|Publication number||US2735941 A|
|Publication date||Feb 21, 1956|
|Filing date||Sep 17, 1945|
|Publication number||US 2735941 A, US 2735941A, US-A-2735941, US2735941 A, US2735941A|
|Inventors||Richard C. Peck|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (5), Referenced by (20), Classifications (9)|
|External Links: USPTO, USPTO Assignment, Espacenet|
Feb. 21, 1956 Filed Sept. 17 1945 R. C. PECK HIGH FREQUENCY VACUUM TUBE CIRCUIT 2 Sheets-Sheet l I; E; J-
6 OU T PUT po 5 62 AAAA gwuem to'b RICHARD C. PECK @QQM W Feb. 21, 1956 R. c. PECK 2,735,941
HIGH FREQUENCY VACUUM TUBE CIRCUIT Filed Sept. 17, 1945 2 Sheets-Sheet 2 TTEE E l sz awe/whom RICHARD C. PECK WWLW 2,135,941 men FREQUENCY VACUUM TUBE CIRCUIT 7 Richard C; Peck, Washington, D. C. indication September 17,1945, Serial N0. 616,948
. 8 Claims. 01. 250-36 '(drantdimiaer Title 35, U. s. C0118 1952 See. 266) invention relates to vacuum tube amplifying circans; more particularly it relates to a means for employing s viitibnal vacuum tubes as oscillators or amplivery" highfreqiiencies.
his so me of flight is the factor which 7 governs the pper limit of frequency at which a convencuum tube may be usefully employed. When e sy is raised to such a high value that the time t eraser-r6115 passing between the electrodes is an able fraction of a period, conventional vacuum tubes and conventional circuits cease to function.
As a practical matter, however, the physical size of vacuum tube and the distributed capacitance and 'iiiducffarice resulting therefrom have in the past fixed a i ifictic'al upper limit of frequency much lower than the or an liniitimposed by transit time of electrons. ect of this invention is to provide a means for omlhgthe frequency-limiting effect of distributed ie'icta cs iii conventional vacuum tubes and thereby i6 6 possible useful employment of conventional t frequencies closely approaching the theoretical transit-time limit.
The invention will be discussed and described with c rice to the appended drawings, of whichi i 'gure 1 is diagrammatic representation of a highfrequency oscillator employing a conventional vacuum tube in a Colpitts circuit; this figure being used to exth' principle of operation of the invention;
Figure 2 is'a diagrammatic showing of a high-frequency oscillator employing an embodiment of the presefht invention in conjunction with a conventional vacult Figure 3 is a diagrammatic showing of another emhddim tit of the invention wherein conventional vacu- 'ss are employed as a frequency multiplying ampli er e 4 is a drawing which shows diagrammatically an od nt ofthe invention employing a split-anode negative resistance magnetron as a high frequency oscila i nre 5 is a view,.partly in cross section, of a physical ctidrl or; high frequency components for use in theembodiment of Figure 3; and
I Figure 6 is another cross section view of the apparatnc or Figure 5.
Referring to Figure 1, the oscillator therein shown eomprisesa triode vacuum tube 5, connected in a form the (Eolpitts circuit adapted for ultra-high-frequennice-. "Transmission line 6 serves as tank circuit for the oscillator; it consists of two conductors, numbered 61 and '62 respectively. One terminal of conductor 61 is connected to the plate of tube 5; the other terminal of conductor 61 is connected through R. F. of choke coil 6 to the positive side of D.-C. source 10. One terminal 6?" conductor 62 is connected to the grid of tube 5; the other. terminal of conductor 62 is connected to ground tn gridleak resistor 9. Conductors 61 and 62 are i6 by condenser 7 at the terminals adjacent choke 8 to or Condenser 7 has substantially zero im- 'at the operating frequency. Line 6 is, there- States Patent O 2,735,941 Patented Feb. 21, 1956 fore, for high frequency currents, a short-circuited section having its open terminals connected between grid and plate of tube 5. The cathode of tube 5 and the negative side of source 10 are grounded. R. F. power may be taken from the oscillator in any manner appropriate to the nature and impedance of the load; in this embodiment the R. F. output terminals 4 are connected respectively to ground and to the plate of tube 5 through blocking condenser 3.
