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US2252058A - Method and means for testing resonant circuits - Google Patents

Method and means for testing resonant circuits Download PDF

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US2252058A
US2252058A US331964A US33196440A US2252058A US 2252058 A US2252058 A US 2252058A US 331964 A US331964 A US 331964A US 33196440 A US33196440 A US 33196440A US 2252058 A US2252058 A US 2252058A
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frequency
circuits
oscillator
circuit
resonant
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Donald S Bond
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RCA Corp
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R27/00Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
    • G01R27/28Measuring attenuation, gain, phase shift or derived characteristics of electric four pole networks, i.e. two-port networks; Measuring transient response
    • G01R27/32Measuring attenuation, gain, phase shift or derived characteristics of electric four pole networks, i.e. two-port networks; Measuring transient response in circuits having distributed constants, e.g. having very long conductors or involving high frequencies

Definitions

  • This invention relates to a method of and means for visually indicating the tracking of a plurality of tunable circuits with respect to each other, or with respect to the signal frequency which, for any dial setting, combines with the local oscillator of a superheterodyne receiver to produce the desired intermediate frequency.
  • Theoretically perfect tracking between the signal frequency circuits and the local oscillator is not usually obtained in receivers of commercial design.
  • a compromise is generally made in which the receiver is aligned at two points near the high and low frequency limits of the receiver, respectively, the oscillator circuit being so designed that a third.V point of alignment is produced near the mid-frequency.
  • the receiver is actually aligned at three points, these points corresponding to the points of intersection of the frequency vs. capacity curves of the oscillator and signal frequency circuits, as is well known.
  • the value of one or more components may vary from the desired value.
  • the oscillator coil, the series capacitor, or a section of the tuning condenser may vary from the prescribed value with the result that the receiver may be badly misaligned at frequencies intermediate the frequencies at which it has been adjusted. Such errors are particularly common in the high frequency bands of the receivers, and, in addition, it is possible to adjust'the oscillator to a frequency on the wrong side of the signal frequency.
  • Other objects of this invention include the provision of a method of and means for producing signal frequency currents Which are automatically maintained at a fixed frequency above or below the oscillator as the receiver is tuned throughout its range; the provision of improved testing apparatus; and the provision of an improved testing method.
  • the foregoing objects are achieved by applying frequency modulated currents to the signal frequency circuits of a receiver, and visually indicating by means of a cathode ray tube, or the like, the resonance curves of each circuit as the circuits are tuned throughout their operating range. Tracking errors at any particular lpoint in the tuning range are determined by measuring the distance between the peaks of the resonance curves.
  • a modification of this invention which is designed particularly for use with superheterodyne receivers, provides a frequency modulated oscillator the average frequency of which is equal to the intermediate frequency of the receiver under test.
  • Figure 1 is the circuit diagram of a device for testing the tracking of two tuned signal frequency circuits
  • Figure 2 is a sketch representing the cathode ray trace produced by such Ia device
  • Figure 3 is a similar sketch of the traces produced by a pair of resonant circuits where the catho'de ray employs the double image principle
  • Figure l is a curve representing the saw-tooth deflecting Voltage spectively, of a receiver of the tuned radio frequency type, or the first and second amplier stages ⁇ of a superheterodyne receiver.
  • Tube I3 is the tube which is normally used to couple the first and second amplifier stages.
  • a separate rectier 25 may be employed in addition to, or as a substitute for the receiver detector tube.
  • the rectified output voltage is applied ⁇ to the second commutator segment 21 through a circuit which may include an amplifierr29.
  • is provided which may be any conventional oscillator, and need not be described in detail. Its output is connected to the receiver antenna binding post 33 and to the grid of lthe amplifier tube
  • is determined by a variable condenser 35 which is preferably operatively connected to variable condensers 3i and k39 which tune the first and second tuned circuits, respectively.
  • is varied above and ⁇ below this average frequency by a mechanical or an electronic f-requency modulator.
  • may be connected in parallel with tuning condenser 35, and rotated at any desired speed by means of a motor 43.
