US2501620A

US2501620A - Wave generating circuits

Info

Publication number: US2501620A
Application number: US484324A
Authority: US
Inventors: Albert M Skellett
Original assignee: Bell Telephone Laboratories Inc
Current assignee: AT&T Corp
Priority date: 1943-04-24
Filing date: 1943-04-24
Publication date: 1950-03-21
Anticipated expiration: 1967-03-21

Description

March 21, 1950 A. M. SKELLETT 2,501,620

WAVE GENERATING CIRCUITS Filed April 24, 1943 4 H 2 Sheets-Sheet 1 H6 W 6 W Mi: k 2 W w l OUTPUT a ISWOUTPUT /NVENTOR AM. SKELLETT A T TORNEV March 21, 195p A. M. SKELLETT 2,501,620

, WAVE GENERATING CiRCUITS Filed April 24, 1943 2 Sheejzs-Sheet 2 GRID POTENTIAL VA R/A T/ON FIG. 8

PLA TE POTENTIAL VAR/A T/ON GRID P0 TEN TIAL F/ 9 I VAR/AT/ON PLA TE P0 751v TIAL m R/A r/o/v v POTENTIAL VARIATION FIG. /0 0F PLATE OF was INVENTOR By A. M. SKELLETT Maw A T TO/FIVE) Patented Mar. 21, 1950 WAVE GENERATING omoorrs Albert M. Skellett, Madison, N. J., assignor to Bell Telephone Laboratories, Incorporated, New

.York, N. Y., a corporation of New York Application April 24, 1943, Serial No. 484,324

3 Claims.

The invention relates to wave generation and particularly to alternating wave generating circuits of the multivibrator type.

The so-called multivibrator is an arrangement of electric space discharge tubes operating as a distorted wave oscillator to produce a discontinuous wave the frequency of which may be adjusted to have any value within Wide limits. In its original form as devised by H. Abraham and E. Bloch and described in an article by them in the Annalen de Physique, volume12, page 237, 1919, it comprises a two-stage resistance-capacity coupled vacuum tube amplifier in which the anode of each tube is capacitively coupled to the control grid of the other tube. The period of oscillation of such a circuit is primarily determined by the time constant of the combination of coupling condenser and the grid resistor through which it discharges in the course of half a cycle.

An object of the invention is to provide the multivibrator type of operation in a wave generating circuit without the use of capacitance for timing control.

Another object is to generate alternating current waves of any desired stable frequency at a high voltage.

Another object is to generate alternating pulses of various wave forms.

These objects are obtained in accordance with the invention by the use of combinations of inductance and resistance to perform the functions of the condenser-resistance arrangements in the usual multivibrator circuit as well as to obtain other useful characteristics not ordinarily obtainable with such a circuit. In one embodiment, the modified multivibrator circuit may comprise a pair of multielectrode electron discharge tubes connected in a symmetrical or unsymmetrical circuit arrangement with highly resistive impedance coupling between the plate of one or both tubes and the control grid of the other tube, and an inductance coil in the control grid or plate circuit of one or both tubes; the time constant of the inductance coils and the resistive impedances with which they work primarily determining the period of oscillation of the multivibrator circuit.

The various objects and features of the invention will be better understood from the following detailed description when read in conjunction with the accompanying drawing in which:

Figs. 1 to 7 show schematically wave generating circuits embodying difierent modifications of the invention; and

Fig. 8 to 10 show curves illustrating typical Wave forms for the control grid and anode poten tials of the tubes in the circuits of Figs. 1 to 3 obtained by actual tests of those circuits.

The symmetrical multivibrator circuit of Fig. 1 includes the two three-electrode amplifying vacuum tubes I and 2. The anode or plate of tube I is connected directly to the control grid of tube 8 through the highly resistive impedance (resistor) 3, and the anode or plate of tube 2 is connected directly to the control grid of tube I through an equivalent highly resistive impedance (resistor) 4. The cathodes of the tubes I and 2 may be heated to incandescence from any suitable source (not shown) which ma be a direct current battery. The control grid-cathode circuit of tube I comprises the cathode resistor 5 and the inductance coil 6 in series, and the control grid-cathode circuit of the tube 2 comprises the same cathode resistor 5 and another inductance coil I, equivalent to the coil 6, in series. Space current is supplied from the common plate battery 8 in parallel to the plates of tubes I and 2 through the individual equivalent series resistors 9 and II), respectively.