The effective length of transmission line 6 includes the length of conductors 61 and 62 plus the length of the leads to and within tube 5 and the actual length of the tube electrodes themselves. According to transmission line theory such a line, open at one end and short-circuited at the other, is capable of oscillating in an infinite number of modes. Of these the fundamental mode is that wherein the total effective length of the line equals one quarter wavelength. The next higher mode has a frequency of oscillation three titmes as great as the fundamental frequency; in that mode the effective length of the line equals three quarters of a wavelength.
It is a property of self-excited vacuum tube oscillators that oscillation will be maintained at that frequency,
wherein losses are lowest for the particular oscillatory circuit being employed. In conventional oscillators using transmission line tank circuits the frequency adopted is that of the fundamental mode of the line. Consequently, while a line-controlled vacuum tube oscillator is theoretically capable of oscillating in many modes, a particular transmission line tank circuit, employed with a particular tube in a conventional circuit, does by its constants determine a unique frequency of oscillation.
In the light of the foregoing paragraphs, assume that a higher frequency is desired from the vacuum tube oscillator of Figure 1. The obvious procedure to ef fect an increase in frequency is to shorten line 6.- As line 6 is made shorter and shorter, the frequency of oscillation grows higher and higher until at last line 6 is eliminated entirely and condenser 7 is shortened directly between the grid and plate terminals of tube 5. The frequency of oscillation obtained under these conditions is the highest obtainable from the tube by conventional means. Moreover the efficiency and stability become very poor as the external line shrinks-in length, and in practice it is often impossible to obtain any oscillation at all when the external line has been reduced to the vanishing point. In any case the maximum frequency obtaintable is well below the theoretical limit imposed by transit time considerations.
With respect to the embodiments of the invention herein described, by enclosing a transmission line tank circuit in an appropriately designed resonant cavity, oscillation at the fundamental mode can be prevented and the tube can be forced to set up and maintain oscillations in the transmission-line tank circuit at one of the lines higher modes. Thus the output frequency of the oscillator may be made an odd multiple of the resonant frequency of the line, and tubes may be employed as oscillators virtually up to the frequency limit imposed by transit time. This result can be obtained because a resonant cavity short-circuits and suppresses all electromagnetic fields within it having a frequency lower than a critical cut-off frequency while allowing electromagnetic fields having a frequency near the cavitys resonant frequency to be maintained within the cavity.
The details of design may be best explained with reference to Figure 2, which shows, in diagrammatic form, one embodiment of the invention. In Figure 2, an oscillator is shown, incorporating tube 15. The tank circuit connected to tube 15 consists of transmission line 16, to gether with the leads and tube elements associated therewith. Line 16 comprises parallel conductors 161 and 162. One end of conductor 161 is connected to the plate of tube the other end is connected through R. F. choke coil 18 to the positive side of D.-C. source 20. One end of conductor 162 is connected to the grid of tube 15, the other end is connected through grid leak resistor 19 to ground. The ends of conductors 161 and 162 adjacent choke 18 and resistor 19 are joined by condenser 17, which is a substantially zero impedance at the operating frequency. The cathode of tube 15 and the negative side of source 20 are grounded.
Entirely surrounding line 16 and a portion of the envelope of tube 15 is resonant cavity 13. Cavity 13 may be cylindrical in shape or it may have a rectangular or other cross-section. Its size in this embodiment is such as to cause the oscillator to resonate at a frequency about three times the natural frequency of the tank circuit comprising line 16 and the leads and tube elements associated therewith. Cavity 13 is closed except for an aperture in one end adequate to admit a portion of the envelope of tube 15 and two small apertures 11 in the opposite end, necessary to allow the leads from line 16 to be brought out. R. F. output may be taken in any manner appropriate to the impedance of the load; in Figure 2 the R. F. output terminals 14 are connected between ground and the plate of tube 15. D. C. voltage on the plate is blocked from the R. F. load by condenser 21.