  • the commutator arm 45 is rotated at a speed which issuitably related to they speed of rotation of modulating condenser 4
  • thespeed of rotation ofthe commutator is onehalf that of the modulating condenser so that a complete modulating cycle is completed duringrthe time veach amplifier is connected to the cathode ray tube. This may be accomplished by a suitable speed reducing gear connected to the motor 43 or Vby means of a separate motor 431.
  • the horizontal deflection of Ithe cathode ray tube 41 is provided by vmeans of -a conventional saw-tooth i oscillator .49 which is synchronized with the modulation frequency by means of a connection 5
  • the saw-tooth oscillator may produce asymmetrical de'flecting voltage of thertype illustrated-'in' Fig. 4 orian asymmetrical 'saw-tooth voltage of the type illustrated in Fig. 5, both of which are Well known.
  • the system is adjusted for operation by adjusting the average frequency of the oscillator to the value desired as the low frequency test point on the receiver.
  • the receiver is adjusted by utilizing the trimmer ,capacitors 53 and 55 to align both circuits to 'the ,same frequency.
  • the circuits may be aligned vat .the low frequency end by varying the coil inductance, if desired.
  • the accuracy of the indication is somewhat improved by employing the double image system in which the cathode ray beam is moved horizontally in a given direction as the oscillator frequency increases, and again in the same direction as :the oscillator frequency decreases.
  • the horizontal deiiecting voltage is of the type illustrated .in Fig. 5.
  • two resonance curves are produced .for each resonant circuit, the curves 4falling onlopposite sides of a center line fo when the resonant frequency of the circuit differs from the average Yfrequency f-of the oscillator.
  • Such a curve is illustrated in Fig. 3.
  • the circuits are aligned when the two resonant peaks coincide.
  • the ytracking of the two tuned circuits over their :entire operating range may be checked rapidly. and accurately .by rotating the tuning condenser ofthe receiver and noting the variation offthe two .resonance curves.
  • Fig.; 6 which is particularly suited for use with a superheterodynereceiver.
  • the oscillator operates at a frequency above orbelow vthesignal frequency by an amount equal to the intermediate frequency. Since the selectivityof the circuit is due primarily vto the intermediate frequency circuits, it will be appreciated. .that the primary consideration in aligning such a .receiver is that the amplifier circuits,.that is, Uhe antenna transformer and the radio frequency ampliflerare tuned to that frequency which combines with the oscillator to produce the intermediate frequency.
  • the rst tuned circuit 9 is, as before, the antenna transformer which normally couples the antenna terminal 33 to the input of amplier tube I3. During this test, however, the grid cap of the amplifier tube is removed and the output of the antenna transformer is connected to a rectifier I9.
  • the second tuned circuit il includes the radio frequency amplifier coil, the secondary of which is normally connected to the grid of the mixer tube l, but for this test, the grid cap is removed and connected to the input of a rectifier 25. It is to be understood that the input characteristics of the rectiers i9 and 25 are preferably made identical to the input characteristics of the tubes Which they replace, so that the circuits Will not be detuned when the substitution is made.
  • the plate of the mixer tube 5l, in a superheterodyne receiver, is normally connected to the primary of the rst intermediate frequency'transformer 59.
  • this connection is broken, by means o1 a socket adapter, by means of which a radio frequency choke 5l is included in the plate circuit, and a connection made to the plate from the ungrounded end of a potentiometer E3 through a blocking capacitor 65.
  • remote from the plate is bypassed to ground by a capacitor 6i.
  • the local oscillator circuit is connected to the number l and number 2 electrodes of the mixer tube 5l in a conventional manner.
  • the frequency of this circuit is determined by a variable capacitor 6@ which is connected in series with the usual tracking capacitor 1l.
  • the oscillator'condenser 59 is operatively coupled to the remaining sections of the tuning condenser 53 and 55, which tune the rst and second signal frequency circuits, respectively.
  • the two rectifiers i9 and 25 are connected to a cathode ray indicator il through commutator segments 2l and 2l and the commutator arm i5, as before.
  • a switch 'i3 by means of which the vertical deflecting electrode of the cathode ray tube may be connected either to the commutator arm 45 or to a suitable point of the audio frequency receiver circuit, the latter connection making possible the use of the cathode ray to check the alignment of the intermediate frequency amplifier in a conventional manner.