Let it be assumed that the plate battery 8 and cathode battery sources of the tubes I and 2 have been connected as described so that the circuit is oscillating, and that the discharge has just been transferred from tube 2 to tube I. The potential of the plate of tub I will then be negative with respect to the supply voltage from battery 8, and the control grid of tube I will be at or near zeropotential with respect to the cathode of that tube. The control grid potential of the other tube 2 will then be more negative than the cut-01f value and the current will be building up in the inductance 1 in the control gridcathode circuit of the tube 2 thus gradually bringing up the potential of the grid of that tube toward the cut-off value. The potential of the plate of tube 2 will be the same as the supply voltage from battery 8.

As the current in inductance coil I increases, the potential across it decreases until the potential of the control grid of tube 2 is brought up to cut-off and current starts to flow through that tube. This will cause the potential of the plate of tube 2 to drop, and this potential drop Will be transmitted through the coupling resistor t to the control grid of tube I. Since this happens suddenly, the inductance coil 6 in the control grid cathode circuit of tube I acts as a very high impedance, much higher than that of the coupling resistor 4, so that most of the voltage drop is impressed on the control grid of tube I. Tube I amplifies this voltage change and its plate po- The upper and lower curves of Fig. 8 respectively show the wave form (variation of amplitude with time) of the grid and plate potentials for one of the tubes of the circuit of Fig. l. The period of oscillation of the multivibrator circuit is determined approximately by the time constant of the coils 6, I and the resistances t, 3 they work with. That is, the period in R Where L is the inductance of a coil and R is the resistance of a coupling resistor.

The constant frequency wave generated by the circuit of Fig. 1 may be taken ofi at any point, for example, through a resistance-capacity coupling from one plate circuit, as shown.

Fig. 2 shows a modified symmetrical multivibrator circuit in accordance with the invention difiering essentially from that of Fig. 1 merely in that the inductance coils t and l are connected in push-pull relation with respect to each other, respectively, in series with the individual portions of the plate-cathode circuits of tubes l and 2 in place of the resistors 9 and it, instead of in series with the control grid-cathode circuits of; those tubes as in Fig. 1; the equivalent resistors 2B and 2i are connected in the control grid-cathode circuitsv of tubes i and 2, respectively, in series with the common cathode resistor 5.; and the generated wave is taken off through another coil H, symmetrically inductively coupled to the coils 6 and i. As shown by the curves of Fig. 9, in the circuit of Fig. 2 the grid potentials are of square wave form and the plate potentials swing over a rather large voltage range, greater than the supply voltage.

Fig. 3 shows an unsymmetrical multivibrator arrangement in accordance with the invention difiering from the circuit of Fig. 2 in the following particulars: The connection between the plate of tube. 2 and the grid of tube i through resistor 4 is eliminated, the connection between the plate of tube 8 and the grid of tube 2. through series resistor 3. being retained. The inductance coil 6 is connected in series with the individual portion of the plate-cathode circuit of tube I as in Fig. 2, but the series coil in the individual portion of the plate-cathode circuit of tube 2 is eliminated. A potentiometer 22 having its resistance element connected between the grid resistor 20 and the positive terminal of battery 8 and its variable arm connected to the grid of tube I, i provided for obtaining in conjunction with battery 8 and cathode resistor a negative grid bias of suitable value in tube i. The circuit is driven by an alternating control wave, for example, a wave comprising a series of sharp pulses recurring at regular intervals so as to provide trigger operation, applied to the control grid-cathode circuit of tube l through the resistance-capacity coupling I2; and the generated wave output of the multivibrator is taken off through a coil I3 inductively coupled to the coil 6.

In the circuit of Fig. 3, the tube 2 is normally 4 conducting and the tube I is normally cut-ofi (non-conducting) by the resultant negative bias applied to its grid from battery 8 through the discharge path of tube 2 with that tube conducting, cathode resistor 5 and potentiometer 22 with proper adjustment of its variable arm. The circuit is triggered off by the application of each control pulse to the control grid-cathode circuit of tube I. The trigger input suddenly raises the potential of the control grid of tube I so that the tube starts to conduct immediately. This action is so sudden that the plate impedance of tube 1 at this time is very high, and the plate potential starts to drop, causing the potential of the control grid of tube 2 to be pushed down through the coupling resistor 3. This lowers the current fiow through tube 2 and hence the current through the common cathode resistor 5 dropping the cathode potential of that tube.

