US2654029A - Electron tube circuit - Google Patents

Description

p 1953 R. B. BUCHNER 2,654,029

' ELECTRON TUBE CIRCUIT Fil ed May 25, 1950 2 Sheets-Sheet 1 INVENTOR. li us ROBERT BERTOLD- BUCHNER P 1953 I R. B. BUCI -INER 2,654,029

ELECTRON TUBE CIRCUIT Filed May 23, 1950 2 Sheets-Sheet 2 INVENTOR.

ROBERT BERTOLD BUCHNER AGENT Patented Sept. 29, 1953 ELECTRON TUBE CIRCUIT Robert Bertold Buchner, Hilversum, Netherlands, assignor to Hartford National Bank and Trust Company, Hartford, Conn., as trustee Application May 23, 1950, Serial No. 163,615 In the Netherlands June 14, 1949 4 Claims.

This invention relates to electron-discharge tube circuit-arrangements.

In many cases, for example, in automatic telephone systems, echo-suppressor circuits, measuring circuits and control-circuits it is required to provide a device which permits the value of a direct voltage to be tested selectively to ascertain whether the tested voltage lies within or without a given voltage range, for example by the response of a relay when the voltage is between definite limiting values or non-response of the relay when the voltage exceeds the higher limiting value or is lower than the lower limiting value. It is desirable that the limiting values should be sharply defined, i. e. the output voltage or out put current of the circuit should be subject to a considerable variation, if the test voltage, upon variation, passes a limit value, while furthermore the limit value should be constant if the voltage is varied either in an increasing or in a decreasing sense.

In the copending U. S. patent application, Serial No. 107,411, filed July 29, 1949, a circuit-arrangement is suggested for comparing two voltages, in which at two definite limiting values of the voltage difierence a steep variation of the outputvoltage or current is obtained by means of feedback. In the said circuit-arrangement, the voltages to be compared are supplied to control.-

grids of two discharge tubes, the common cathode I circuit of which comprises a third tube. A control-electrode of a fourth tube is coupled, through a rectifier, to the anode circuits of the first two tubes, and the fourth tube is coupled to the third tube such that feed-back takes place. If the input voltage difference is lower than a definite threshold value, the rectifiers are cut off and the feed-back factor is zero. If the absolute value of the input voltage difference exceeds a threshold value, one of the rectifiers becomes conductive and the feed-back factor is approximately unity, so that a very small variation of one of the input voltages produces a considerable variation of the current passing through the fourth tube.

The object of the present invention is to provide a simple circuit-arrangement which comprises fewer tubes than the aforesaid arrangement. It utilizes a circuit-arrangement of a kind known per se, in which a control-voltage is supplied to a control-electrode of a first discharge tube, one output circuit of which is aperiodically coupled to a control-electrode of a second discharge tube, and one output circuit of the second tube is aperiodically coupled to an input circuit of the first tube in such manner as to obtain positive feed-back. Such a circuit-arrangement is sometimes referred to as a trigger circuit. A trigger circuit may, for example, be arranged in such manner that a control-electrode of each tube is coupled, through a battery or through a potentiometer circuit-arrangement, to a point of an output circuit, for example an anode circuit of a screen-grid circuit of the other tube. Use may also be made of a circuit, in which the cathode circuits of the tubes have a common resistance and only the control-electrode of the first tube is coupled to an output circuit of the other tube.

It is known to choose the elements of such a circuit such that the feed-back factor is substantially unity. However, these known circuits have only one limiting value.

According to the invention, a circuit-arrangement in which a control voltage is supplied to a control electrode of a first discharge tube of which an output circuit is coupled aperiodically to a control-electrode of a second discharge tube and an output circuit of the second tube is coupled aperiodically to an input circuit of the first discharge tube such that positive feed-back occurs, is characterized in that the coupling circuit between the output circuit of the first tube and the control-electrode of the second tube comprises a parallel-connection of two branches, each of. which comprises a rectifier, the rectifiers being conductive in opposite senses and having different biassing voltages such that the first rectifier is conductive when the control-voltage exceeds a definite first limiting value and the second rectifier is conductive when the controlvoltage is lower than a definite second limiting value which is lower than the first limiting value, the feed-back factorbeing substantially unity, if one of the rectifiers and the two tubes are conductive.

