage V_C on the capacitive load reaches the supply voltage, at time T2, the energy stored in the inductor 14 reaches its maximum value as the inductor current I_L reaches its maximum, while the inductor voltage V_L reaches zero. The energy stored in the inductor continues to charge the load as the inductor current I_L decreases to zero at time T3. That is, the energy stored in the inductor 16 has decreased to zero when the inductor current I_L reaches zero and the voltage across the load reaches +2V, at time T3 in another quarter cycle of the resonant frequency f_R. The time interval from T1 to T3 represents one-half the cycle time at the resonant frequency of the L-C circuit. At time T3, the capacitive load 10 is charged but cannot discharge through the second diode 26, which is reverse-biased as indicated by the voltage at V_B in FIG. 2. Thus, the diode 26 stops the current I_L at half-cycle and prevents it from swinging back in the reverse direction. Therefore, the transistor timing for biasing on and off is not as critical as it otherwise would be, as the diode helps control the current direction to the correct transistor.

The time interval from T3 to T4 constitutes a waiting time interval, after which the second half of the drive circuit 12 voltage cycle is begun when the drive voltage V_A again becomes high at time T4. The waiting time interval is typically part of a predetermined interval from time T1 to T4 that depends on the desired frequency of voltage applied to the piezoelectric load 10, and is controlled by the drive voltage source 22. When the drive voltage V_A becomes high at time T4, the first transistor 18 is biased on, or begins conducting, and the second transistor 20 is biased off. The supply voltage +V is thereby cut off from the circuit, and the piezoelectric load 10 discharges through the first diode 24 and the first transistor 18.

When the piezoelectric load 10 discharges, current I_L flows through the inductor 14 again, but in the opposite direction from before. The inductor current I_L reaches its negative peak at time T5 after another quarter cycle when the piezoelectric load 10 has fully discharged and the inductor voltage V_L is equal to zero. That is, all the energy previously stored in the load 10 is now stored in the inductor 14 as the load voltage has gone from +2V to zero. The inductor 14 then releases its stored energy, again in the opposite direction from before, and therefore releases sufficient energy from time T5 to T6 to charge the load 10 to an equal but opposite charge as before, that is, from zero to -2V. Thus, at time T6, the inductor current I_L reaches zero and the piezoelectric voltage V_C reaches -2V.

After another waiting time interval from time T6 to T7, the first voltage cycle is ended when the drive voltage V_A again drops at time T7. Again, the waiting time interval on V_A is controlled by the drive voltage source 22. When the drive voltage V_A drops at time T7, the second transistor 20 again conducts, and the supply voltage +V is again connected to the inductor 14 and piezoelectric element 10. Once again, current will flow through the inductor 14 until the voltage across the piezoelectric load 10 is equal to the supply voltage, +V, at time T8. At this point, current through the inductor 14 reaches its maximum, and the inductor 14 is fully charged. The inductor 14 then releases its energy into the load 10 from time T8 to T9, augmenting the charge on the load 10.

Because the voltage across the load 10 changed during time T7 to T8 from -2V to +V while the inductor 14 was being charged, a change of three supply voltage units V, the energy released during time T8 to T9 from the inductor 14 as it discharges will correspond to the higher voltage and therefore will be sufficient to increase the voltage V_C across the load 10 by three supply voltage units. Therefore, the voltage V_C across the piezoelectric load 10 during time T8 to T9 will swing about the supply voltage and will increase from +V to +4V. At time T9, the inductor 14 has released all of its energy, the inductor current I_L has dropped to zero, and the voltage V_C across the load 10 has reached its maximum. After a waiting time interval from time T9 to T10, the next half of the voltage cycle begins when the drive voltage V_A rises at time T10.

