US2476803A - High stability receiver circuit - Google Patents

High stability receiver circuit Download PDF

Info

Publication number
US2476803A
US2476803A US503363A US50336343A US2476803A US 2476803 A US2476803 A US 2476803A US 503363 A US503363 A US 503363A US 50336343 A US50336343 A US 50336343A US 2476803 A US2476803 A US 2476803A
Authority
US
United States
Prior art keywords
tube
core
cathode
sheath
capacitor
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US503363A
Inventor
James D Booth
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
CBS Corp
Original Assignee
Westinghouse Electric Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Westinghouse Electric Corp filed Critical Westinghouse Electric Corp
Priority to US503363A priority Critical patent/US2476803A/en
Application granted granted Critical
Publication of US2476803A publication Critical patent/US2476803A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03DDEMODULATION OR TRANSFERENCE OF MODULATION FROM ONE CARRIER TO ANOTHER
    • H03D9/00Demodulation or transference of modulation of modulated electromagnetic waves
    • H03D9/06Transference of modulation using distributed inductance and capacitance
    • H03D9/0608Transference of modulation using distributed inductance and capacitance by means of diodes
    • H03D9/0616Transference of modulation using distributed inductance and capacitance by means of diodes mounted in a hollow waveguide

Definitions

  • My invention relates to radio circuits, and, in particular, relates to circuits for heterodyning radio frequency currents.
  • Oneespecially important field of application being to currents of extremely high frequencies such as 500 megacycles per second.
  • circuits At higher frequencies it is especially important that circuits be designed for the best possible stability. In such circuits it is particularly difficult to prevent reaction of one circuit on another in an objectionable degree. Similar reasons make it difiicult to-provide circuit arrangements which shall be sharply resonant to but a single frequency.
  • 'converter tube circuits such as those of a radio receiver, in which an incoming signal is heterodyned or mixed with'the output of a local oscillator.
  • One object of-my invention is accordingly to provide a method of coupling an input circuit with an amplifier tube by means of a coupling which shall be sharply resonant at only single i frequencies and integral multiples thereof.
  • Another object of my invention is to provide for coupling an input circuit to a tube by a resonant coupling in the form of a segment of a concentric line in which the entire arrangement is sharply resonant to but a single frequency and integral multiples thereof.
  • Another object of my invention is to provide a coupling between an input circuit and a tube in the form of a concentric line so arranged that the internal reactance of the tube is so connected as not to interfere with the sharpness of resonance of the concentric line segment to a single frequency or exact integral of harmonic thereof.
  • Stillanother object of my invention is to pro control electrode of a grid controlled tube in such a way that the said capacitor and the capacitance between the grid electrode and other electrodes of the tube form an efiective voltage and impedance divider between the input circuit and the tube.
  • Still another object of my invention is to provide an arrangement for coupling an input circuit, a converter tube and a local oscillator tube in such a way as to produce a very low degree of coupling between the resonant circuit of the local oscillator tube and the input circuit.
  • a still further object of my invention is to provide an arrangement for coupling a local oscillator tube to a converter tube. in such a way as to minimize the coupling between the resonant circuit of the oscillator tube and the converter tube.
  • a still further object of my invention is to provide a method of connecting an input circuit, a converter tube and an oscillator tube in such a way as to insure that the local oscillator tube produces currents determined substantially solely by the constants of its own resonant circuit.
  • a still further object of my invention is to provide a method of connecting a receiving antenna through a converter tube to an oscillation generator in such a way as to prevent the oscillation generator energy from being radiated by the receiving antenna.
  • an input antenna l which may be of a type adapted to receive ultra high frequency currents is connected through a concentric line 2 to a resonator 3 comprising a conducting core 4 located in the axis of a cylindrical surrounding conducting sheath 5.