Cavity 13 has a physical dimension of approximately three-quarter wavelength at the resonant frequency of the system, but the capacitive loading of line 16 on the cavity 13 decreases its electrical length to a half wavelength. Since cavity 13 is essentially closed at both ends the lowest mode it can sustain is the half wavelength mode, which means line 16, connected for odd quarter wavelength operation, is forced into the three-quarter wavelength mode or higher.
When cavity 13 is oscillating in its fundamental mode the wavelength of oscillation is about twice the length of the cavity, a condition requiring substantially zero electric field at each end of the cavity and maximum electric field at a point about midway between the ends. This set of conditions conforms very well to three-quarter wave oscillation by the tank circuit associated with tube 15, since such oscillation places an electric-field node at the shorted end of line 16, an electric field maximum a quarter wavelength from the end, or about mirway between the ends of cavity 13, and another electric field node at the point one-half wavelength from the shorted end. The actual tube elements and the portion of the leads within the tube envelope external to cavity 13 constitute, electrically, a third quarter-wavelength, which places an electric field maximum between the plate and grid. (The electrical quarter-wave Within the envelope of tube 15 will normally be much less than a physical quarter-wave in length, because of the loading effect of the plate-to-grid capacitance.)
Whereas the cavity 13 encourages oscillation in the three-quarter Wavelength or triple frequency mode, it makes oscillation of tube 15 in the tank circuits fundamental mode impossible, because the frequency of fundamental mode oscillations is below the cutoff frequency of the cavity and cannot be sustained therein.
By employment of the present invention the upper frequency limit of standard tubes can be greatly increased over the frequencies obtainable with conventional circuits. For example, an RCA 8012 tube, whose upper frequency limit in conventional circuits is about 600 mc./s, has been made to oscillate, by use of this invention, at frequencies above 800 rnc./s.
Moreover, because of the high quality factor of the cavity, plus the higher quality factor obtainable in the tank circuit when its length need not be of vanishing proportions, improved etiiciency and frequency stability are obtained at very high frequencies with this invention.
This invention may also be applied to a frequency mul- 4 tiplying amplifier. Figure 3 shows a typical embodiment of this sort wherein a pairt of tubes are employed in pushpull as a frequency tripler. Referring to Figure 3, transmission line tank circuit 23, approximately one-quarter Wavelength long for the frequency of the input signal, consists of parallel conductors short circuited at one end. The open ends of line 23 are connected respectively to the grids of tubes 25 and 35, the short circuited end of line 23 is connected to ground through condenser 28 and resistor 29 in parallel. R. F. energy at the input frequency may be applied to input terminals 30. Coupling loop 22, connected to terminals 30, is inductively coupled to line 23. The cathodes of tubes 25 and 35 are grounded. Transmission line tank circuit 36 consists of two parallel conductors short circuited at one end. The open ends of line 36 are connected respectively to'the plates of tubes 25 and 35. The physical dimensions. of line 36 are approximately similar to those of line 23 In this embodiment the cavity does not wholly enclose the transmission line and part of the tube envelope as in the embodiment of Figure 2. If the frequency sought is not so high as to approach the absolute maximum, the cavity may be placed around only the transmission line itself as in Figure 3. Cavity 33 in Figure 3 resonates, with line 36 within it, at three times the signal frequency applied to input terminals 30. Cavity is closed but for apertures 32 in one end, to permit the passage of the conductors of line 36, and small aperture 38 in the opposite end. The short circuited end of line 36 is connected to the positive side of D.-C. source 40 by a wire passing out of cavity 33 through aperture 38. Condenser 37 is connected between the short-circuited end of line 36 and the adjacent end of cavity 33. The outside surflaee of cavity 33 and the negative side of source 40in; grounded. R. F. output from this circuit, as with the previous embodiment shown, may be taken in any man ner appropriate to the impedance of the load. In Figure 3 output terminals 27 are connected to the respective plates of tubes 25 and 35 through blocking condensers 26. The output voltage at terminals 27 is balanced rela, tive to ground. I