  • the movable arm of potentiometer 53 is connected to the grid electrode of an amplifier tube l5.
  • a pair of potentiometersV 'il and i9 are connected in parallel between ground and the anode of amplifier 'i5 through a blocking capacitor 3l.
  • the first potentiometer Tl is connected to the input electrode of the receiver radio frequency amplifler tube i3, While the second potentiometer 'FQ is connected to the receiver antenna binding post 33.
  • the frequency modulated oscillator 33 is provided, the average frequency of which is equal to the intermediate frequency of the receiver. It is modulated throughout a range of frequencies by means of a frequency modulator 85. As before, the frequency modulator supplies a synchronizing voltage for the cathode ray saw-tooth oscillator 6.9,Wl1ic ⁇ h ⁇ may be of either type discussed above.
  • the output of the modulated oscillator 83 is connected to the control grid electrode of the mixer tube 5l'.
  • the modulated intermediate frequency currents from the oscillator 83 are combined in the mixer tube 5l With the locally generated oscillations of the receiver.
  • the plate circuit of the mixer tube 5l therefore, includes sum and difference components. If the oscillator is operating above the signal frequency to produce the receiver intermediate frequency, then the difference component appearing in the plate circuit Will necessarily be equal to the signal frequency to which the receiver will respond for the given setting of the oscillator. If the oscillator is operating below the signal frequency, as is the case in said receivers in high frequency bands, the sum component will then be equal to the signal frequency to which the receiver Will respond for the particular oscillator frequency. Thus if the signal frequency circuits 0f the receiver are adjusted to the signal frequency component produced in the output of the mixer tube, and this throughout the entire operating range of the receiver, the desired alignment and tracking Will have been achieved.
  • the tuning knob 8l By setting the tuning knob 8l to the desired aligning point, the frequency of the local oscillator is first adjusted and then the signal frequency circuits are adjusted until their resonant peaks, illustrated in Fig. '7, fall upon the vertical line fu which corresponds to the signal frequency.
  • Fig. 7 Only one curve for each resonant circuit has been indicated in Fig. 7 but it is to be understood that the double system similar to that illustrated in Fig. 3 may also be used.
  • the tracking of the two signal frequency circuits is determined by slowly rotating the tuning knob 3l throughout its entire range. Since the signal frequency itself is varied, since it is derived from the local oscillator, the center line fo on the cathode ray screen represents the correct frequency at all points. Consequently, the degree and direction of the deviation of the antenna and amplifier circuits are instantly observed. If the receiver has been improperly aligned this fact may be immediately determined, since in that case the signal frequency circuits Will not track properly and will deviate Widely from the normal frequency fo. Normal deviations may be marked directly on the cathode ray screen so that the operator may check the accuracy of the alignment in a minimum of time.
  • the method of indicating the alignment of said circuits throughout their tuning range which includes the steps of generating a radio frequency voltage the nominal frequency of which is variable over said range of frequencies, modulating the frequency of said radio frequency voltage throughout a range less than said range of frequencies, applying said frequency modulated voltage to said resonant circuits, producing separate indications of the resonant rise of voltage in said circuits, and simultaneously varying the nominal frequency of said frequency modulated voltage and the resonant frequency of said circuits, the difference between said indications being a measure of the alignment of said circuits.
  • the method of indicating the alignment of said circuits which includes the steps of generating a radio frequency Voltage the nominal frequency of which is variable over a range of frequencies, modulating the frequency of said voltage at a constant rate throughout a range less than said range of frequencies, applying said frequency modulated voltage to said resonant circuits, producing separate indications of the resonant rise of voltage in said circuits, and simultaneously varying the resonant frequency of said circuits and the nomiynal frequency of said radio frequency voltage through similar frequency ranges to indicate the relative alignment of said circuits throughout their operating range.
