US2777992A

US2777992A - Reactance tube circuit

Info

Publication number: US2777992A
Application number: US342627A
Authority: US
Inventors: Anderson Eldon
Original assignee: Collins Radio Co
Current assignee: Collins Radio Co
Priority date: 1953-03-16
Filing date: 1953-03-16
Publication date: 1957-01-15
Anticipated expiration: 1974-01-15

Description

REAQTANCE TUBE CIRCUIT Filed March 16, 1953 10 400/0 4 Ivar Still 17' 0/? JNVENTOR. 200 All/0:12:00

United rates Patent REACTANCE TUBE CIRCUIT Eldon Anderson, Cedar Rapids, Iowa, assignor to Collins Radio Company, Cedar Rapids, Iowa, in corporation of Iowa Application March 16, 1953, Serial No. 342,627

6 Claims. (Cl. 332-24) This invention relates in general to reactance tube circuits and in particular to reactance tube circuits which have a resonant phase shifting grid circuit.

A reactance tube circuit is similar to a capacitance or inductance. An alternating voltage placed across such a circuit will produce a quadrature current in the same manner as a voltage across a capacitance or inductance.

The reactance tube circuit, however, has an additional property in that its reactance can be made proportional to an audio voltage. It is analogous to a capacitor or inductor whose reactance varies in proportion to an audio voltage which then produces a quadrature current that varies in proportion to the audio voltage.

Two reactance tubes which produce opposite and equal quadrature currents may be connected with their plates in parallel, and their unmodulated equal plate currents will cancel each other. If the plate current of each tube is then modulated by an audio voltage which is opposite in phase on each tube, the plate current of one tube will alternately increase while the plate current of the other tube is alternately decreasing, etc. The net plate reactive current from both tubes will no longer completely cancel and their difference will be proportional to the audio voltage. The net current will lag when the audio voltage increases and lead when the audio voltage decreases or vice versa depending on which way the audio voltage is connected.

The conventional reactance tube circuit uses a resistance-capacitance phase shifting grid circuit such as shown in Termans Radio Engineering, 3rd edition, at page 493. The ninety degree phase shift betweenplate current and plate voltage is obtained in its phase shifting circuit byrnaking the resistance very large compared to the reactance so that the current through that circuit will .be substantially in phase with the plate voltage across it. Then the voltage across the reactance has a ninety degree phase relationship with the current throughit and will be substantially ninety de rees out of phase with the plate voltage. The reactive voltage is then placed across the reactive tubes control grid to produce plate current which has substantially ninety degrees phase relationship with the plate voltage. A difiiculty with the conventional circuit is that the very high resistance required in the'phase splitter circuit to obtain the ninety degree phase shift allows only a relatively small voltage across the reactive element to drive the tube control grid, and therefore only a relatively small reactive current can be obtained from such tube when compared with its rated current. it is therefore the principal object of this invention to provide a reactance tube circuit which will provide as largea grid driving voltage as necessary to obtain as large a quadrature plate current as desired.

It is anotherobject of this invention to provide areactance tubecircuit which will provide a large reactive -.current swing with a very small audio modulating signal voltage.

It is still another object of this invention to provide a reactance tube circuit which can producelarge modu- 2,777,992 Patented Jan. 15, 1957 "ice lated reactive currents when operated at a low plate voltage which will therefore allow the modulated oscillator to operate at a low voltage level.

It is another object of this invention to provide a reactance tube modulator which can obtain a large frequency deviation proportional to a small audio signal while its oscillator is operated at a low power level.

This invention obtains a large grid voltage which is ninety degrees out of phase with the plate voltage by providing a series resonant phase shifting circuit across,

the plate voltage and by taking the grid voltage across a reactive element.

Other features and advantages not specifically en11merated will become apparent after considering the following Figure 5 indicates the phase relationship between the net output current and the plate voltage.

Now considering the invention in more detail, a circuit for one embodiment is schematically shown in Figure l which shows an oscillator 1th that is connected at point 14 to a pair of

plates

12 and 13 of a pair of tubes V and V2, respectively, through a direct current blocking condenser ll. The cathode 17 of tube V; is connected to the cathode 19 of tube V2 and both cathodes are connected to ground through a biasing resistor RB which is in parallel with a bypass condenser CB.

Tube Vi has a phase shifting circuit 15 which consists of a resistor R1, a capacitor C1 and an inductance L1 in series. Resistor R1 is connected to point 14 through a blocking condenser Z'S and the opposite end of inductance L1 is grounded through another blocking condenser Likewise, the tube V2 has a phase shifting circuit 'Zt'l which consists of a resistor R2, an inductance L2, and a capacitor C all in series, with resistor R2 connected to point 14 through blocking condenser 28 and the opposite end of capacitor C2 grounded. Tube V1 has a control grid 16 which is connected to the side opposite ground of inductance L1, and tube V2 has a control grid 18 which is connected to the ungrounded side of capacitor C2. A 5 plus power supply is connected to the plates of tubes; V1 and V2 through a choke coil 25 A grid leak resistor 31 is connected between grid 16 and ground, and a grid leak resistor 32. is connected between grid 13 and ground.

