US2158255A - Permeability-tuned intermediatefrequency transformer - Google Patents

Permeability-tuned intermediatefrequency transformer Download PDF

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US2158255A
US2158255A US176496A US17649637A US2158255A US 2158255 A US2158255 A US 2158255A US 176496 A US176496 A US 176496A US 17649637 A US17649637 A US 17649637A US 2158255 A US2158255 A US 2158255A
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inductance
circuits
frequency
gain
circuit
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William A Schaper
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Johnson Laboratories Inc
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    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H7/00Multiple-port networks comprising only passive electrical elements as network components
    • H03H7/01Frequency selective two-port networks
    • H03H7/0153Electrical filters; Controlling thereof
    • H03H7/0161Bandpass filters

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  • BClaiml- This invention relates to improvements in highfrequency resonant systems, such, for example, as those which are generally employed between the output terminals of a first vacuum tube and the input terminals of a second vacuum tube,
  • Resonant systems of the above-mentioned type are of two principal forms, one employing a single resonant circuit and the other employing two coupled resonant circuits, each circuit having an inductor and a capacitor, one or both of which elements is adjustable to align the circuits at a particular frequency or to permit varying the resonant frequency of each circuit over a limited range.
  • the present invention is particularly addressed to the form employing two resonantcirgo cults.
  • variable inductors preferably of the type employing movable ferromagnetic cores for inductance adjustment.
  • the resonant circuits may be tuned by inductance variation to secure alignment at a desired frequency and, once established, this alignment is substantially permanent.
  • coupled resonant-circuit devices adjustable by movable ferromagnetic cores have already been proposed, and in some of these the arrangement is such as to maintain the overall selectivity nearly the same for all positions of the adjustable cores.
  • any practical device V which achieves substantial constancy of one will of necessity have some variation of the other.
  • devices according to the present invention including the illustrative embodiments herein described, will have some variation in their selectivity as the cores are adjusted, but, as will be explained, this variation is small, particularly at critical coupling.
  • each circuit has constant gain, and the coupling between the circuits automatically varies as the cores are moved so as to maintain the over-all gain substantially constant.
  • a particular device will, in general, be adjustable to secure resonance at a particular frequency.
  • the inductance is varied to compensate for deviations in the capacitances in the circuits with which the device is associated, in such a way as to bring the product of the total effective capacitance and the total effective inductance to the correct value for the particular frequency.
  • the capacitance value in a particular case is high, the inductance value is adjusted to be correspondingly lower, and
  • each of the circuits is to have constant gain is that the ratio of its inductance to the product of its resistance and its capacitance, or L/RC, shall remain constant for any setting of the adjustments necessary to secure resonance at the intended frequency.
  • the method by which-the over-all gain of a device in accordance with my present invention is kept substantially constant consists first in arranging each of the circuits so that its individual dynamic resistance or L/RC ratio will, remain constant, and second in arranging the coupling between the two circuits so that it will automatically vary in accordance with a required relation to provide substantially constant over-all gain, regardless of adjustments in either of the circuits.
  • the inductors are so constructed that, at the chosen frequency and regardless of any adjust ment of inductance, they maintain substantially constant the ratio of inductance to the product of resistance and capacitance, L/RC, for the inividual circuits.
  • L/RC resistance and capacitance
  • the induct ance adjustment cam oi the circuits cured by movement oi a ferromagnetic core rota trve to the inductance coii in that circuit, these coils with their cores being so po i d h movement of either core to adjust the inductance capacitances or directly proportional to the cmcuit inductances.
  • Pairs or coupled circuitsof the hype here under consideratiom'however are usuy operated at a degree coupling somewhat reater than the critical value, in order to ac cure a desired width of band ofthe frequencies passed.
  • the size of the magnetic particles in the core and the method of insulation and degree of compression must be chosen with respect to the type of magnetic material employed.
  • Core materials suitable for use in embodiments of my invention and methods of constructing such cores are described in United States Patents Nos. 1,940,- 228, 1,932,689 and 1,982,690 to Polydorofi.
  • a core In general, if a core is to maintain the L/RC ratio in a circuit constant, it must increase the resistance in the circuit considerably more rapidly than it increases the inductance as it is inserted into the coil.
  • thecore must be designed with respect to the coil with which it is to be used, it is not possible togive specific directions for its construction, but the illustrative example to be described in connection with the drawings will be an adequate guide to the man skilled in the art.