The operation of the embodiment of Figure 3 is similar in principle to that of the oscillator shown in Figure 2. The plate tank circuit is prevented by cavity 33 from oscillating at its normal fundamental frequency and is consequently set into oscillation in its triple-frequency, or three-quarter wavelength, mode by the energy supplied by tubes 25 and 35. The output power taken from ter minals 27 has, therefore, three times the frequency'of the energy fed to input terminals 30. By employing the principles of this invention, conventional tubes may be made to operate efficiently and stably at frequencies well above the practical frequency limits of conventional fre quency multiplier circuits. I
Figure 4 shows an embodiment of the invention efii ploying a split-anode negative resistance magnetron'as a high-frequency oscillator. The employment of the invention in this manner permits realization of higher frequency output from the magnetron than is available by conventional means and yields a higher degree of frequency stability than is usually obtainable from negative resistance magnetrons. Referring to Figure 4; tube 45 is a magnetron tube of the negative resistance split anode type. It is placed in a steady magnetic field provided by" a magnet which is not shown in the drawing. The two anode segments of the magnetron 45 are connected re-' spectively to the open terminals of a short-circuited transmission line section 4-6, which serves as resonant circuit for the magnetron oscillator. Line 46 is housed in a closed conducting resonant cavity 43, the conductors of line 46 protruding from the closed cavity 43 through apertures 53. The short-circuited end 47 of line 46 is connected to the end of cavity 43 at point 48, situated at a point within cavity 43 whereat the electric field is minimum when the cavity is oscillating in its fundamental mode. The positive side of D.-C. source 50 is connected to the outer surface of cavity 43 and the negative side of source 50 is connected to the cathode of magnetron tube 45. R. F. output may be taken from the oscillator by connecting a load to output terminals 51, which are connected to the ends of coupling loop 52. Coupling loop 52 extends through small apertures 54 in cavity 43 and is inductively coupled to line 46.
In operation, the properties of the magnetron cause a negative A.-C. resistance to appear across the anode segments of tube 45, supplying energy to transmission line tank circuit 46 and sustaining oscillations therein. As in the previously described embodiments, cavity 43 prevents the line 46 from oscillating in its fundamental mode. Line 46 can and does oscillate in its three-quarter wavelength mode, however, since oscillation in that mode produces fields which coincide with and reinforce oscillations in the cavity. The net effect, as in the other embodiments of the invention herein shown, is to permit successful and stable operation at frequencies closely approaching the limit imposed by transit time. In an application where the frequency required is very near the limit obtainable, the cavity may be constructed as in Figure 2, to Wholly enclose line 46 and part of the envelope of magnetron 45 as well, thus reducing the portion of the tank circuit outside the cavity to the anode segments themselves and a part of the leads within the evacuated tube envelope.
Figures and 6 illustrate typical physical construction which might be employed for the cavity and transmission line assembly used in the invention. Figure 5 is a view, partly in cross section, of an assembly suitable for use in the embodiment of Figure 3. The section in Figure 5 is taken along the axis of the resonant cavity. Figure 6 is a view of the same embodiment taken in section in a plane perpendicular to the cavity axis as indicated by the dotted line 6-6 in Figure 5.
Referring to Figure 5, the resonant cavity in this representative embodiment is cylindrical; the principal element 73 of the cavity is tubular and formed of rigid conducting material. The remainder of the cavity is formed by circular end plates 72 and 74, also formed of rigid conducting material. End plate 72 is secured to element 73 by a plurality of screws 83, symmetrically disposed around the periphery of plate 72 and threaded into holes drilled and threaded therefor in element 73. End plate 74 is similarly secured to the opposite end of element 73 by screws 81. Transmission line 76 consists of parallel conductors joined at one end, forming a bifurcated conducting member as shown. The open ends of line 76 pass through threaded insulating bushings 82, which are securely threaded into apertures in end plate 72. The axial openings in bushings 82 through which the conductors of line 76 pass are proportioned to effect a snug fit therefor.