  • a radio device having a plurality of resonant circuits tunable over a range of frequencies in response to a common control means
  • the method of indicating the relative resonant frequencies of said circuits throughout said range which includes the steps of generating an alternating voltage the nominal frequency of which is variable over a range in response to said common control means, modulating the frequency of said voltage above and below said nominal frequency s at a constant rate, applying said modulated voltage simultaneously to said resonant circuits, adjusting the nominal frequency of said voltage to a value substantially equal to the resonant frequency of said circuits at a given point in said range, indicating the resonant rise of voltage of said Ycircuits at said point, and operating said control means to tune said circuits throughout said range, While correspondingly varying the nominal frequency of said alternating voltage.
  • a radio device having a plurality of resonant circuits tunable over a range of frequencies in response to a common control means
  • the method of indicating the relative resonant frequencies of said circuits throughout said range which includes the steps of generating an alternating voltage the nominal frequency of which is variable over a range corresponding to the range covered by said tunable circuits, cyclically modulating the frequency of said Voltage, impressing said modulated voltage simultaneously on said resonant circuits, adjusting the nominal frequency of said voltage to a value substantially equal to the resonant frequency of said circuits at a given point in said range, indicating the resonant rise of voltage of said circuits at said point, and operating said control means to tune said circuits throughout said range while correspondingly varying the nominal frequency of said voltage.
  • the method of indicating the tracking of said circuits which includes the steps of generating an alternating voltage, cyclically varying the frequency of said voltage over a range of frequencies less than the tunable range of said circuits, applying said cyclically varying voltage to said circuits, producing indications of the resonant rise of voltage in said circuits, and simultaneously varying the average frequency of said alternating voltage and the resonant frequency of said circuits throughout said range, the difference between said indications at any point being an indication of the tracking of said circuits.
  • the method of indicating the tracking of said circuits which includes the steps of generating an alternating voltage whose frequency is also variable over said range of frequencies in response to said common control means, cyclically varying the frequency of said voltage over a range of frequencies inclusive of the range covered by the resonance curve of said tunable circuits, applying said Voltage to said tunable circuits, Visually and separately indicating the resonant rise of voltage vs. frequency characteristic of said tunable circuits, and operating said common control means to vary the resonant frequency of said circuits and the frequency of said voltage throughout said range, the difference between said indications being a measure of the error in tracking of said circuits.
  • the method of indicating the tracking of said circuits which includes the steps of generating an alternating voltage whose average frequency is tunable over said range in response to said common control means, separately varying the frequency of said voltage over a range of frequencies which includes the range covered by the resonance curve of said tunable circuits, applying said voltage to said circuits, deriving output voltages from said resonant circuits, commutating said voltages, producing a beam of electrons, deflecting said beam in a first direction in accordance with said commutated voltages, deflecting said beam in a second direction in synchronism with the cyclic varia-tion of the frequency of said voltage, utilizing said beam to produce luminous traces of the resonance characteristic of said circuits, and simultaneously varying the average frequency of said voltage and the resonant frequencies of said tunable circuits throughout said range, the distance between the peaks of said
  • the method of determining the tracking of said circuits which includes the steps of generating an alternating voltage whose nominal frequency is variable over said first range of frequencies, cyclically modulating the frequency of said voltage throughout a second range smaller than said rst range, applying said modulated Voltage to said circuits, deriving output voltages from said circuits, producing a beam of electrons, deflecting said beam in a first direction alternately and successively in accordance with said output voltages, deflecting said beam in a second direction in synchronism with the cyclic modulation of said alternating voltage, utilizing said beam to produce traces representing the resonance characteristic of said circuits, tuning said circuits over said first range of frequencies While simultaneously varying the nominal frequency of said alternating voltage over the same range of frequencies, the distance between the peaks of said traces at any point being a measure of the tracking of said circuits at that point.
  • a superheterodyne receiver having a local oscillator tunable over a iirst range of frequencies and a resonant circuit simultaneously tunable over a second range of frequencies displaced from saidrrst range' by a fixed interme d-iate frequency
  • the method of checking the tracking between saidl tunable circuit and said oscillator Which includes the steps ⁇ of generating an alternating voltage of said intermediate frequency, combining said voltage with oscillations produced by said local oscillator to produce a signal-frequency voltage, applying said vsignalfrequencyvvoltage to said resonant circuit, and indicating the deviation of the resonant frequency of said circuit from the frequency of said signal frequency voltage.