  • the sheath 5 is made of approximately an integral number of quarter wave lengths of the -frequency which it isexpected to receive and is closed at each end by conducting walls.
  • One end of the core 4 is connected to one said end wall and to ground while the other end is connected to the other said end wall through a variable capacitor 6.
  • the core of the transmission line 2 is connected to a tap point I, the position of which may. if desired, be varied by suitable arrangements along the core 4, thereby producing an impedance match between the input line 2 and the input circuit of an amplifier or other tube to which it is expected to transmit energy.
  • a tube 8 provided with an. anode 9 and a cathode II and a control electrode I2 receives energy from the resonator 3.
  • a point on the core 4 closely adjacent the capacitor 6 is connected through a capacitor I3 to the control electrode I2.
  • the control electrode I2 is likewise connected through a, leak resistor It to its cathode I l which is preferably of the unipotential type.
  • the anode 9 is connected through a resistor It to the positive terminal of a source of direct current I5, the negative terminal of which is grounded.
  • the tube 8 is shown arranged. to convert, or mix the incoming signals with the output of a local oscillator tube It which may be of any suitable type but is preferably in the form of a tube having an anode II, a cathode I8 and a control electrode I9.
  • the anode I1 and the control electrode I 9 are coupled to each other by some convenient resonant circuit, for example, a pair of rods Ill, 22' having a length substantially equal to one quarter wave length of the current to be generated'bythe oscillation generator I6.
  • the anode I1 is connected through a resistor 23 to the-positive. terminal of a source of direct current 24, the negative terminal of which is grounded.
  • the control electrode 2I is connected through a resistor 25 to ground.
  • the cathode I8 is connected to the core 26 of a second segment of concentrictransmission line which preferably has. a length different from an integral'of one quarter wave length of the oscillation generator Hi.-
  • the sheath 21 of the last mentioned transmission line segment is connected to the core at the end remote from the cathode I8 and is likewise grounded.
  • the transmission line 25;, 21' is not resonant: to the frequency of the oscillation generator I6.
  • the core 26, is likewise connected by conductor 26A to the, oathode II- of the tube; 8 at Point 2&3.
  • the input circuit has negligible reactance due to the fact that it is resonantly tuned, the position of the tap I at a point remote from either end of the core 4 does not prevent the sharp tuning of the resonator 3 to a single frequency or integral harmonics thereof.
  • the capacitor I3 is preferably made about equal in value, or at least of the same order of magnitude, as the capacitance 28. If this is done the capacitances I3 and 28 form an effective voltage and impedance divider between the resonator 3 and the other electrode of the tube 8. By properly varying the value of the capacitor IS, the ratio of this voltage division may be controlled at will and the arrangement thus provides a device for impedance matching the output of the resonator 3 to the input of the tube, 8.
  • the variable tap 1, together with the resonator 3 and the capacitances I3 and 28, thus likewise provide an arrangement for effectively matching the impedance of the input circuit 2 to the input circuit of the tube 8.
  • the oscillation generator I6 its frequency is substantially determined by the resonant circuit comprising the rods 2!, 22, this frequency being such as'to constitute the length of these rods an integral, number of quarter wave lengths.
  • the concentric line 25, Z'I in the cathode lead from the tube I6 has substantially no effect on the oscillation frequency of the generator I6
  • the segment of the core 26 between the point of connection thereto of the cathode II and the ground forms a common path in the particular circuits of the tubes 8' and I6 and constitutes a coupling between them which is sufficient to mix the frequency generated by the tube I6 with the frequency impressed on the control electrode I2 by the input from antenna I.
  • the tube 8 Since the tube 8 is connected only indirectly to the network comprising oscillation generator IS- and is separated from the resonant circuit 2 I, 22 thereof, there is very little tendency for the currents of the frequency incident upon the antenna I to alter the frequency of oscillation of the tube I6.