An audio signal input voltage is impressed on a primary 22 of an audio transformer 21 which has a secondary 23 with a grounded center tap 24. A suppressor grid 26 of tube V1 is connected to one end of secondary 23, and a suppressor grid 27 of tube V2 is connected to the other end of secondary 23.

In operation, an alternating current oscillator voltage E will exist across the plates of tube V1, tube V2, and phase shifting circuits l5 and 20. The direct current blocking capacitors 11 and 28 have negligible reactance at the operating frequency for the circuit. Tubes V1 and voltage across capacitor C1, and a ninety degree leading 3 vc'tlta g'e across inductance Li. These voltage relationships are diagrammatically shown in Figure 2. Blocking capacitors 25 and 28 have neglig ible reactance at the operating frequency. Likewise, voltage E across phase shifting circuit 2i} will cause an alternating current 12 which will result in an in-phase voltage across resistor R2, ti ninety degree leading voltage across inductance L2, and a ninety degree lagging voltage across capacitor C2.

It will be noted that the alternating voltage on grid 16 of tube Vi will be the voltage across inductance L1, which is designated in Figure 2 as voltage Ee since the alternating voltage across blocking capacitor 25 is small. Also the alternating voltage on control grid 18 of tube V2 will be the voltage across capacitor C: which is designated in Figure 3 as Ee,. When phase shifting circuits and 20 are resonated, the currents I1 and I2 are both in phase with voltage E0 and the voltages EG, and Ed, are then in quadrature with E0 and opposite in phase from each other as shown in Figure 4. Resistors R1 and R2 are equal, and capacitances C1 and C2 and inductances L1 and L2 are chosen so that the absolute voltage Ee, at operating frequency across L1 will be equal to the absolute voltage Ea, across C2.

Since the tubes V1 and V2 are identical, the equal magnitude grid voltages on each tube will cause equal magnitude plate currents to fiow. Since generally plate current has an 180 degree phase relationship with grid voltage, it is seen in Figure 4 that the alternating plate current 1P1 of tube V1 is equal and opposite to the alternating plate current In, of tube V2 because their grid voltages EG, and En, are equal and opposite.

en there is no modulating audio voltage, the plate currents In, and In, will cancel each other since they are equal and opposite and will not provide any net plate current I to the oscillator tank circuit 10. Together, tubes V1 and V2 will therefore have zero reactance when no modulation is applied. The only effect which the reactance tube circuit will then have on the oscillator will be due to the current drawn through phase shifting circuits 15 and 20 which can be limited to any desired value by choosing resistors R1 and R2. Since the load drawn from the oscillator by the phase shifting circuits will be constant regardless of the amount of loading on the oscillator, it will not be a source of instability for the oscillator.

When audio voltage is applied to primary 22, two equal but opposite phase audio voltages will be induced in the secondary 23 because of center tap 24. One voltage EM will be induced in the half designated as MN and the other voltage Es will be induced in the half designated as NS. Because of their opposite phase, voltage EM will be increasing while voltage Es will be decreasing and vice versa. Due to the transconductance of the suppressor grids 26 and 27, the plate currents In, and In, will therefore proportionately increase and decrease respectively at the same instant. The currents In, and IP, will then no longer be equal and their difierence, which is the net output current I, will be proportional to the audio input voltage. This will be seen by examining Figure 4 and observing what opposite variations in the length of the IP, and In, vectors will do. Net current I will lead when the audio voltage swings positive, and it will lag when the audio voltage swings negative as shown in Figure 5. The output impedance of the circuit will therefore vary capacitively on positive audio swings and inductively on negative audio swings which will frequency modulate oscillator tank circuit 10 about its center resonant fre-- quency.

Blocking condenser blocks grid current flow through L1 and grid leak resistors 31 and 32 prevent charge buildup on control grids 16 and 18.

Since a preferred embodiment of this invention has been disclosed, various modifications and changes may be made by those skilled in the art without departing from the spirit and scope of the invention as hereafter defined by the appended claims.

I claim:

l. A reactance tube circuit comprising, a pair of electron tubes, an audio transformer with its primary connected to an input signal, the mid-point of the secondary of said transformer connected to ground, one end of said secondary of said transformer connected to a first grid of said first electron tube, the other end of said secondary connected to a first grid of the second electron tube, the cathodes of said first and second electron tubes connected together, the plates of said first and second electron tubes connected together, a first phase shifting circuit comprising a first condenser and first inductor connected respectively in series between ground and the plates of said tubes, a second phase shifting circuit comprising a second inductor and second condenser connected respectively in series between ground and the plates of said tubes, a second control grid of the first electron tube connected to the ungrounded terminal of the first condenser, 21 second control grid of the second electron tube connected to the ungrounded terminal of the second inductor, and a tunable oscillator connected to the plates of said first and second electron tubes.