This action efiectively decreases the grid bias on tube I and hastens the transfer of the discharge from tube 2 to tube I through this regenerative action. In this case, the cathode resistor 5 acts to provide positive feedback.

This action continues at a very fast rate until the discharge has transferred to tube I. The current continues to build up in the coil 6 in the plate-cathode circuit of tube l, raising the plate potential of tube I and thus the potential on the grid of tube 2 through the coupling resistor 3. When the potential of the grid of tube 2 is built up through this action to the cutoff value, tube 2 starts to conduct. This increases the current flow through the common cathode resistor 5 increasing the bias on tube l, and through the same action as described above, but in the opposite sense, the discharge quickly transfers to the grid of tube 2 to remain there until the next trigger pulse comes along.

The duration of the pulse thus generated in the coil 6 is determined approximately by the time constant of that coil 6 in series with the tube resistance. When the discharge transfers to tube 2, a very high potential is generated in the coil, as indicated by the curve of Fig. 10. In order to generate a high voltage output wave by this means, the coil 6 may be used as the primary winding of a step-up transformer, and the coil I3 in the outputcircuit, inductively coupled to coil 5 as the secondary winding of that transformer. By the use of a small double triode for tubes I and 2, sparks of several thousand volts have been obtained with the circuit of Fig. 3. If the bias on the control grid of tube l is increased, this circuit, like those of Figs. 1 and 2, will oscillate by itself when the batteries are connected to the tubes.

The coil 5 in the circuit of Fig. 3 may be the operating Winding of an electromagnetic relay, in which case the relay will remain operated for a definite time, no matter what the duration of the trigger pulse, provided, of course, that it is less than the duration of the generated pulse. Thus the circuit may operate as a hold-up circuit. Another use might be that of pulse preshaping in telegraphy, etc.

Fig. 4 shows another unsymmetrical multivibrator circuit embodying the invention, differing essentially from that of Fig. 3 in that the re-. sistor 9 is substituted for the inductance coil t in series with the plate-cathode circuit of tube I and an inductance coil 1 is connected in place of the series resistor 2| (shown in Fig. 3) between the control grid of tube 2 and a variable contact on the common cathode resistor 5. This multivibrator circuit is triggered of! by pulses applied by the saturable magnetic core input transformer ll to the control grid-cathode circuit of tube I, and the generated wave is supplied to an output circuit through coil l inductively coupled to coil 1.

The operation of the circuit of Fig. 4 is similar to that of the circuit of Fig. 3 described above. The cathode resistor 5 again provides positive feedback, and the duration of the square pulse generated by the multivibrator is determined by the resistances which are effectively in series with the coil 1 when the current is building up through it (and the voltage across it is decreasing). Like the circuits of the other figures, the circuit of Fig. 4 will self-oscillate providing the biases applied to the grids of both tubes are sufficient to make them both conducting at once under which condition the circuit set-up is unstable and acts like a two-stage amplifier with positive feedback.

The unsymmetrical multivibrator circuit of Fig. 5 differs essentially from that of Fig. 3 in that the coupling from the plate of tube I to the control grid of tube 2 is obtained by a coil l6 coupled to the coil 6 in the plate-cathode circuit of tube I, that is, by a transformer formed by these two coils instead of by the resistor 3. As in the circuit of Fig. 3, the trigger pulse is applied to the control grid-cathode circuit of tube I through a resistance-capacity coupling l2, and the output is taken ofi from the plate circuit through another resistance capacity coupling 23 instead of through a coil inductively coupled to the coil 6. The operation of the circuit of Fig. 5 will be obvious from that described for the similar circuits of Figs. 3 and 4.