  • Fig. l is an elevation, partly in section, of one form of coupling device'useful in carrying out my invention
  • FIG. 2 is a View of the coupling device of Fig; l, talren on the line 2-2 of l;
  • FIG. 3 is a schematic circuit diagram showing a coupling device such as the one illustrated in Figs. 1 and 2 connected between two vacuum tubes;
  • Figs. a and 5 show graphically how the gain and selectivit respectively, of a device in accordance with the invention vary as the inductance is changed in each of the resonant circuits.
  • a coupling device consisting of base plate i supporting spaced and internally threaded plugs 22 and 3 of metal or other suitable material.
  • Tubes 3 and 5 of insulating material are respectively mounted on plugs 2 and 3, with their axes in parallel relation.
  • Tube 4 supports an inductance coil ii, which preferably wound in twosections or pies, and within the tube is disposed core i with s. free sliding. fit.
  • Core l is made of compressed comminuted ferromagnetic material, and is attached to screw 8 by an insulating connector 9.
  • C011 6 and core 1 comprise adjustable inductor 6 1. Screw 8 engages the threads in plug 2, so that core I may be moved axially with respect to coil 8 by turning screw 3.
  • Tube, 5 contains a similar core, i0, similarlywhich are connected respectively in shunt with 3 coils 6 and i2.
  • a metal shield can it surroundsbase plate I and the parts carried thereby, base plate I being supported adjacent one side wall ofshield can It by nuts H engaging the exterarcane -nally threaded portions of plugs I and 8 which extend through the shield can.
  • tubes 4 and 5 have an-inside diameter of inch and a length of 1 1% inches.
  • Coils 6 and I! each consist of two pies 95 inch wide and u inch apart. Each pie consists of190 turns of 30/48 single-silk covered enamelled Litz wire. The inductance of each coil is 126'! microhenries in air. The Q of each coil in air is 157, and is 150 when shield can I6 is in place.
  • vacuum tubes i8 and I! are coupled by a coupling device contained within shield IS.
  • the output circuit of vacuum tube i8 includes an input resonant circuit comprising inductor lfl-II and shunt capacitor i5.
  • an output resonant circuit comprising inductor 6-4 and shunt capacitor I4 is connected in the input circuit of vacuum tube i9.
  • cores iii and I By adjustment of cores iii and I relatively to coils l2 and 6, respectively, the effective inductances of the input and output resonant circuits may be varied.
  • Input inductor lii-I2 is inductively coupled to output inductor 6-1, the degreeof coupling depending upon the spacing between tubes 4 and Sand upon the positions of cores 1 and i0 relative to coils G and II, respectively.
  • the insertion of cores 1 and iii inv to coils Band II respectively simultaneously increases the inductance of coils 6 and I! while maintaining the L/RC ratio of each resonant circuit substantially constant, and varies the inductive coupling between inductors 0-I and l0i2 substantially in accordance with Equation (2) given above; and the over-all gain of the coupling device is maintained substantially constant.
  • the above-mentioned inductance adjustment is made, not to vary thefrequency at which the device is to operate, but to compensate for' small variations in the tube and circuit capacitances and thus secure resonance at the desired frequency.
  • curve III shows the gain of a device in accordance with the invention when it is associated with an armplifying vacuum tube in the manner shown in Fig. 3.
  • the gain variation is about one per cent for a wide range of inductance variation.
  • Fig. 5 of the drawings the selectivity of a 456-kilocycle device in accordance with the invention is graphically presented.
  • , 22 and 23 show the selectivity for inductance values of 1505 microhenries, 1690 michrohenries and 2100 microhenries, respectively.
  • the variation of band width is only two kilocycles, and the maximum band width is 22 kilocycles.
  • the magnetic core may be utilized to increase the L/R and hence the Q of the coil.
  • the cores are partly inserted and the initial insertion of the core may be made to produce a substantial increase in the Q of the inductor.
  • This initial Q although somewhat decreased when the core is further inserted for adjustment of the inductance value, nevertheless remains higher than the Q of the air-core coil alone at the frequency at which the device is designed to operate.
  • a selective high-frequency coupling device including in combination input and output resonant circuits each having aninductor and a fixed capacitor and intended for operation at a given frequency, means for adjusting the inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said circuits being so coupled as to maintain the over-all gain of said coupling device .substantially constant regardless of said inductance adjustment.