  • a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit and common means for tuning said oscillator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency
  • the method of checking the tracking of said oscillator and said signal frequency circuit which includes the steps of generating intermediate frequency oscillations, combining said intermediate frequency oscillations with oscillations produced by said local oscillator to produce signal frequency oscillations, applying said signal frequency oscillations to said signal frequency circuit, and indicating the deviation of the resonant frequency of said circuit from said signal frequency.
  • a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit, and common means for tuning said oscil lator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency
  • the method of checking the tracking of said oscillator and said circuit which includes the steps of generating a current of said intermediate frequency, combining said current with currents of said oscillator frequency to produce signal frequency currents, applying said signal frequency currents to said circuit, and indicating the deviation of the resonant frequency of said circuit from said signal frequency.
  • a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit, and common means for tuning said oscillator and said circuit throughout frequency ranges Which differ by a substantially constant intermediate frequency
  • the method of checking the tracking of said oscillator and said circuit which includes the steps of generating a frequency modulated current the average frequency of which is equal to said intermediate frequency, combining said current With currents of said oscillator frequency to produce signal frequency currents, applying said signal frequency currents to a circuit, and visually indicating the deviation of the resonant frequency of said circuit as said oscillator and said circuit are tuned throughout their respective ranges.
  • a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit, and common means for tuning said oscillator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency
  • the method of checking the tracking of said oscillator and said circuit which includes the steps of generating a frequency modulated current the average frequency of which is equal to said intermediate frequency, combining said currents with other currents of said oscillator frequency to produce frequency modulated signal frequency currents, applying said signal frequency currents to said circuit, deriving rectified output currents proportional to the resonant rise -in voltage in said circuit, and utilizing'said output currents to indicate visually the deviation of the resonant frequency of saidvcircuit from said signal frequency as said oscillator Vand said circuit. are tuned throughout their respective ranges.
  • the method of determining the alignment of a superheterodyne receiver having a variable frequency local oscillator, at least one signal frequency circuit and means for simultaneously tuning said oscillator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency which includes the steps of generating a current of said intermediate frequency, modulating the frequency of said current throughout a range of the order of the bandwidth of said circuit, combining said modulated intermediate frequency current with oscillatory currents from said local oscillator to produce frequency modulated signal frequency currents, applying said signal frequency currents to said signal frequency circuit, deriving rectified output currents from said circuit and utilizing said output currents to produce a trace corresponding to the resonance curve of said circuit, the deviation of the resonant frequency of said circuit from the average frequency of said signal frequency currents being a measure of the tracking of said circuit.
  • a device for indicating the alignment of a receiver having a pair of tunable signal frequency circuits which includes, in combination, means for producing a frequency-modulated current of said signal frequency, means for applying said signal frequency currents to said circuits, means for simultaneously varying the resonant frequency of said tunable circuits and the average frequency of said signal frequency currents, and means for indicating the deviation of the resonant frequency of said circuits from the average frequency of said signal frequency currents.
  • a device for indicating the alignment of a superheterodyne receiver having a pair of tunable signal frequency circuits and a tunable local oscillator which includes, in combination, means including said local oscillator for producing a frequency-modulated signal frequency current,
  • a device for indicatingv the alignment of a superheterodyne receiver having a pair of tunable sign-a1 frequency circuits and a tunable local oscillator which includes, in combination, an intermediate frequency oscillatorgvmeans for periodi--v cally varying the frequency of said oscillator, means for combining currents from said intermediate frequency oscillator With currents from said local oscillator to produce a frequency modulated signal frequency current, means for ap- 10

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Description

D. S. BOND Aug. 12, 1941.
METHOD AND MEANS FOR l.TESTING RESONANT CIRCUITS Filed April 27, 1940 2 Sheets-Sheet 1 Snvenfor o n d Gttomeg Donald 5'. B
D. s. BOND 2,252,058
METHOD AND MEANS FOR TESTING RESONANT CIRCUITS Filed April 27, 1940 2 Sheets-Sheet 2 W @m6 S39 &6? I m.w\ uw MN rubi E .N tml w L mm..