  • the coupling between the antenna I and the resonant circuit of the oscillator generator I6 is extremely Weak.
  • the coupling between the oscillation generator I6 and the antenna I is reduced to a very low value by the network comprising the capacitance 28, capacitor I3, resonator 3 and tap point I. In consequence of this extremely low value of coupling between the oscillator generator I6 and antenna l, substantially no energy of the frequency oscillation generator I5. is fed back and radiated from. antenna I.
  • a resonator comprising a central conducting core surrounded by a conducting sheath, means for connecting one end of said sheath to one end of said core directly and for connecting the other end of said sheath to the other end of said core through a capacitor, a tube provided with an anode, a cathode and a control electrode, means for connecting said control electrode through a second capacitor to the end of said core adjacent said first capacitor, and a connection from said cathode to said sheath, means for connecting said input line to an intermediate point on said core, an oscillation generator comprising an anode, a control electrode and a cathode, a resonant circuit interconnecting said anode and said control electrode, a lead connecting said cathode and said anode comprising a central conductive core and a surrounding conducting sheath, a connection between an intermediate point on said central conducting core and the first-mentioned cathode and a connection between said surrounding sheath, the end
  • a resonator comprising a central conducting core surrounded by a conducting sheath, means for connecting one end of said sheath to one end of said core directly and for connecting the other end of said sheath to the other end of said core through a capacitor, a tube provided with an anode, a cathode and a control electrode, means for connecting said control electrode through a second capacitor to the end of said core adjacent said first capacitor, and a connection from said cathode to said sheath, means for connecting said input line to an intermediate point on said core, an oscillation generator comprising an anode, a control electrode and.- a cathode, a resonant circuit interconnecting said anode and said control electrode, comprising two quarter wave conductors in inductive relation with each other, a lead connecting said cathode and said anode comprising a central conductive core and a surrounding conducting sheath, a connection between an intermediate point on said central conducting core and the first-mentione
  • a resonator comprising a central conducting core surrounded by a conducting sheath, means for connecting one end of said sheath to one end of said core directly and for connecting the other end of said sheath to the other end of said core through a capacitor, a tube provided with an anode, a cathode and a cathode electrode, means for connecting said control electrode through a second capacitor to the end of said core adjacent said first capacitor, and a connection from said cathode to said sheath, said input line being connected to an intermediate point on said core, said second capacitor having a capacitance of the order of magnitude of the capacitance between said control electrode and said cathode, an oscillation generator comprising an anode, a control electrode and a cathode, a resonant circuit interconnecting said anode and said control electrode, a lead connecting said cathode and said anode comprising a central conductive core and a surrounding conducting sheath, a connection between an
  • a first tube comprising an anode, a control electrode and a cathode
  • a second tube comprising an anode, a control electrode and a cathode
  • a resonant circuit interconnecting the control electrode and cathode of said first tube
  • a connection between the cathode and anode of said second tube comprising a central conductive core surrounded by a conducting sheath connected to said core at its end remote from the cathode of said second tube, a resonant circuit positioned outside said sheath and interlinking the control electrode and anode of said second tube
  • a connection between the cathode of said first tube and a point intermediate the ends of said core means for causing current fiow from the end of said core remote from the cathode of said second tube to the anode thereof and means for causing current flow from the end of said core remote from the cathode of said second tube to the anode of said first tube.