At the beginning of the second half of the second voltage cycle at time T10, the second transistor 20 is biased off and the first transistor 18 begins conducting when V_A rises. This discharges the piezoelectric load 10, which produces a current I_L through the inductor 14. The inductor current I_L reaches its peak at time T11 when the voltage across the load 10 goes from +4V to zero, a difference across the load 10 of four supply voltage units. Therefore, when the inductor 14 releases its stored energy in the opposite direction from time T11 to T12, charging the piezoelectric load 10 to an opposite polarity, the inductor 14 produces a load voltage V_C having an equal but opposite magnitude, namely, -4V. After a waiting time interval from time T12 to T13, the second voltage cycle terminates at time T13 and the third voltage cycle begins when the drive voltage V_A again drops and the load voltage V_C swings symmetrically about the supply voltage, changing from -4V to +V and from +V to +6V.

For resonant energy transfer, the supply voltage +V should be applied at a frequency less than the resonant frequency f_R of the circuit 12 in combination with the load 10. The waiting time interval during each half cycle, such as the interval from time T3 to T4 and from time T6 to T7, can be selected to produce the desired audio output where the capacitive load 10 comprises a piezoelectric element. For example, if the L-C circuit in accordance with the invention comprises the piezoelectric element 10 and the inductor 14 and has a resonant frequency of 100 kHz, making them small enough to be implanted, then a complete cycle of charging and recharging would comprise two polarity reversals on the piezoelectric load 10 and, with no waiting time interval, would occur 200,000 times per second and take five microseconds to complete. That is, the supply voltage +V would be applied at the resonant frequency of the L-C circuit and the piezoelectric element 10 would vibrate accordingly.

If, however, the time interval for each half cycle is controlled by the drive voltage source 22 to increase from five microseconds to one-half of a millisecond (500 microseconds), making the time for a complete cycle from time T1 to T7, for example, equal to 1000 microseconds, the piezoelectric element 10 will vibrate at a frequency of approximately 1 kHz. Thus, even though the inductive and capacitive components might be small enough to be implanted and, therefore, have a resonant frequency beyond the audible range, the circuit 12 can utilize a predetermined half-cycle time period to produce an audible frequency at the capacitive load 10 while still providing resonant application of energy from the supply 16. Thus, the waiting time interval is contained within the half-cycle time. Moreover, using a single drive signal V_A simplifies the control of the two transistors 18 and 20. The use of a single drive signal is made possible by the selection of two transistors of opposite polarity.

In theory, the augmented charging and discharging of the capacitive load 10 about the supply voltage +V could continue indefinitely. In actuality, the swings in voltage are not quite so large as depicted, due to losses in the various circuit components, and are limited by a circuit characteristic known as the quality factor Q. That is, the maximum instantaneous output voltage across the load 10 will be 2Q*V/π. As known to those skilled in the art, Q is equal to the ratio of the reactive element impedance, L or C, to the pure resistance of the circuit. In practice, the Q value can be on the order of 50 or 100. Thus, the resonant energy transfer circuit 12 can generate an output voltage having an instantaneous output value much greater than the supply voltage.

FIG. 3 is a diagram of a drive circuit 13 in which the positive swing of the output voltage can be precisely controlled, and made to swing about a reference potential, such as ground or zero, rather than the supply voltage +V when an energy increase is not wanted. The circuit illustrated in FIG. 3 includes the same basic elements as illustrated in FIG. 2, in which like elements have like reference numerals. Therefore, transistors 18, 20 of opposite polarity are used. In FIG. 3, however, the gate of the second transistor 20 is connected to an OR-gate 30. One input terminal of the OR-gate 30 is connected via a line 31 to the drive signal source 22, while the other input terminal of the OR-gate 30 is connected via a line 32 to a controller 34. The controller 34 is connected via a line 35 to the circuit between the inductor 14 and the piezoelectric load 10. When the magnitude of the load voltage V_C gets larger than a predetermined amount, such as +4V, the controller 34 raises its output level on the line 32 to the OR-gate, thereby biasing the second transistor 20 off and cutting off the supply voltage source 16, limiting any additional transfer of energy to the load 10.

The controller 34 can be selected to respond to any condition that corresponds to the occurrence of the maximum load voltage desired, such as maximum power output or drug pump pressure.