The feed-back factor is zero or at least very low when the two rectifiers are cut off, i. e. if the voltage to be tested has a value between the two limiting values.

In one embodiment of the circuitarrangement, a potentiometer is connected between two points of constant potential and the series-connection of the two rectifiers is connected between two points of the said potentiometer, the junction point of the rectifiers being connected to a point of the output circuit of the first discharge tube and the control-electrode of the second tube being connected to a further point of the potentiometer.

In a further embodiment, a potentiometer,

part of which is shunted by the series-connection of the rectifiers is connected between a point of the output circuit of the first discharge tube and a point of constant potential. The junction point of the rectifiers is connected to the control-electrode of the second tube, and the control-electrode is furthermore connected, through at least one resistance, to a point of constant potential.

The output voltage is preferably taken from a. point coupled to a point of an output circuit of each of the tubes through a rectifier, the rectifiers being so arranged that said point invariably follows either the higher or the lower potential of the points of the output circuits of the tubes.

In order that the invention may be more clearly understood and readily carried into effect, it will now be described more fully with reference to the accompanying diagrammatic drawings, given by way of example, in which:

Figs. 1, 3, 4 and 5 each show an embodiment of the circuit-arrangement according to the invention, and

Figs. 2a and 2b are diagrams by means of which the operation of the circuit-arrangements will be explained.

In the circuit-arrangement shown in- Fig. 1, a voltage V to be tested. is supplied by way of a terminal to the control-grid of a tube B1. The cathode circuits of the tube-B1 and a tube B2 comprises a common resistance R1. The anodes of these tubes are fed through. resistances R2 and R3, respectively, from a voltage source-V2.

The control-grid of tube B2 is connected, through the series-combination of a rectifier g2 and a battery Ba, to a point 2 of the anode circuit of tube B1. A rectifier g1 is connected between point 2 and a tapping on battery Ba. The control-grid of B2 is furthermore connected through a resistance R4 to a point I of a potentiometer RR6R7 connected between the voltage sources V1 and V2.

The control-grid of an auxiliary tube B3 is coupled throu h a leakage resistance R18 and rectifiers g3 and g4 to the anodes of tubes B1 and B2. Leakage resistances R18 prevent the controlgrid of tube B3 from assuming ahigh positive potential relative to its cathode. The rectifiers are arranged such that the control-grid assumes the higher of the potentials of the point 2 and a point 3 of the anode circuit of tube B2. presence of the leakage resistance Rs between point 4, intermediate the rectifiers 93 and 94. and the voltage source V1, at least one of the rectifiers is conductive. The cathode of tube B3 is connected to a point 8 of the potentiometer R5R6R'l. The resistances R5, Rs and R1 are chosen such that the potentials of points I and 8 are only slightly affected by the emission-current of tube B3. The anode circuit of Ba includes the winding of a test relay TR.

This circuit-arrangement operates as follows. Tube B1 is cut off if a comparatively low test voltage V0 is supplied to its control-grid, the anode volta e at point 2 then being equal to V2. The potential of point I is lower than the potential V2 less the voltage of battery Ba. The rectifier g2 is then conductive, so that the control-grid of tube B2 has a comparatively high potential and tube B2 is conductive. Consequently, the potential of the control-grid of tube B3 has a comparatively high value, so that relay TR is energized.

If the potential of the control-grid of tube B1 is caused to increase, tube B1 becomes conductive at a definite limiting voltage V 1, the voltage of point 2 drops and consequently also the potential Owing to the of the control-grid of tube B2 drops. Since the potential of the control-grid of tube B2 varies in an absolute sense more than the potential of point I, the current flowing through tube 132 decreases more than the current passing through tube B1 increases, so that the voltage drop across the cathode resistance R1 decreases.

The voltage across resistance R1 is operative in the grid circuit of tube B1 and in such sense that the variation of the control-grid potential of tube B1 is supported, so that a feed-back effect is obtained. The variation of the anode currents of tubes B1 and B2 is shown in Figs. 2a by the curves iar and id: as functions of the input voltage V0.