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Control Of Motors That Do Not Use Commutators (AREA)

Description

July 19, 1949. J. b. BOOTH 2,476,803 a HIGH STABI LITY RECEIVER CIRCUIT I Filed Sept. 22. 1943 I OUTPUT chew/7i 2.2 002752 wqz s LEA/6T0 WITNESSES: INVENTOR James fifiaoflz.
Patented July 19, 1949 TENT OFFICE HIGH STABILITY necervenomourr' James D. Booth, Catonsville, Md., assignor to Westinghouse Electric Corporation, East Pittsburgh, Pa., a corporation of Pennsylvania Application September 22, 1943, Serial No. 503,363
4 Claims. 1.
My invention relates to radio circuits, and, in particular, relates to circuits for heterodyning radio frequency currents. Oneespecially important field of application being to currents of extremely high frequencies such as 500 megacycles per second.
At higher frequencies it is especially important that circuits be designed for the best possible stability. In such circuits it is particularly difficult to prevent reaction of one circuit on another in an objectionable degree. Similar reasons make it difiicult to-provide circuit arrangements which shall be sharply resonant to but a single frequency. One situation in which difiiculties of the foregoing nature are noticeable is in 'converter tube circuits such as those of a radio receiver, in which an incoming signal is heterodyned or mixed with'the output of a local oscillator. I have found great difliculty with prior art arrangements for coupling local oscillator and converter tubes in reducing the coupling between the oscillator and the input circuit to the converter sufficiently to prevent the oscillator from looking into step with the frequency of the incoming signal instead of maintaining its own frequency and heterodyning the latter.
One object of-my invention is accordingly to provide a method of coupling an input circuit with an amplifier tube by means of a coupling which shall be sharply resonant at only single i frequencies and integral multiples thereof.
Another object of my invention is to provide for coupling an input circuit to a tube by a resonant coupling in the form of a segment of a concentric line in which the entire arrangement is sharply resonant to but a single frequency and integral multiples thereof.
Another object of my invention is to provide a coupling between an input circuit and a tube in the form of a concentric line so arranged that the internal reactance of the tube is so connected as not to interfere with the sharpness of resonance of the concentric line segment to a single frequency or exact integral of harmonic thereof.
Stillanother object of my invention is to pro control electrode of a grid controlled tube in such a way that the said capacitor and the capacitance between the grid electrode and other electrodes of the tube form an efiective voltage and impedance divider between the input circuit and the tube.
Still another object of my invention is to provide an arrangement for coupling an input circuit, a converter tube and a local oscillator tube in such a way as to produce a very low degree of coupling between the resonant circuit of the local oscillator tube and the input circuit.
A still further object of my invention is to provide an arrangement for coupling a local oscillator tube to a converter tube. in such a way as to minimize the coupling between the resonant circuit of the oscillator tube and the converter tube.
A still further object of my invention is to provide a method of connecting an input circuit, a converter tube and an oscillator tube in such a way as to insure that the local oscillator tube produces currents determined substantially solely by the constants of its own resonant circuit.
A still further object of my invention is to provide a method of connecting a receiving antenna through a converter tube to an oscillation generator in such a way as to prevent the oscillation generator energy from being radiated by the receiving antenna.
Other objects of my invention will become apparent upon reading the following description taken in connection with the drawing in which the single figure is a diagrammatic showing of 1circuits embodying the principles of my invenion.
Referring in detail to the drawing, an input antenna l which may be of a type adapted to receive ultra high frequency currents is connected through a concentric line 2 to a resonator 3 comprising a conducting core 4 located in the axis of a cylindrical surrounding conducting sheath 5. The sheath 5 is made of approximately an integral number of quarter wave lengths of the -frequency which it isexpected to receive and is closed at each end by conducting walls. One end of the core 4 is connected to one said end wall and to ground while the other end is connected to the other said end wall through a variable capacitor 6. The core of the transmission line 2 is connected to a tap point I, the position of which may. if desired, be varied by suitable arrangements along the core 4, thereby producing an impedance match between the input line 2 and the input circuit of an amplifier or other tube to which it is expected to transmit energy.
A tube 8 provided with an. anode 9 and a cathode II and a control electrode I2 receives energy from the resonator 3. For this purpose a point on the core 4 closely adjacent the capacitor 6 is connected through a capacitor I3 to the control electrode I2. The control electrode I2 is likewise connected through a, leak resistor It to its cathode I l which is preferably of the unipotential type. The anode 9 is connected through a resistor It to the positive terminal of a source of direct current I5, the negative terminal of which is grounded.