Illu
Patented Aug. 12, 1941 METHOD AND MEANS FOR TESTING RESONANT CIRCUITS Donald S. Bond, Philadelphia, Pa., assgnor to yRadio Corporation of America, a corporation of Delaware I Application April 27, 1940, Serial No. 331,964
`(ICI. Z50- 20) 18 Claims.
This invention relates to a method of and means for visually indicating the tracking of a plurality of tunable circuits with respect to each other, or with respect to the signal frequency which, for any dial setting, combines with the local oscillator of a superheterodyne receiver to produce the desired intermediate frequency.
In a radio receiver having a common tuning or control knob for varying the resonant frequency of a plurality of selector circuits through the operating range of the receiver, it is necessary to adjust the coil inductances and the capacity of the tuning capacitors so that the various tuned circuits each resonate at the same frequency throughout the range of the receiver. This is usually accomplished by means of trimmer capacitors which are connected in parallel with the main tuning condenser. An additional problem is involved in the case of a superheterodynereceiver, since the frequency of the local oscillator, which is generally tuned by a variable capacitor similar to those used to tune the radio frequency circuits, must be maintained at a fixed frequency above or below the resonant frequency of the other circuits,-which are herein called the signal frequency circuits.
Theoretically perfect tracking between the signal frequency circuits and the local oscillator is not usually obtained in receivers of commercial design. A compromise is generally made in which the receiver is aligned at two points near the high and low frequency limits of the receiver, respectively, the oscillator circuit being so designed that a third.V point of alignment is produced near the mid-frequency. Thus the receiver is actually aligned at three points, these points corresponding to the points of intersection of the frequency vs. capacity curves of the oscillator and signal frequency circuits, as is well known.
Assuming that each receiver from a production line is correctly wired and that each component is of the correct value, satisfactory overall periormance isobtained when the receiver is aligned at the two points mentioned above. However, the value of one or more components may vary from the desired value. Thus the oscillator coil, the series capacitor, or a section of the tuning condenser may vary from the prescribed value with the result that the receiver may be badly misaligned at frequencies intermediate the frequencies at which it has been adjusted. Such errors are particularly common in the high frequency bands of the receivers, and, in addition, it is possible to adjust'the oscillator to a frequency on the wrong side of the signal frequency.
The mere fact that the receiver was apparently adjusted properly at one or two points does not guarantee the proper performance throughout the operating range of the receiver.
It is the principal object of this invention to provide a method of and means for observing the tracking of the tuned circuits of a receiver at the points of alignment and also at all intermediate points. Other objects of this invention include the provision of a method of and means for producing signal frequency currents Which are automatically maintained at a fixed frequency above or below the oscillator as the receiver is tuned throughout its range; the provision of improved testing apparatus; and the provision of an improved testing method.
In accordance with one embodiment of this invention, the foregoing objects are achieved by applying frequency modulated currents to the signal frequency circuits of a receiver, and visually indicating by means of a cathode ray tube, or the like, the resonance curves of each circuit as the circuits are tuned throughout their operating range. Tracking errors at any particular lpoint in the tuning range are determined by measuring the distance between the peaks of the resonance curves. A modification of this invention which is designed particularly for use with superheterodyne receivers, provides a frequency modulated oscillator the average frequency of which is equal to the intermediate frequency of the receiver under test. By coupling this oscillator to the receiver oscillator, a combination current is produced, the nominal frequency of which is equal to the signal frequency required to produce the given intermediate frequency for all points within the operating range. The deviation of the resonant frequency of the signal frequency circuits from this locally produced signal is indicated by means of a cathode ray tube, and is a measure of the receiver alignment.
This invention will be better understood from the following description when considered in connection with the accompanying drawings. Its scope is indicated by the append-ed claims.