Fig. 2b shows the variation of the anode voltages Val and V32 as functions of the input voltage V0. By a suitable choice of the circuit elements, the feed-back factor is unity so that an extremely small variation of the input voltage V0 at the threshold value Vgl produces a considerable variation. of the current in passing through tube B1.

The current passing through tube I31v increases rapidly until the potential of point 2, less the voltage of battery Be, is equal to the potential of point- 1'. Owing to the potential drop of point 4, the tube B3 is. cut off and the relay TR is deenergized.

The process is completely reversible, if the feedback factor is equal to or smaller than unity, i. e., in this case, each value of the voltage V0 is associated with only one value of 111 or iaz. However, if the feed-back factor exceeds unity, the currents vary with an increase of V0 according to the fulllinecurve 1'01 and ice and, with a decrease of V0, according to the broken-line curve ia i and ia z. In this event, consequently, the threshold value is not constant.

With a further increase of voltage V0, rectficr g: is cut off. The control-grid of tube B; is 1-. longer coupled to the anode of tube B1 and as sumes the constant potential of point I. The current izn subsequently increases comparatively slowly. Owing to the increase in voltage drop across resistance R1, the effective voltage between the grid and the cathode of tube B2, and consequently also the. current iaz decreases. If the resistance R1 has a high value, the slope of the variation of im as a function of V o is, in this interval, approximately equal to half the mutual conductance of each of the tubes B1 and B2.

As soon as voltage V0 has increased to the value V52, at which the potential of point 1e.- the voltage between the taping a and the n" terminal of the battery, is equal to the potenti of point I, rectifier g1 becomes conductive and the feed-back factor is again unity. With a very small increase of voltage V0 the action is similar to that at the limiting value Vgl and the voltage at the control-grid or tube B2 drops to such an extent that tube B2 is cut off and the anode current of tube Bl. increases considerably.

The control-grid of tube B3 follows the poten tial of point 3 and the potential increases very rapidly. Tube B3 again becomes conductive and relay TR is energized. The current ial increases very slowly, owing to the high resistance R1 in the cathode circuit of tube B1. The value of resistance R1 is preferably high so that the controlgrid of tube B1 does not carry grid-current at the highest voltage V0 to be tested and the input resistance of the circuit is substantially infinitely high.

The difference between the limiting values Vgl and Vgz i. e. the limit width of the arrangement may be varied by means of the tapping a of battery B8" In the arrangement described, the relay TB is only energized, if voltage V0 is lower than V111 or exceeds V 2, and the relay is not energized, if V0 lies between the limiting values. The limiting values are very sharply defined. It is obvious that if the rectifiers g3 and g4 are connected in opposite senses and the leakage resistance Re is connected to voltage source V2 instead of to voltage source V1, point will follow the lower of the potentials of points 2 and 3. In this variant, the tube B3 is conductive and relay TR. energized only, if V0 lies in the range between the limiting values V 1 and V 2.

The use of the battery Be. as a coupling element involves various practical disadvantages. The battery has a fluctuating potential and every test circuit requires a separate battery. These disadvantages are avoided in the circuits shown in Figs. 3, 4 and 5.

The circuit shown in Fig. 3 resembles that of Fig. 1 and corresponding elements bear the same references. However, the manner in which the control-grid of tube B2 is coupled to the anode circuit of tube B1 is different.

The control-grid of tube B2 is connected to a point II of a potentiometer R9, R10, R11, R12 connected between voltage sources V1 and V2. The resistance R10 is shunted by the series-connection of rectifiers g1 and g2 and the anode of tube B1 is connected to the junction point of the rectifiers.

Rectifier 92 is conductive when tube B1 is cut off, hence when voltage V0 has a comparatively low value. Upon an increase of voltage V0 to the alue V 1, B1 becomes conductive and the potential of the point 2 and a point 9 of the potentiometer drops, so that the potential of the controlgrid of tube B2 also decreases. The feed-back factor is now substantially unity and the anode current m1 varies extremely steeply as a function of voltage V0, similarly as in the circuit shown in Fig. 1, until the potential of point 2 has decreased to such an extent that rectifier 12 is cut off. Rectifiers g1 and g2 are thus both out off and the control-grid of tube B2 assumes a constant potential which is determined by the ratio in which potentiometer R9, R10, R11 and R12 is divided by the point I I. The anode currents i111 and iaz then vary comparatively slowly. Upon 1 an increase of voltage V0 to the value V 2 the potential of point 2 has decreased to a value equal to the potential of point I 0, provided the rectifiers g1 and g2 are both out off. Upon a further increase of voltage V0, rectifier g1 becomes conductive, due to which the potential of point It follows that of point 2.