2. A reactance tube circuit comprising, a pair of electron tubes with their plates and cathodes connected together respectively, an input transformer with its primary connected to an input voltage, the midpoint of the secondary of said input transformer connected to ground, one end of said secondary connected to a first control grid of said first electron tube, the other end of said secondary connected to the first control grid of the second electron tube, a variable oscillator with its frequency controlling circuit connected to the plates of said first and second electron tubes, a first phase shifting circuit comprising a resistor, a condenser and an inductor connected serially between the plates of said electron tubes and ground with one terminal of said inductor connected to ground, a second phase shifting circuit comprising a resistor, an inductor and a condenser serially connected between the plates of the electron tubes and ground with one terminal of said condenser conected to ground, a second control grid of the first electron tube connected to the other terminal of said inductor of the first phase splitting circuit, and a second control grid of the second electron tube connected to the other terminal of said condenser of the second phase splitting circuit.

3. A reactance tube circuit comprising, a pair of electron tubes with their plates and cathodes connected together respectively, an input transformer with its primary connected to an input voltage, the midpoint of the secondary of said input transformer connected to ground, one end of said secondary connected to a first control grid of said first electron tube, the other end of said secondary connected to the first control grid of the second electron tube, a variable oscillator with its frequency controlling circuit connected to the plates of said first and second electron tubes, a first phase shifting circuit comprising a resistor, a condenser and an inductor serially connected between the plates of said electron tubes and ground with one terminal of said inductor connected to ground, a second phase shifting circuit comprising a resistor, an inductor and a condenser connected between the plates of the electron tubes and ground with one terminal of said condenser connected to ground, a second control grid of the first electron tube connected to the ungrounded terminal of the inductor of the first phase shifting circuit, a second control grid of the second electron tube connected to the ungrounded terminal of the condenser of the second phase shifting circuit, and said first and second phase shifting circuits resonant at the desired center operating frequency of the oscillator.

4. A modulator circuit for varying the frequency of an oscillator comprising, a pair of electron tubes with their plates and cathodes connected together'respectively, the

oscillator connected to the plates of said first and second electron tubes, a first phase shifting circuit connected between the plates of said tubes and ground and comprising a resistor, a capacitor and an inductor and connected in series with one terminal of said inductor connected to ground, a second phase shifting circuit connected between the plates of said tubes and ground and comprising a resistor, an inductor and a capacitor and connected in series with one terminal of said capacitor connected to ground, an input transformer with its primary connected to an input voltage, the secondary of said input transformer with its center point connected to ground, one end of said sec ondary connected to a first control grid of the first electron tube, the other end of said secondary connected to a first control grid of the second electron tube, a second control grid of the first electron tube connected to the other terminal of said inductor of the first phase shifting circuit, and a second control grid of the second electron tube connected to the other terminal of said capacitor of the second phase shifting circuit.

5. A modulator circuit for varying the frequency of an oscillator comprising, a pair of electron tubes with their plates and cathodes connected together respectively, the oscillator connected to the plates of said first and second electron tubes, a first phase shifting circuit connected between the plates of said tubes and ground and comprising a resistor, a capacitor and an inductor and connected in series with one terminal of said inductor connected to ground, a second phase shifting circuit connected between the plates of said tubes and ground and comprising a resistor, an inductor and a capacitor and connected in series with one terminal of said capacitor connected to ground, an input transformer with its primary connected to an input voltage, the secondary of said input transformer with its center point connected to ground, one end of said secondary connected to a first control grid of the first electron tube, the other end of said secondary connected to a first control grid of the second electron tube, a sec- 0nd control grid of the first electron tube connected to the other terminal of said inductor of the first phase shifting circuit, a second control grid of the second electron tube connected to the other terminal of said capacitor of the second phase shifting circuit, and the first and second phase shifting circuits resonant at the desired center frequency of the oscillator.

6. A modulator circuit for varying the frequency of an oscillator comprising, a pair of electron tubes with their plates and cathodes connected together respectively, the oscillator connected to the plates of said first and second electron tubes, a first phase shifting circuit connected between the plates of said tubes and ground and comprising a resistor, a capacitor and an inductor and connected in series with one terminal of said inductor connected to ground, a second phase shifting circuit connected between the plates of said tubes and ground and comprising a resistor, an inductor and a capacitor and connected in series with one terminal of said capacitor connected to ground, an input transformer with its primary connected to an input voltage, the secondary of said input transformer with its center point connected to ground, one end of said secondary connected to a first control grid of the first electron tube, the other end of said secondary connected to a first control grid of the second electron tube, a second control grid of the first electron tube connected to the other terminal of said inductor of the first phase shifting circuit, a second control grid of the second electron tube connected to the other terminal of said capacitor of the second phase shifting circuit, and first and second grid resistors connected between the second grids of the first and second electron tubes and ground.

References Cited in the file of this patent UNITED STATES PATENTS 2,279,660 Crosby Apr. 14, 1942 2,296,630 Crosby Sept. 22, 1942 2,324,282 Crosby July 13, 1943