The tube 8 is shown arranged. to convert, or mix the incoming signals with the output of a local oscillator tube It which may be of any suitable type but is preferably in the form of a tube having an anode II, a cathode I8 and a control electrode I9. The anode I1 and the control electrode I 9 are coupled to each other by some convenient resonant circuit, for example, a pair of rods Ill, 22' having a length substantially equal to one quarter wave length of the current to be generated'bythe oscillation generator I6. The anode I1 is connected through a resistor 23 to the-positive. terminal of a source of direct current 24, the negative terminal of which is grounded. The control electrode 2I is connected through a resistor 25 to ground.
The cathode I8 is connected to the core 26 of a second segment of concentrictransmission line which preferably has. a length different from an integral'of one quarter wave length of the oscillation generator Hi.- The sheath 21 of the last mentioned transmission line segment is connected to the core at the end remote from the cathode I8 and is likewise grounded. As a result of the above-described arrangement the transmission line 25;, 21' is not resonant: to the frequency of the oscillation generator I6. The core 26, is likewise connected by conductor 26A to the, oathode II- of the tube; 8 at Point 2&3.
Between the electrode [2 and the other electrodes of the tube 8, notably the cathode, there is an inherent capacitance which is represented in'the drawing by the capacitor 28. This capacitor 28 in series with the. coupling capacitor I3 is, in effect. connected between one end of the re 4 and ro n nd the capacitor is, in efiect, likewise so connected. This network of capacitances connected between said end of the core (I and its grounded sheath 5 will alter the frequency to which, the resonator 3 is resonant from exact correspondence to the length between its end faces. However, they will not in any way disturb the sharpness of its resonance to one particular frequency and integral multiples thereof. The particular value of this frequency can be varied through a. range by adjustment of the variable capacitor IL The situation just outlined is in contrast to that which would exist were the capacitor I3 connected to the core 4 at some point substantially displaced along the core 6 from its said end. In. the last-mentioned situation the capacitances determining the mode of electrical oscillation of the resonator 3 would be made unsymmetrical'and the chamber would not resonate to a single frequency. The connection of the capacitor I3 to a point near the end of the core 4 which is remote from that connected to the sheath 5* is, accordingly, 2. valuable feature of my invention. It may be noted that the transmission line 2 and tap I connect the antenna I: to the input circuit generally to a point on the core I which is remote from each end of that core. However, where, as is conventional in the case, the input circuit has negligible reactance due to the fact that it is resonantly tuned, the position of the tap I at a point remote from either end of the core 4 does not prevent the sharp tuning of the resonator 3 to a single frequency or integral harmonics thereof.
The capacitor I3 is preferably made about equal in value, or at least of the same order of magnitude, as the capacitance 28. If this is done the capacitances I3 and 28 form an effective voltage and impedance divider between the resonator 3 and the other electrode of the tube 8. By properly varying the value of the capacitor IS, the ratio of this voltage division may be controlled at will and the arrangement thus provides a device for impedance matching the output of the resonator 3 to the input of the tube, 8. The variable tap 1, together with the resonator 3 and the capacitances I3 and 28, thus likewise provide an arrangement for effectively matching the impedance of the input circuit 2 to the input circuit of the tube 8.
Turning to the oscillation generator I6, its frequency is substantially determined by the resonant circuit comprising the rods 2!, 22, this frequency being such as'to constitute the length of these rods an integral, number of quarter wave lengths. Such being the case, the concentric line 25, Z'I in the cathode lead from the tube I6 has substantially no effect on the oscillation frequency of the generator I6 However, the segment of the core 26 between the point of connection thereto of the cathode II and the ground forms a common path in the particular circuits of the tubes 8' and I6 and constitutes a coupling between them which is sufficient to mix the frequency generated by the tube I6 with the frequency impressed on the control electrode I2 by the input from antenna I. As a result, currents of the mixed frequencies may be derived from the output circuit between the lead 29 and ground. The value of the voltage of the frequency of the oscillator I6 thus impressed on the tube 8 can, of course, be varied by altering the position of the tap point of the lead connecting cathode II to the core 26.
Since the tube 8 is connected only indirectly to the network comprising oscillation generator IS- and is separated from the resonant circuit 2 I, 22 thereof, there is very little tendency for the currents of the frequency incident upon the antenna I to alter the frequency of oscillation of the tube I6. In short, the coupling between the antenna I and the resonant circuit of the oscillator generator I6 is extremely Weak. Similarly, the coupling between the oscillation generator I6 and the antenna I is reduced to a very low value by the network comprising the capacitance 28, capacitor I3, resonator 3 and tap point I. In consequence of this extremely low value of coupling between the oscillator generator I6 and antenna l, substantially no energy of the frequency oscillation generator I5. is fed back and radiated from. antenna I.