The feed-back factor is now again substantially unity. If rectifier 91 is conductive, the feed-back factor is naturally not exactly equal to that when rectifier g2 is conductive. If, however, the value of resistance R10 is low with respect to the sum of resistances R11, R12 the difierence is practically negligible.

In the device shown in Fig. 4, use is made of a trigger circuit in which the control-electrode of each of the tubes B1 and B2 are coupled to an output circuit of the other tube.

The screen-grid of tube B1 is connected to a tapping l3 of a potentiometer R15R1s connected between the anode of tube B1 and the voltage source V1.

Between the anode of tube B1 and the source V1 is connected a potentiometer Rl'7Rl8Rl9, of which resistance R18 is shunted by the seriesconnection of rectifiers g1 and g2. The controlgrid of tube B2 is connected to the junction point 6 of these rectifiers and is furthermore connected through resistance R4 to point 1 of the potentiometer RsR'l connected between the sources V1 and V2. The cathode leads of the tubes B1 and B2 comprise resistances R23 and R24, respectively, which may sometimes be dispensed with. The anodes are fed through resistances R2 and R3, respectively. The test voltage V0 is supplied to the control-grid of tube B1. Similarly to the circuits shown in Figs. 1 and 3, the output voltage is taken from point 4 which is coupled, through rectifiers 9'3 and 94, to the anodes of tubes B1 and B2.

The control-grid of the auxiliary tube Be, the anode circuit of which comprises the relay TR, is connected to point I 6 of a potentiometer R2oR21 connected between point 4 and source V1.

The cathode lead of tube B3 comprises a resistance R25. At a comparatively high value of potential V0, tube B1 is cut off and points 2 and 4 have a potential substantially equal to source V2. Tube B3 is then conducting, relay TR is energized, and point l5 has a potential which exceeds the constant potential of point I.

In this case, the rectifier g2 is conductive and the control-grid of tube B2 has a potential at which the tube is conductive. The potential of the anode of tube B2 and consequently of the screen-grid of tube B1 is comparatively high and the rectifier 94 is cut off. If the voltage V0 is caused to increase, tube B1 becomes conductive at a definite limiting voltage V 1. Due to this, the potential of the control-grid of tube B2 decreases, so that the potentials of the anode of tube B2 and of the screen-grid of tube B1 increase. The increase of the voltage V0 is thus supported by the increase in screen-grid potential of tube B1. The elements are such that the feed-back factor is practically unity, so that in the conductive state of the two tubes B1 and B2 and of the rectifier g1 or 92, a very small variation of voltage V0 produces a great variation of the emission current of tube B1.

Owing to the sharp drop of potential of point 2, tube B3 is cut off and relay TR is de-energized.

Upon a further extremely small increase of V0, the voltage at point l5 drops below the potential of point 1 and the rectifier 92 becomes conductive. In the next following voltage range of voltage V0, the control-grid of tube B2 assumes the constant value of point 7. Consequently, the current flowing through the tube B2 remains constant, as does the screen-grid potential of tube B1.

The emission-current of tube B1 slowly increases with an increase of voltage V0, the slope being primarily determined by resistance R23 in the cathode lead. If voltage V0 has increased to the value V81, the potential of point H has dropped to the voltage of point 1 and rectifier 1 becomes conductive.

Upon a further increase of voltage V0, the potential of point 6 drops below the potential of point 1, so that the screen-grid potential of tube B1 increases. The feed-back factor is now again unity and the anode voltage of tube B2 increases steeply with an increase of voltage V0, so that, since rectifier 94 is now conductive and rectifier g3 is cut off, tube B3 becomes conductive and relay TR is energized.

Consequently, relay TR only becomes de-energized if the test voltage V0 has a value between the limiting values V 1 and Vg2. The voltage range may be varied by varying the resistance 7 R18- It is desirable that the value of this resist anceshould be low with respect to that ;of.'re. sistance R19, in order to ensure that. the .feedback factor has the same value, i. e. .unity at the limiting values Vg1 and V 2.