Referring to the drawings, Figure 1 is the circuit diagram of a device for testing the tracking of two tuned signal frequency circuits; Figure 2 is a sketch representing the cathode ray trace produced by such Ia device; Figure 3 is a similar sketch of the traces produced by a pair of resonant circuits where the catho'de ray employs the double image principle; Figure lis a curve representing the saw-tooth deflecting Voltage spectively, of a receiver of the tuned radio frequency type, or the first and second amplier stages` of a superheterodyne receiver. Tube I3 is the tube which is normally used to couple the first and second amplifier stages. Its plate is connected to the second tuned circuit In normal operation its grid would be connected to the secondary l5 of the first tuned circuit 9 by means of a lead ll. In order to test the receiver, however, the grid cap` is removed .from the tube and connected to a .rectifier i9 having similar input impedance characteristics. The rectifier output is connected to a commutator armature 2| through a circuit which may include an :amplifier 23. vThe output of th-e second tuned circuit is normally connected to the receiver detector tube. Consequently, it is possible to utilize the existing detector by connecting a test prod toa suitable point at which a' rectied voltage. is available. On the other hand, a separate rectier 25 may be employed in addition to, or as a substitute for the receiver detector tube. VIn any case, the rectified output voltage is applied `to the second commutator segment 21 through a circuit which may include an amplifierr29. l
A frequency modulated oscillator 3| is provided which may be any conventional oscillator, and need not be described in detail. Its output is connected to the receiver antenna binding post 33 and to the grid of lthe amplifier tube |3. The average frequency of the oscillator 3| is determined by a variable condenser 35 which is preferably operatively connected to variable condensers 3i and k39 which tune the first and second tuned circuits, respectively. The frequency of oscillator `3| is varied above and` below this average frequency by a mechanical or an electronic f-requency modulator. For example, a rotating condenser 4| may be connected in parallel with tuning condenser 35, and rotated at any desired speed by means of a motor 43.
The commutator arm 45 is rotated at a speed which issuitably related to they speed of rotation of modulating condenser 4| so that the outputs of amplifier 23 and 29 are alternately and successively vconnected to the vertical deiiecting electrode of a cathode ray tube M. Preferably thespeed of rotation ofthe commutator is onehalf that of the modulating condenser so that a complete modulating cycle is completed duringrthe time veach amplifier is connected to the cathode ray tube. This may be accomplished by a suitable speed reducing gear connected to the motor 43 or Vby means of a separate motor 431.
The horizontal deflection of Ithe cathode ray tube 41 is provided by vmeans of -a conventional saw-tooth i oscillator .49 which is synchronized with the modulation frequency by means of a connection 5| Awhich lis, for example, connected to a small generator mounted `on the shaft of motor 43. The saw-tooth oscillator may produce asymmetrical de'flecting voltage of thertype illustrated-'in' Fig. 4 orian asymmetrical 'saw-tooth voltage of the type illustrated in Fig. 5, both of which are Well known. The system is adjusted for operation by adjusting the average frequency of the oscillator to the value desired as the low frequency test point on the receiver. Since the oscillator frequency is being swept through t'his average value, a pair of resonance curves will be produced on the cathode ray tube corresponding to the resonant characteristics of the two circuits under test. While these curves will be drawn alternately, due to the operation of the commutator, they will appear simultaneously on the cathode ray screen and may be visually compared. 'I'wo such curves are illustrated in Fig. 2. The actual resonant frequency f1 of the first resonant circuit does not coincide with the actual resonant frequency f2 of the second circuit. rIhe distance between the two resonant peaks is, therefore, a measure of the tracking error at the low frequency point in question.
.Byrotating the tuning knob to increase the frequency response of the tuned circuits and oscillator, a continuous check may be had of the tracking of the two circuits. At the high frequency end the receiver is adjusted by utilizing the trimmer , capacitors 53 and 55 to align both circuits to 'the ,same frequency. In accordance with conventional practice .the circuits may be aligned vat .the low frequency end by varying the coil inductance, if desired.
The accuracy of the indication is somewhat improved by employing the double image system in which the cathode ray beam is moved horizontally in a given direction as the oscillator frequency increases, and again in the same direction as :the oscillator frequency decreases. In ordertogaccomplish this the horizontal deiiecting voltage is of the type illustrated .in Fig. 5. In such a case, two resonance curves are produced .for each resonant circuit, the curves 4falling onlopposite sides of a center line fo when the resonant frequency of the circuit differs from the average Yfrequency f-of the oscillator. Such a curve is illustrated in Fig. 3. The circuits are aligned when the two resonant peaks coincide. As before, the ytracking of the two tuned circuits over their :entire operating range may be checked rapidly. and accurately .by rotating the tuning condenser ofthe receiver and noting the variation offthe two .resonance curves.