Figs. 6 and '7 show modifications of the multivibrator circuits of Figs. 1 and 2 respectively, which will be efiective to make the outputs of these circuits closely approximate sine waves. Fig. 6 differs from the circuit of Fig. 1 merely in the addition of the condensers l1 and I8 connected across the resistances 9 and I0, respectively, in series with the plate-cathode circuits of tubes l and 2, and Fig. 7 differs from Fig. 2 merely in the addition of the condenser l9 connected across the plate circuit inductance coils 6 and I in series. The function of the added elements is to smooth out the abrupt transitions from one tube to the other and thus to enable sine wave outputs to be produced. The arrangement of Fig. 7 particularly should produce a very good sine wave.

It is obvious that the principles of the invention are applicable to multivibrator circuits employing any even number of tubes, or electron discharge tubes having more than three electrodes, as well as to multivibrator frequency stepup and step-down circuits, in which case the control oscillation injected into the grid or plate circuit would be of a frequency which is a submultiple or a harmonic of the multivibrator frequency, respectively.

Other modifications of the circuits illustrated and described which are Within the spirit and scope of the invention will occur to persons skilled in the art.

What is claimed is: I

1. A wave generator of the multivibrator type comprising a pair of electron discharge devices each having a heated cathode, an anode and a control grid, circuits respectively interconnecting the anode and cathode of each device having a common portion including a source of space current and other portions individual to the respective devices, other circuits respectively inincluding resistance only, an electrical coupling between the anode of each device and the control grid of the other device, at least one of said couplings being purely resistive, inductance in series in at least one of the individual portions of said anode-cathode interconnecting circuits, the period of oscillation of said generator being determined primarily by the time constant of said inductance and the circuit resistance effectively in series therewith and an output circuit coupled to at least one of the individual portions of the said anode-cathode interconnecting circuits for taking off the generated wave.

2. An unsymmetrical multivibrator comprising two electron discharge tubes each having a heated cathode, an anode and a control grid, control grid-cathode circuits for said tubes, anode-cathode circuits-for said tubes, including a common source of space current, an inductance in series with the anode-cathode circuit of one of said tubes, a coupling between the anode-cathode circuit of each tube and the control grid-cathode circuit of the other tube, at least one of the couplings being highly resistive, means for biasing the control grids of said tubes so that one tube is normally conducting and the other normally non-conducting, means to apply an alternating control wave to the control grid-cathode circuit of the normally non-conducting tube to start the multivibrator into oscillation with first one tube and then the other tube conducting alternately, the period of oscillation being determined primarily by the time constant of said inductance and the resistances effectively in series therewith, and means to take off the generated oscillations from one of said circuits.

3. An unsymmetrical multivibrator comprising two electron discharge tubes each having a heated cathode, an anode and a control grid, control grid-cathode circuits for said tubes, anode-cath- Ode circuits for said tubes including a common source of space current, an inductance coil connected in series with the anode-cathode circuit of one tube, a coupling between the anode-cathode circuit of each tube and the control gridcathode circuit of the other tube, one of the couplings being obtained by coupling said inductance coil in the anode-cathode circuit of said one tube inductively to the control grid-cathode circuit of the other tube, the other of said couplings being highly resistive, means for biasing the grids of said tubes so that one tube is normally conducting and the other normally non-conducting, means to apply an alternating control Wave to the control grid-cathode circuit of the normally non-conducting tube to start the multivibrator into oscillation, the period of oscillation being determined primarily by the time constant of said inductance coil and the resistances effectively in series therewith, and means to take oil the generated oscillations from one of said circuits.

ALBERT M. SKELLETT.

REFERENCES CITED The following references are of record in the file of this patent:

UNITED STATES PATENTS Number Name Date 1,587,520 Hartley June 8, 1926 1,698,290 Alexanderson Jan. 8, 1929 (Other references on following page) 7 8 UNITED STATES PATENTS FOREIGN PATENTS 1 Number Country Date 'fiiggg g gff i g g 355,705 Great'Br'ita' in Aug.24,1931 adogallw Vance Sept 14 1937 5 356,111 Great Bntam Aug. 24, 1931 2,159,493 Wright May 23, 1939 OTHER REFERENCES Proceedings of the Cambridge Philosophical $254181 F d fi A 1 Society, vol. '33, 1933, pages "549-558, ASca1e-of- 2659 an e "Two" High-Speed Counter Using Hard Vacuum 96 Blumlem 1941 10 Triodes, by W. B. Lewis. (Copy :in Patent Office -v2,41-'1,-522 Shenk Mar. 18, 1947 Library)