  • a selective high-frequency coupling device including in combination input and output resonant circuits each having an inductor and a fixed capacitor and intended for operation at a given frequency, means for adjusting the inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said means varying the effective resistance of said inductors in such a way as to maintain the ratio of inductance to the product of resistance and capacitance for each of said circuits substantially constant, and said circuits being so coupled as to maintain the overall gain of said coupling device substantially constant regardless of said inductance adjustment.
  • a selective high-frequency coupling device including in combination input and output resonant circuits each having an inductor and a fixed capacitor and intended for operation at a given frequenicy, movable ferromagnetic cores for adjusting the. inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said cores varying the resistance of said inductors in such a way as to maintain the ratio of inductance to the product of resistance and capacitance for,
  • a selective high-frequency coupling device including in combination a pair of coupled resonant circuits each having an inductor and a fixed capacitor and intended for operation at a given frequency, movable ferromagnetic cores for adjusting the inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said cores varying the eifective resistance of each inductor in such a way as to maintain the ratio of inductance to the product of resistance and capacitance for each of said circuits substantially constant and amaarss simultaneously varying the coupling between said circuits in such a way as to maintain the over-all gain of said coupling device substantially constant regardless of said inductance adjustment.
  • a selective high-frequency coupling device including in combination input and output resonant circuits each having an inductor and a fixed capacitor, and inductance-adjusting means associated with each of said inductors for tuning the corresponding circuit to resonance at a given frequency, said circuits being coupled, said inductance-adjusting means and said coupling c0- operating to maintain the ratio of inductance to the product of resistance and capacitance for each of said circuits substantially constant and to maintain the over-all gain of said coupling device substantially constant regardless of said inductance adjustment.

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Description

May 16, 1939. w. A. scHAPER 2,158,255
PEHMEABILI'I'Y'TUNED INTERMEDIATE-FREQUENCY TRANSFORMER Filed Nov. 26, 1957 2 Sheets-Sheet 1 INVENTOR l V/LL/AM 4. 5CHAPER ATTO R N EY May 16, 1939.
w. A. scHAPER 2,158,255
PERMEABILITY- TUNED INTERMEDIATE -FREQUENCY TRANSFORMER 2 Sheets-Sheet 2 Filed Nov. 26, 1937 INF UT OFF RESONANCE INPUT AT RESONANCE FOR FIXED OUTPUT INDUCTANCE IN MICROHENRIES 1 1, 1 1 1 l l 50 -40 3O 20 IO W L 1 /AM A. JC/fAPf/E WW6. 7 a
ATTORN EY Patented May 16, 1939 UNITED STATES PATENT "OFFICE FREQUENCY TRANSFORMER poration of Illinois Application November 26, 1937, Serial No. 178,496
BClaiml- This invention relates to improvements in highfrequency resonant systems, such, for example, as those which are generally employed between the output terminals of a first vacuum tube and the input terminals of a second vacuum tube,
and which are intended for operation at a particular frequency, for example, in the intermediate-frequency amplifiers of radio receivers oi the superheterodyne type.
Resonant systems of the above-mentioned type are of two principal forms, one employing a single resonant circuit and the other employing two coupled resonant circuits, each circuit having an inductor and a capacitor, one or both of which elements is adjustable to align the circuits at a particular frequency or to permit varying the resonant frequency of each circuit over a limited range. The present invention is particularly addressed to the form employing two resonantcirgo cults.
degreeof inductive coupling between the two.
resonant circuits. The usual type of adjustable "trimmer capacitor, however, is appreciably affected by changes in temperature, and such capacitors also change in capacitance value with time, thus making it difficult if not impossible to maintain the desired performance characteristics in capacitively tuned fixed-inductance coupled resonant-circuit devices of the types now commonly employed.
The difficulty just described may be eliminated by employing fixed capacitors and accomplishing tuning by the use of variable inductors, preferably of the type employing movable ferromagnetic cores for inductance adjustment. In such a device, the resonant circuits may be tuned by inductance variation to secure alignment at a desired frequency and, once established, this alignment is substantially permanent. Several forms of coupled resonant-circuit devices adjustable by movable ferromagnetic cores have already been proposed, and in some of these the arrangement is such as to maintain the overall selectivity nearly the same for all positions of the adjustable cores.
' Under-certain circumstances, and in certain types of radio broadcast receivers and other similar apparatus, however, it may be highly desirable to maintain the gain, rather than the selectivity, of such a coupling device substantially ment of the components. The present invention presents the solution of this problem and describes illustrative embodiments which in actual practice have been found to achieve the desired result in a highly satisfactory manner.