The circuit may be varied in several ways. Thus, for instance, the method of coupling the control-grid of tube B2 and the output circuit of tube B1, as shown in Fig. 4, may also be used for the trigger circuit shown in Fig. 3, in which, consequently, the coupling between the output current of tube B2 and the input control-circuit of tube B1 is established by the common resistance R1 in the cathode leads. Conversely, the method of coupling the control-grid of tube B2 and the anode circuit of tube B1 shown in Fig. 3 may be used for the trigger circuit shown in Fig. 4.

The output voltage of point 4 need not be used to control a relay, but may alternatively be supplied. to a suitable indicator, for'example a Braun tube. Furthermore, a test relay may be connected between output circuits of tubes B1 and B2 and the auxiliary tube B3 omitted. Such a circuit is shown in Fig. 5, in which the trigger circuit corresponds to that shown in Fig. 3.

However, instead of the anode, the screen-grid of tube B1 is connected to the common point of rectifiers g1 and. 92. A rectifying bridge built up of four rectifiers g5, g6, g7 and g8 is connected between points 2 and 3. The output diagonal of this bridge comprises the test relay TR between points [8 and I9. This circuit operates similarly to that shown in Fig. 3.

At a low potential V0, the tube B1 is cut off, tube B2 is conductive and relay TR is energized. If voltage V increases and exceeds the limiting value Vgl, tube B1 becomes conductive and the current through tube B2 decreases. In the voltage range between the values Vgl and vgll, the anode currents of tubes B1 and B2 differ comparatively slightly, so that relay TR is de-energized. If the voltage V0 increases and exceeds the value Vg2, the tube B2 is cut off and relay TR is energized.

Similarly to the circuits shown in Figs. 1, 3 and 4, the process is reversible if the feed-back factor is equal to or smaller than unity.

The rectifier-bridge g to g8 serves to prevent magnetic reversal of the relay TR and the relay TR from becoming temporarily de-energized if, in testing difierent voltages, voltages lying on different sides of the threshold range are successively supplied to the input terminal I.

It will be obvious that the circuits described can be used not only for testing voltages but also with advantage for other purposes, for ex 8 ample, for-deriving. pulses with constant amplitudes from an alternating voltage.

What I claimis: 1

l. A circuit-arrangement in which a controlvoltage is supplied to a control-e ectrode of a first discharge tube having an output circuit coupled aperiodically to a control-electrode of a second discharge tube an output circuit or" the second tube being coupled aperiodic-ally to an input circuit of the first tube such that positive feedback occurs, the coupling circuit between the output circuit of the first tube and the control-electrode of the second tube comprising pant-tile combination of two branches, each of which comprises a rectifier, the rectifiers being conductive in opposite senses and having diil ent biassing voltages such that the first rectifier is conductive when the control-voltage exceeds a definite first limiting value and the second rectifier is conductive when the control-voltage ower than a definite second limiting value love '1 the first limiting' value, the feed-back factor bcin': substantially unity if one of the rectifiers and both tubes are conductive.

2. A circuit-arrangementas claimed in claim 1. characterized in that a voltage divid r is connected between a point of the output circuit or" the first discharge tube and a point of constant potential, part of which voltage divider is shunted by the series connection of two rectifiers, and the junction point of the rectifiers is connected to the control-electrode of the second tube, this control-electrode furthermore being connected, through at least one resistance, to a point of constant potential. v

3. A circuit-arrangement, as set forth in claim 1, wherein said parallel combination of two branches comprises a voltage divider connected between two points of potential, the rectifier of one branch being connected between a first tap on said divider and the output circuit of said first tube, the rectifier of the other branch being connected in opposing polarity relative to the first rectifier between a second tap on said divider and the output circuit of said first tube, the control electrode of said second tube being connected to a third tap on said divider.

4. A circuit-arrangement, as set forth in claim 1, further including a pair of rectifying elements connected in series opposition between a point in the output circuit of the first tube and a corresponding point in the output circuit of the second tube, and means connected to the junction of said elements to derive a control voltage therefrom.

ROBERT BERTOLD BUCI-INER.

No references cited.

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