Nova Patents
US2006099A

Audion amplifier

Abstract

This record has no abstract on file.

US2006099A, drawing sheet 1
Sheet 1 of 3

Term

Term ended

Expired 10 August 1953, 73.1 years ago.

  1. Priority and filed
  2. Granted
  3. Expired
  4. Today

4 claims: 3 independent, 1 dependent

  1. 1
    I claim:05 1. In the operation of an amplifier stage including a tube having a cathode cooperating with a signal grid and anode, the method of reducing the transconductance of the tube from signal grid to anode without increasing the distortion introduced into the amplified output of the tube, comprising the establishing of a positive or accelerating field between the signal grid and cathode, controlling the electron flow from said cathode to the region of the positive field and signal grid 75 A is the plate current grid bias characteristic obtained when the bias voltage Ei on the inner grid was reduced to zero, and this will be recognized as having the general form of the charac5 teristic of the usual amplifier tubes. Curves B, C and D are characteristic curves obtained when the voltage Ei on the inner grid had values of —5, — 10 and —15 'volts, respectively. /Point X on curve A is the h'orihal operating point for inaxi10 mum gain and, as is well known, the stage gain may be reduced by making the signal grid bias Es more negative, for example by shifting the operating point to one of the positions indicated by Xi, X2, X3. The stage gain fdr an impressed sig15 nal voltage E is proportional to the trarisconductance or slope of the curve at the operating point. di v 20 dEi while the distortion of the signal is proportional to d 2 ip dEJ 25 and to the higher order deriya,tiyes.. Inspection nf. curve. A shows.that the curvature at operating points, for, reduced..stage gain is substantially . greater than.the,curyature at th.e point X and it is therefore apparent that the distortion increases 30 when the bias E3 on the signal grid is adjusted to reduce the stage gain. The operating point may be shifted to another curve by adjustment of the negative bias Ei on the inner grid and, if bias E3 remains fixed, the oper35 ating point will move downward along the ordinate through point X to the curve B, C, etc. for the selected value of . the inner grid bias Ei. The series of operating points xi, xa, xa thus obtained by adjustment of Ei are located at portions of 40 curves B, C, D, respectively, which have less slope and less curvature than curve A at point X. For purposes of comparison, the points Xi, X2 and X3 were located at those regions on curve A at which the slope was the same as that of curves B, C, D at 45 points xi, xa, X3, respectively. The stage gain for small inputs will therefore be the same when operating at either of the pairs of points, Xi, xi or X2, xa, etc., but the distortion is substantially less when a fixed signal grid bias is used and the gain 50 is controlled by adjustment of the inner grid bias Ei. So long as the operating point is shifted along curve A by adjusting the signal grid bias, a decrease in transconductance is obtainable only '55 with an increase in distortion, while by shifting the operating point across the family of curves by different bias voltages Ei, the transconductance is decreased with an actual decrease in distortion, since the curvature of successive curves decreases 60 for increasing values of Ei. The control obtained is quite like that obtained with filamentary cathodes by adjustment of the heating current and is, in fact, based upon a variation of the electron stream in which the signal 65 grid is located. The positively polarized grid G2 attracts electrons from the cathode K and those electrons which are thus attracted and pass through the grid G2 are in turn drawn toward the plate P by the more positive potential of the plate. 70 But the number of electrons which can reach the region of the grid G2 is controlled by the inner grid Gi. So far as concerns the control action of the signal grid G3, the electron source is not the cathode K but is a virtual cathode which may be 75 considered as existing in the region of the grid G2.
  2. 2
    2,006,099 by a negative field adjacent said cathode, initially impressing on the signal grid such a negative bias which results in substantially maximum amplification and increasing the signal grid 5 bias in a negative sense as the negative field is increased in magnitude to reduce the stage gain. 2. An amplifier stage comprising a vacuum tube having a cathode, a positively polarized anode and three grid electrodes between said 10 cathode and anode, means impressing a negative bias on the outermost and innermost of said three grids, means polarizing the intervening grid positive with respect to said cathode, circuit connections impressing a signal voltage between the 15 outer of said grids and cathode, an output circuit between said anode and cathode, means for adjusting the negative bias on the inner negative grid, a fourth grid located between the outermost of said grids and anode, a direct current circuit 20 between said fourth grid and cathode including a resistance and a current source establishing a positive potential on said fourth grid;said resistance having a magnitude such that space current flow in said direct current circuit pro25 duces a substantial potential drop across the same when the negative potential on said inner grid is adjusted for maximum gain.
  3. 3
    An amplifier stage comprising a tube having a cathode cooperating with a signal grid and an anode to form an amplifier, an input circuit con- 5 nected betwen said signal grid and cathode, an output circuit between said anode and cathode, means for controlling the gain of the stage and comprising a pair of oppositely polarized electrodes located between said cathode and signal io grid, and means including a potentiometer located at a point remote from said tube and a contact adjustable therealong for adjusting the potential between one of said electrodes and the cathode. 15