It is to be'noted that since the conditions which must be fulfilled to secure constant gain are mathematically different from those required for constant selectivity, any practical device V which achieves substantial constancy of one will of necessity have some variation of the other. Thus devices according to the present invention, including the illustrative embodiments herein described, will have some variation in their selectivity as the cores are adjusted, but, as will be explained, this variation is small, particularly at critical coupling.
In accordance with the invention, the result is secured by a construction such that each circuit has constant gain, and the coupling between the circuits automatically varies as the cores are moved so as to maintain the over-all gain substantially constant.
It 'is an object of the invention, therefore, to provide a high-frequency coupling device in which substantially uniform gain is secured, regardless of inductance adjustment, without resort to expensive or complicated mechanical arrangements.
It is also an'object of this invention to provide a high-frequency coupling device in which the coupling between the resonant circuits is automatically regulated to compensate for the effect of adjustments of the individual resonant-circuit inductance values on the over-all gain characteristic.
In the design of devices in accordance with the invention, it is necessary to first determine the frequency at which they are to be operated. A particular device will, in general, be adjustable to secure resonance at a particular frequency. When the device is installed in the receiver and is adjusted to operate at the particular frequency for which it was designed, the inductance is varied to compensate for deviations in the capacitances in the circuits with which the device is associated, in such a way as to bring the product of the total effective capacitance and the total effective inductance to the correct value for the particular frequency. Thus, if the capacitance value in a particular case is high, the inductance value is adjusted to be correspondingly lower, and
vice versa.
The condition to be fulfilled if each of the circuits is to have constant gain is that the ratio of its inductance to the product of its resistance and its capacitance, or L/RC, shall remain constant for any setting of the adjustments necessary to secure resonance at the intended frequency.
The method by which-the over-all gain of a device in accordance with my present invention is kept substantially constant consists first in arranging each of the circuits so that its individual dynamic resistance or L/RC ratio will, remain constant, and second in arranging the coupling between the two circuits so that it will automatically vary in accordance with a required relation to provide substantially constant over-all gain, regardless of adjustments in either of the circuits.
Since the capacitances in each circuit are fixed, the inductors are so constructed that, at the chosen frequency and regardless of any adjust ment of inductance, they maintain substantially constant the ratio of inductance to the product of resistance and capacitance, L/RC, for the inividual circuits. Each circuit then has constant gain throughout its range of adJustability. Ellie device is preferably so designed that the capacitive coupling between the circuits is negligible,
and the arrangement is such that the inductive coupling coefiicient in changes automatically by the correct amount for any charms in the M ductance values, L1 or in, of either of the ihduc= tors, these quantities being related in the wolilrnown equation In: i l
in accordance with invention, the induct ance adjustment cam oi the circuits cured by movement oi a ferromagnetic core rota trve to the inductance coii in that circuit, these coils with their cores being so po i d h movement of either core to adjust the inductance capacitances or directly proportional to the cmcuit inductances. Pairs or coupled circuitsof the hype here under consideratiom'however, are usuy operated at a degree coupling somewhat reater than the critical value, in order to ac cure a desired width of band ofthe frequencies passed. Mathematical analysis of both the over coupled and the undercoupled conditions shows that the coupling coemcient may be expressed in terms of the individual circuit inductance values as follows:
where cis the over-all gain, at the center or the response curve, which is to be constant; and ho is a constant which depends upon theinductance and capacitance of each circuit and the frequency, and is defined by tion of k for variations in the circuit inductances,
To maintain constant L/RC in each of the circuits, the size of the magnetic particles in the core and the method of insulation and degree of compression must be chosen with respect to the type of magnetic material employed. Core materials suitable for use in embodiments of my invention and methods of constructing such cores are described in United States Patents Nos. 1,940,- 228, 1,932,689 and 1,982,690 to Polydorofi. In general, if a core is to maintain the L/RC ratio in a circuit constant, it must increase the resistance in the circuit considerably more rapidly than it increases the inductance as it is inserted into the coil. Since, in any practical case, thecore must be designed with respect to the coil with which it is to be used, it is not possible togive specific directions for its construction, but the illustrative example to be described in connection with the drawings will be an adequate guide to the man skilled in the art.