I have described a specific embodiment of my invention but the principles thereof are oi broader application in ways which should be evident to those skilled in the art.
' I claim as my invention:
1. In combination with an input line, a resonator comprising a central conducting core surrounded by a conducting sheath, means for connecting one end of said sheath to one end of said core directly and for connecting the other end of said sheath to the other end of said core through a capacitor, a tube provided with an anode, a cathode and a control electrode, means for connecting said control electrode through a second capacitor to the end of said core adjacent said first capacitor, and a connection from said cathode to said sheath, means for connecting said input line to an intermediate point on said core, an oscillation generator comprising an anode, a control electrode and a cathode, a resonant circuit interconnecting said anode and said control electrode, a lead connecting said cathode and said anode comprising a central conductive core and a surrounding conducting sheath, a connection between an intermediate point on said central conducting core and the first-mentioned cathode and a connection between said surrounding sheath, the end of said conducting core remote from the cathode of said oscillation generator and the first-mentioned sheath.
2. In combination with an input line, a resonator comprising a central conducting core surrounded by a conducting sheath, means for connecting one end of said sheath to one end of said core directly and for connecting the other end of said sheath to the other end of said core through a capacitor, a tube provided with an anode, a cathode and a control electrode, means for connecting said control electrode through a second capacitor to the end of said core adjacent said first capacitor, and a connection from said cathode to said sheath, means for connecting said input line to an intermediate point on said core, an oscillation generator comprising an anode, a control electrode and.- a cathode, a resonant circuit interconnecting said anode and said control electrode, comprising two quarter wave conductors in inductive relation with each other, a lead connecting said cathode and said anode comprising a central conductive core and a surrounding conducting sheath, a connection between an intermediate point on said central conducting core and the first-mentioned cathode and a connection between said surrounding sheath, the end of said conducting core remote from the cathode of said oscillation generator and the first-mentioned sheath.
3. In combination with an input line, a resonator comprising a central conducting core surrounded by a conducting sheath, means for connecting one end of said sheath to one end of said core directly and for connecting the other end of said sheath to the other end of said core through a capacitor, a tube provided with an anode, a cathode and a cathode electrode, means for connecting said control electrode through a second capacitor to the end of said core adjacent said first capacitor, and a connection from said cathode to said sheath, said input line being connected to an intermediate point on said core, said second capacitor having a capacitance of the order of magnitude of the capacitance between said control electrode and said cathode, an oscillation generator comprising an anode, a control electrode and a cathode, a resonant circuit interconnecting said anode and said control electrode, a lead connecting said cathode and said anode comprising a central conductive core and a surrounding conducting sheath, a connection between an intermediate point on said central conducting core and the first-mentioned cathode and a connection between said surrounding sheath, the end of said conducting core remote from the cathode of said oscillation generator and the first-mentioned sheath.
4. In combination, a first tube comprising an anode, a control electrode and a cathode, a second tube comprising an anode, a control electrode and a cathode, a resonant circuit interconnecting the control electrode and cathode of said first tube, a connection between the cathode and anode of said second tube comprising a central conductive core surrounded by a conducting sheath connected to said core at its end remote from the cathode of said second tube, a resonant circuit positioned outside said sheath and interlinking the control electrode and anode of said second tube, a connection between the cathode of said first tube and a point intermediate the ends of said core, means for causing current fiow from the end of said core remote from the cathode of said second tube to the anode thereof and means for causing current flow from the end of said core remote from the cathode of said second tube to the anode of said first tube.
JAMES D. BOOTH.
REFERENCES CITED The following references are of record in the file of this patent:
UNITED STATES PATENTS Number Name Date 2,106,776 Trevor et a1 Feb. 1, 1938 2,152,335 Trevor et a1 Mar. 28, 1939 2,223,835 Smith Dec. 3, 1940 2,197,124 Conklin Apr. 16, 1940 2,236,004 MacLean Mar. 25, 1941 2,277,638 George Mar. 24, 1942 2,366,750 Pray Jan. 9, 1945 OTHER REFERENCES Proceedings I. R. 151., June 1934, pp. 699-708, article on Suppression circuits. Print in 250-2033.
US503363A 1943-09-22 1943-09-22 High stability receiver circuit Expired - Lifetime US2476803A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US503363A US2476803A (en) 1943-09-22 1943-09-22 High stability receiver circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US503363A US2476803A (en) 1943-09-22 1943-09-22 High stability receiver circuit