From the closed or short-circuited end of line 76 a stub extension 78 protrudes along the axis of line 76, passing through bushings 77 and 87 which are fitted into an aperture in the center of end plate 74. A flange 84 on stub '78 fits snugly against bushing 77; the end of stub 78 is threaded and nut 79 is tightly threaded thereon so as to hold bushings 87 in place and effect rigid mechanical support for line 76. External connection to the short circuited end of line 76 may be effected by connection to the external end of stub 78. Stub 78 and the surrounding conducting surface of end plate 74 form the condenser shown in diagrammatic form in Figure 3 as condenser 37.
Figure 6 shows a section of the apparatus of Figure 5 taken in a plane perpendicular to the section in Figure 5. The section shown in Figure 6 is indicated on Figure 5 by the dotted line 66, looking toward end plate 72 as indicated by the arrows in Figure 5. Tubular element 73 is seen in cross section, as are the conductors of line 76. End plate 72 and insulating bushings 82 appear in plan view as shown in the drawing.
It will be understood that the embodiments of the invention shown and described herein are exemplary only, and
that the scope of the invention is to be determined by reference to the appended claims.
The invention described herein may be manufactured and used by or for the Government of the United States of America for governmental purposes without the payment of any royalties thereon or therefor.
What is claimed is:
' 1. A distributed-constants tanks circuit enclosed at least in part by a cavity resonator and electrically coupled thereto, said cavity resonator having a cutoff frequency higher than the frequency of the fundamental mode of oscillation of the tank circuit.
2. A tank circuit comprising a section of transmission line, said tank circuit enclosed at least in part by a cavity resonator and electrically coupled thereto, the lowest frequency of resonance of said cavity resonator being approximately an integral multiple of the frequency of the fundamental mode of oscillation of the tank circuit.
3. The combination of an oscillator comprising a distributed constants tank circuit having a given fundamental frequency of resonance, and a cavity resonator having a higher fundamental frequency of resonance than said tank circuit enclosing at least in part said tank circuit and electrically coupled thereto, said cavity resonator acting to operatively suppress fundamental mode oscillations in said tank circuit.
4. The combination of an oscillator comprising a tank circuit having a section of transmission line, said tank circuit having a given fundamental frequency of resonance, and a cavity resonator having a higher fundamental frequency of resonance than said tank circuit enclosing at least in part said transmission line and electrically coupled thereto, said cavity resonator serving to operatively suppress fundamental mode oscillations in said tank circuit.
5. An oscillator comprising a vacuum tube having at least first and second electrodes; a tank circuit effectively comprising the first and second electrodes, leads thereto within the tube, and a section of transmission line; and a cavity resonator having a cutoff frequency higher than the frequency of the fundamental mode of oscillation of the tank circuit, said cavity resonator enclosing the section of transmission line and enclosing at least in part said leads within the tube, said cavity resonator serving to suppress fundamental-mode oscillations in the tank circuit.
6. An oscillator comprising a vacuum tube having a grid and a plate; a tank circuit effectively comprising the grid, the plate, leads thereto within the tube, and a section of transmission line; and a cavity resonator having a cutoff frequency higher than the frequency of the fundamental mode of oscillation of the tank circuit, said cavity resonator enclosing the section of transmission line and enclosing at least in part said leads within the tube, said cavity resonator serving to suppress fundamental mode oscillations in the tank circuit.
7. An oscillator comprising a magnetron tube, a distributed constants tank circuit operatively coupled to said magnetron tube, and a cavity resonator enclosing the tank circuit at least in part and of such dimensions as to operatively suppress fundamental-mode oscillations in the tank circuit.
8. An amplifier having input means for applying high frequency energy to the input means, a vacuum tube fed by the input means; a tank circuit having distributed constants; a cavity resonator enclosing the tank circuit at least in part and of such dimensions as to operatively suppress fundamental mode oscillations in the tank circuit, and coupling means operative to feed energy from the vacuum tube to the tank circuit.