The invention will now be described by referenceto a preferred embodiment shown in the accompanying draw'mgs, in which:
Fig. l is an elevation, partly in section, of one form of coupling device'useful in carrying out my invention;
2 is a View of the coupling device of Fig; l, talren on the line 2-2 of l;
3 is a schematic circuit diagram showing a coupling device such as the one illustrated in Figs. 1 and 2 connected between two vacuum tubes; and
Figs. a and 5 show graphically how the gain and selectivit respectively, of a device in accordance with the invention vary as the inductance is changed in each of the resonant circuits.
Reierrin.g to Figs. 1 and 2 of the drawings, there is shown a coupling device consisting of base plate i supporting spaced and internally threaded plugs 22 and 3 of metal or other suitable material. Tubes 3 and 5 of insulating material are respectively mounted on plugs 2 and 3, with their axes in parallel relation. Tube 4 supports an inductance coil ii, which preferably wound in twosections or pies, and within the tube is disposed core i with s. free sliding. fit. Core l is made of compressed comminuted ferromagnetic material, and is attached to screw 8 by an insulating connector 9. C011 6 and core 1 comprise adjustable inductor 6 1. Screw 8 engages the threads in plug 2, so that core I may be moved axially with respect to coil 8 by turning screw 3. Tube, 5 contains a similar core, i0, similarlywhich are connected respectively in shunt with 3 coils 6 and i2.
A metal shield can it surroundsbase plate I and the parts carried thereby, base plate I being supported adjacent one side wall ofshield can It by nuts H engaging the exterarcane -nally threaded portions of plugs I and 8 which extend through the shield can.
In one successful embodiment of the invention intended to be used at 458 kilocyclas, tubes 4 and 5 have an-inside diameter of inch and a length of 1 1% inches. Coils 6 and I! each consist of two pies 95 inch wide and u inch apart. Each pie consists of190 turns of 30/48 single-silk covered enamelled Litz wire. The inductance of each coil is 126'! microhenries in air. The Q of each coil in air is 157, and is 150 when shield can I6 is in place. When cores 1 and III are fully inserted in coils 6 and II, respectively, the inductance of each coil is increased to 2294 microhenries, so that the cores have an effective permeability of approximately 1.8 when used with the above-described two-pie coils. Coils O and 42 are mounted 1}! inches between centers, and are equally spaced from base plate I.
Referring to Fig. 3 of the drawings, vacuum tubes i8 and I! are coupled by a coupling device contained within shield IS. The output circuit of vacuum tube i8 includes an input resonant circuit comprising inductor lfl-II and shunt capacitor i5. Similarly, an output resonant circuit comprising inductor 6-4 and shunt capacitor I4 is connected in the input circuit of vacuum tube i9. By adjustment of cores iii and I relatively to coils l2 and 6, respectively, the effective inductances of the input and output resonant circuits may be varied. Input inductor lii-I2 is inductively coupled to output inductor 6-1, the degreeof coupling depending upon the spacing between tubes 4 and Sand upon the positions of cores 1 and i0 relative to coils G and II, respectively.
In operation, the insertion of cores 1 and iii inv to coils Band II respectively simultaneously increases the inductance of coils 6 and I! while maintaining the L/RC ratio of each resonant circuit substantially constant, and varies the inductive coupling between inductors 0-I and l0i2 substantially in accordance with Equation (2) given above; and the over-all gain of the coupling device is maintained substantially constant. The above-mentioned inductance adjustment is made, not to vary thefrequency at which the device is to operate, but to compensate for' small variations in the tube and circuit capacitances and thus secure resonance at the desired frequency.
Referring to Fig. 4 of the drawings, curve III shows the gain of a device in accordance with the invention when it is associated with an armplifying vacuum tube in the manner shown in Fig. 3. The gain variation is about one per cent for a wide range of inductance variation.
In Fig. 5 of the drawings, the selectivity of a 456-kilocycle device in accordance with the invention is graphically presented. Curves 2|, 22 and 23 show the selectivity for inductance values of 1505 microhenries, 1690 michrohenries and 2100 microhenries, respectively. At a ratio of output off resonance to output at resonance of 10, the variation of band width is only two kilocycles, and the maximum band width is 22 kilocycles.
If the inductors are made in accordance with the disclosure of United States Patent No. 1,982, 690 to Polydorofl, the magnetic core may be utilized to increase the L/R and hence the Q of the coil.
As will be seen from Figs. 1 and 2 of the drawings, the full range of adjustability of the cores does not completely remove them from the coils.