Publications (1)

Publication Number Publication Date
US2476803A true US2476803A (en) 1949-07-19

Family

ID=24001770

Family Applications (1)

Application Number Title Priority Date Filing Date
US503363A Expired - Lifetime US2476803A (en) 1943-09-22 1943-09-22 High stability receiver circuit

Country Status (1)

Country Link
US (1) US2476803A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2512399A (en) * 1947-09-20 1950-06-20 Hartford Nat Bank & Trust Co Mixing circuit
US2679001A (en) * 1950-10-11 1954-05-18 Electro Voice Television receiving system
US2828466A (en) * 1950-06-03 1958-03-25 Coleman Instr Inc Alternating current ph electrometer
US3020401A (en) * 1960-01-11 1962-02-06 Rs Electronics Corp High frequency receiver with resonant cavity
US4267604A (en) * 1978-02-01 1981-05-12 Sony Corporation UHF electronic tuner

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2106776A (en) * 1935-02-23 1938-02-01 Rca Corp Receiving system
US2152335A (en) * 1935-12-06 1939-03-28 Rca Corp Short wave system
US2197124A (en) * 1937-04-30 1940-04-16 Rca Corp Oscillator with amplifier coupling
US2223835A (en) * 1938-01-29 1940-12-03 Rca Corp Ultra high frequency device
US2236004A (en) * 1938-07-30 1941-03-25 Rca Corp Ultra high frequency signaling system
US2277638A (en) * 1939-06-20 1942-03-24 Rca Corp Ultra high frequency system
US2366750A (en) * 1941-08-02 1945-01-09 George E Pray Tuning impedances for high radio frequencies

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2106776A (en) * 1935-02-23 1938-02-01 Rca Corp Receiving system
US2152335A (en) * 1935-12-06 1939-03-28 Rca Corp Short wave system
US2197124A (en) * 1937-04-30 1940-04-16 Rca Corp Oscillator with amplifier coupling
US2223835A (en) * 1938-01-29 1940-12-03 Rca Corp Ultra high frequency device
US2236004A (en) * 1938-07-30 1941-03-25 Rca Corp Ultra high frequency signaling system
US2277638A (en) * 1939-06-20 1942-03-24 Rca Corp Ultra high frequency system
US2366750A (en) * 1941-08-02 1945-01-09 George E Pray Tuning impedances for high radio frequencies

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2512399A (en) * 1947-09-20 1950-06-20 Hartford Nat Bank & Trust Co Mixing circuit
US2828466A (en) * 1950-06-03 1958-03-25 Coleman Instr Inc Alternating current ph electrometer
US2679001A (en) * 1950-10-11 1954-05-18 Electro Voice Television receiving system
US3020401A (en) * 1960-01-11 1962-02-06 Rs Electronics Corp High frequency receiver with resonant cavity
US4267604A (en) * 1978-02-01 1981-05-12 Sony Corporation UHF electronic tuner

Similar Documents

Publication Publication Date Title
US2441598A (en) Wave transmission
US2223835A (en) Ultra high frequency device
US2469222A (en) Crystal rectifier converter
US2272062A (en) Coaxial line ultra high frequency amplifier
US2135672A (en) Ultra short wave system
US2476803A (en) High stability receiver circuit
US2441452A (en) Frequency changing circuits
US2427107A (en) Centimeter wave apparatus
US2550524A (en) Balanced microwave detector
US2116996A (en) Variable tuned circuits
GB592402A (en) Improvements in apparatus for amplifying, generating, or changing the frequency of electric oscillations of ultra-high frequency
US2404745A (en) Ultra high frequency electron discharge device system
US2617038A (en) Ultrahigh-frequency device
US2594167A (en) Ultrahigh-frequency bridge circuits
US3270292A (en) Ultra high frequency transistor oscillator
US2637813A (en) Balanced microwave detector
US2141242A (en) Ultra short wave system
US2479537A (en) Detector-oscillator circuit for ultra high frequency receivers
US3443199A (en) Wave frequency multiplier employing a nonlinear device in a band-pass filter
US2516990A (en) Ultra high frequency mixer circuits
US2591982A (en) Superheterodyne receiver for very short waves
US2567208A (en) Crystal mixer for multiplex broadcasting
US2433386A (en) Ultra high frequency mixer circuit
GB632658A (en) Improvements in or relating to mixing circuit arrangements
US2203085A (en) Electrical oscillator for generation of high frequencies