References Cited in the file of this patent
|Cited Patent||Filing date||Publication date||Applicant||Title|
|US2239905 *||Feb 19, 1938||Apr 29, 1941||Rca Corp||Filter circuits|
|US2310695 *||Sep 30, 1941||Feb 9, 1943||Bell Telephone Labor Inc||Oscillating system|
|US2314132 *||Jun 21, 1941||Mar 16, 1943||Bell Telephone Labor Inc||High frequency amplifier|
|US2427241 *||Mar 24, 1943||Sep 9, 1947||Hartford Nat Bank & Trust Co||Push-pull circuit arrangement for ultra-short waves|
|US2483189 *||Nov 28, 1945||Sep 27, 1949||Hartford Nat Bank & Trust Comp||Transmission line oscillator|
|Citing Patent||Filing date||Publication date||Applicant||Title|
|US2863007 *||Jun 23, 1954||Dec 2, 1958||Karl Fischer||Distributed amplifier arrangement|
|US3117285 *||May 26, 1960||Jan 7, 1964||Marconi Co Ltd||Very high frequency amplifier arrangements|
|US3202866 *||Dec 23, 1960||Aug 24, 1965||Philips Corp||Twin-tetrode electron discharge device having two-wire lecher line input and u-shapedmetal strip output means|
|US3558969 *||Dec 9, 1968||Jan 26, 1971||Philips Corp||Electron discharge tube having an anode forming part of a lecher-line with a heat dissipating element|
|US3699475 *||Feb 16, 1971||Oct 17, 1972||Gte Automatic Electric Lab Inc||Double-mode tuned microwave oscillator|
|US6396359 *||Apr 13, 2000||May 28, 2002||California Institute Of Technology||Tunable, distributed, voltage-controlled oscillator|
|US6529085||Feb 14, 2002||Mar 4, 2003||California Institute Of Technology||Tunable, distributed, voltage-controlled oscillator|
|US6573731||Jul 20, 2000||Jun 3, 2003||Tokyo Electron Limited||Electron density measurement and control system using plasma-induced changes in the frequency of a microwave oscillator|
|US6646386||Jul 20, 2000||Nov 11, 2003||Tokyo Electron Limited||Stabilized oscillator circuit for plasma density measurement|
|US6741944||Jul 20, 2000||May 25, 2004||Tokyo Electron Limited||Electron density measurement and plasma process control system using a microwave oscillator locked to an open resonator containing the plasma|
|US6799532||Aug 29, 2003||Oct 5, 2004||Tokyo Electron Limited||Stabilized oscillator circuit for plasma density measurement|
|US6853260||Sep 19, 2002||Feb 8, 2005||California Institute Of Technology||Tunable, distributed voltage-controlled oscillator|
|US6861844||Jul 20, 2000||Mar 1, 2005||Tokyo Electron Limited||Electron density measurement and plasma process control system using changes in the resonant frequency of an open resonator containing the plasma|
|US7091802||Jul 19, 2004||Aug 15, 2006||President And Fellows Of Harvard College||Methods and apparatus based on coplanar striplines|
|US7242272||Jul 19, 2004||Jul 10, 2007||President And Fellows Of Harvard College||Methods and apparatus based on coplanar striplines|
|US7274262||Jul 27, 2006||Sep 25, 2007||Presidents And Fellows Of Harvard College||Methods and apparatus based on coplanar striplines|
|US7741921||May 5, 2008||Jun 22, 2010||Waveworks, Inc.||Trigger-mode distributed wave oscillator system|
|US20050068116 *||Jul 19, 2004||Mar 31, 2005||President And Fellows Of Harvard College||Methods and apparatus based on coplanar striplines|
|US20050068127 *||Jul 19, 2004||Mar 31, 2005||President And Fellows Of Harvard College||Methods and apparatus based on coplanar striplines|
|WO2005011101A2 *||Jul 19, 2004||Feb 3, 2005||William Andress||Methods and apparatus based on coplanar striplines|
|U.S. Classification||331/91, 331/99, 331/76, 331/101, 330/55, 330/53|