A third MOSFET-type transistor 36 is coupled to the circuit 13 by the anode side of a third diode 38. The cathode side of the third diode 38 is connected to the junction point 27. The gate terminal of the third transistor 36 is coupled by a coupling capacitor 40 to the drive signal source 22. The third transistor 36 is of the same polarity as the second transistor 20, and therefore the third transistor 36 turns on and off with the drive signal V_A as did the second transistor 20 in FIG. 2. The gate terminal of the third transistor 36 is also connected to the reference voltage by a fourth diode 42. The fourth diode 42 ensures that only negative voltage is coupled to the gate of the third transistor 36. Finally, the source terminal of the third transistor 36 is connected via a line 44 to the reference potential.

Those skilled in the art will recognize that the third transistor 36 and the second transistor 20 are similarly connected to the L-C circuit comprising the piezoelectric load 10 and the inductor 14, their drains being connected by diodes to the junction point 27 and their gates being connected to the drive signal source 22, the difference being that the second transistor's 20 gate is connected to the drive signal V_A via the OR-gate 30 via a line 29 and its source terminal is connected to the supply voltage source 16, while the third transistor's 36 gate is connected to the drive signal V_A via the coupling capacitor 40 and its source terminal is connected to the reference potential, or ground. Thus, by using the controller 34 to bias off the second transistor 20, the positive swing of the voltage across the load 10 can be made to swing about ground, or zero, rather than the supply voltage +V. The diodes 24 and 38 are used to steer the current, so that the transistor that receives current is the one that needs current. In addition, the diodes 24, 26, and 38 help to catch the current at a half-cycle point to control the charging and recharging cycles of the load 10. In this way, the voltage level across the load 10 is kept to a predetermined maximum value.

The operation of the FIG. 3 circuit is best understood with reference to the timing diagrams of FIG. 4. The timing diagrams illustrate the drive voltage V_A and controller voltage V_CONTROL, the voltage V_L of the inductor 14, the voltage V_C of the piezoelectric element 10, and the inductor current I_L. In the example illustrated in FIG. 4, the controller 34 of the drive circuit 13 is selected to allow a maximum load voltage V_C of +4V. The first voltage cycle and part of the second cycle, from time T1 through time T9, is identical to that shown in FIG. 2. Therefore, the waiting time intervals are controlled by the drive signal source 22 to produce the desired frequency, and the second voltage cycle begins at time T7 when V_A drops, biasing on the second transistor 20 and the third transistor 36, and connecting the supply voltage source 16 to the circuit and discharging the load 10. At time T8, the voltage across the load 10 has swung from -2V to zero and up to +V, and begins to swing upwardly about the supply voltage to reach its peak of +4V at time T9.

At time T9, the controller 34 recognizes that the maximum load voltage of +4V has been reached, and raises its output level V_CONTROL the line 32, thereby raising the output of the OR-gate 30 on the line 29, biasing off the second transistor 20 and removing the supply voltage source 16 from the circuit 13. The third transistor 36 remains conducting, however, and therefore any positive current can continue to flow through the inductor 14, through the load 10, into ground, up through the line 44, through the third transistor 36 and the third diode 38, and back to the inductor. Thus, the diodes 24, 26, and 38 help to steer the current to the right transistor. After a waiting time interval, the drive signal V_A again becomes high, turning on the first transistor 18, thereby discharging the capacitive load 10, charging the inductor 14 and recharging the load 10 to -4V, and so on. Thus, the voltage V_C across the capacitive load 10 can be set to alternate about a predetermined value, such as zero, rather than continuing to swing symmetrically in increasing amplitude about the supply voltage +V on positive voltage swings.

The present invention therefore uses a supply voltage and an L-C circuit to provide resonant transfer of energy from a capacitive load to an inductive element and back to the capacitive load, that otherwise would be dissipated as heat. Furthermore, the circuit operates under a wide range of drive frequencies. That is, where a predetermined frequency is desired for driving a capacitive load that is a piezoelectric element, the components can be selected for optimal size, such as for implantation, and the piezoelectric frequency of vibration can be set to the desired amount by adjusting a waiting time interval. Finally, the circuit is capable of producing instantaneous peak voltages across the capacitive load that are many times the size of the supply voltage. The present invention thereby provides an extremely efficient transfer of energy and a wide range of applications.

<b>Reference list</b>

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