Thus for any condition of adjustment, the cores are partly inserted and the initial insertion of the core may be made to produce a substantial increase in the Q of the inductor. This initial Q, although somewhat decreased when the core is further inserted for adjustment of the inductance value, nevertheless remains higher than the Q of the air-core coil alone at the frequency at which the device is designed to operate.
Thus the use of properly designed inductors employing ferromagnetic cores provides not only substantially constant gain throughout the range of adjustability,'but also an improved degree of selectivity over that previously realized in coupling devices intended for the same purpose.
The scope of the invention is not limited to the embodiments shown in the drawings and described herein, but includes as well such further modified forms as will occur to those skilled in the art to embody the principles hereinabove disclosed.
Having thus described vmy invention, what I claim is:
1. A selective high-frequency coupling device including in combination input and output resonant circuits each having aninductor and a fixed capacitor and intended for operation at a given frequency, means for adjusting the inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said circuits being so coupled as to maintain the over-all gain of said coupling device .substantially constant regardless of said inductance adjustment.
2. A selective high-frequency coupling device including in combination input and output resonant circuits each having an inductor and a fixed capacitor and intended for operation at a given frequency, means for adjusting the inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said means varying the effective resistance of said inductors in such a way as to maintain the ratio of inductance to the product of resistance and capacitance for each of said circuits substantially constant, and said circuits being so coupled as to maintain the overall gain of said coupling device substantially constant regardless of said inductance adjustment.
3. A selective high-frequency coupling device including in combination input and output resonant circuits each having an inductor and a fixed capacitor and intended for operation at a given frequenicy, movable ferromagnetic cores for adjusting the. inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said cores varying the resistance of said inductors in such a way as to maintain the ratio of inductance to the product of resistance and capacitance for,
tance thereof due to conditions of use to thereby maintain resonance at said frequency, the coupling between said circuits being varied by said cores in such a way as to maintain the over-all gain of said coupling device substantially constant regardless of said inductance adjustment.
5. A selective high-frequency coupling device including in combination a pair of coupled resonant circuits each having an inductor and a fixed capacitor and intended for operation at a given frequency, movable ferromagnetic cores for adjusting the inductance of each of said circuits to compensate for changes in the capacitance thereof due to conditions of use to thereby maintain resonance at said frequency, said cores varying the eifective resistance of each inductor in such a way as to maintain the ratio of inductance to the product of resistance and capacitance for each of said circuits substantially constant and amaarss simultaneously varying the coupling between said circuits in such a way as to maintain the over-all gain of said coupling device substantially constant regardless of said inductance adjustment.
6. A selective high-frequency coupling device including in combination input and output resonant circuits each having an inductor and a fixed capacitor, and inductance-adjusting means associated with each of said inductors for tuning the corresponding circuit to resonance at a given frequency, said circuits being coupled, said inductance-adjusting means and said coupling c0- operating to maintain the ratio of inductance to the product of resistance and capacitance for each of said circuits substantially constant and to maintain the over-all gain of said coupling device substantially constant regardless of said inductance adjustment.
WILLIAM A. SCHAPER.
ijertificate of (Zorrection Patent No. 2,l58,2f55.
May 16, 1939.
WILLIAM A. SCHAPER It is hereby certified that errors appear in the printed specification of the above numbered patent requiring correction as follows: Page 2, first column, lines 3839,
for the equation page 3, first column, line 64, for the word output both occurrences, read input; and second column, line 72, claim 4, for fixer read fixed; and that the said Letters Patent should be read with these corrections therein that the same may conform to the record of the case in the Patent Office.
Signed and sealed this 4th day of July, A. D. 1939.
[sent] Henry Van Arsdale Acting Commissioner of Patents.
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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2509427A (en) * 1946-08-28 1950-05-30 Mallory & Co Inc P R Transformer
US2544152A (en) * 1943-10-27 1951-03-06 Hartford Nat Bank & Trust Co High-frequency coil system
US2544508A (en) * 1948-03-26 1951-03-06 Rca Corp Signal transfer apparatus

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2544152A (en) * 1943-10-27 1951-03-06 Hartford Nat Bank & Trust Co High-frequency coil system
US2509427A (en) * 1946-08-28 1950-05-30 Mallory & Co Inc P R Transformer
US2544508A (en) * 1948-03-26 1951-03-06 Rca Corp Signal transfer apparatus

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