,A modification of this invention is illustrated in Fig.; 6 which is particularly suited for use with a superheterodynereceiver. In a receiver of this type the oscillator operates at a frequency above orbelow vthesignal frequency by an amount equal to the intermediate frequency. Since the selectivityof the circuit is due primarily vto the intermediate frequency circuits, it will be appreciated. .that the primary consideration in aligning such a .receiver is that the amplifier circuits,.that is, Uhe antenna transformer and the radio frequency ampliflerare tuned to that frequency which combines with the oscillator to produce the intermediate frequency. It is not sufficient, therefore, merely to check the aligtiment ofthe signal frequency circuits, that is, the antenna -transformer and the amplifier transformer, since such a test does not take into consideration variations in the oscillator frequency. Consequently, I vhaveprovided a method of testing a superheterodyne receiver in which the signal? utilized to test the alignment of the signal frequency circuits, corresponding to that produced by oscillator 3| of Fig. 1, is a function of the actual' oscillator 'frequencyat each point throughout the operating range. By indicating the deviation of the resonance frequencies of the signal frequency circuits from the frequency of this resultant current, the resultant curves accurately determine the true operating alignment of the receiver.
Referring to Fig. 6, the rst tuned circuit 9 is, as before, the antenna transformer which normally couples the antenna terminal 33 to the input of amplier tube I3. During this test, however, the grid cap of the amplifier tube is removed and the output of the antenna transformer is connected to a rectifier I9. The second tuned circuit il includes the radio frequency amplifier coil, the secondary of which is normally connected to the grid of the mixer tube l, but for this test, the grid cap is removed and connected to the input of a rectifier 25. It is to be understood that the input characteristics of the rectiers i9 and 25 are preferably made identical to the input characteristics of the tubes Which they replace, so that the circuits Will not be detuned when the substitution is made.
The plate of the mixer tube 5l, in a superheterodyne receiver, is normally connected to the primary of the rst intermediate frequency'transformer 59. For the purpose of the present test, however, this connection is broken, by means o1 a socket adapter, by means of which a radio frequency choke 5l is included in the plate circuit, and a connection made to the plate from the ungrounded end of a potentiometer E3 through a blocking capacitor 65. The end of the radio frequency choke coil 5| remote from the plate is bypassed to ground by a capacitor 6i.
The local oscillator circuit is connected to the number l and number 2 electrodes of the mixer tube 5l in a conventional manner. The frequency of this circuit is determined by a variable capacitor 6@ Which is connected in series with the usual tracking capacitor 1l. The oscillator'condenser 59 is operatively coupled to the remaining sections of the tuning condenser 53 and 55, which tune the rst and second signal frequency circuits, respectively.
The two rectifiers i9 and 25 are connected to a cathode ray indicator il through commutator segments 2l and 2l and the commutator arm i5, as before. For convenience, I have provided a switch 'i3 by means of which the vertical deflecting electrode of the cathode ray tube may be connected either to the commutator arm 45 or to a suitable point of the audio frequency receiver circuit, the latter connection making possible the use of the cathode ray to check the alignment of the intermediate frequency amplifier in a conventional manner.
The movable arm of potentiometer 53 is connected to the grid electrode of an amplifier tube l5. A pair of potentiometersV 'il and i9 are connected in parallel between ground and the anode of amplifier 'i5 through a blocking capacitor 3l. The first potentiometer Tl is connected to the input electrode of the receiver radio frequency amplifler tube i3, While the second potentiometer 'FQ is connected to the receiver antenna binding post 33.
The frequency modulated oscillator 33 is provided, the average frequency of which is equal to the intermediate frequency of the receiver. It is modulated throughout a range of frequencies by means of a frequency modulator 85. As before, the frequency modulator supplies a synchronizing voltage for the cathode ray saw-tooth oscillator 6.9,Wl1ic`h` may be of either type discussed above. The output of the modulated oscillator 83 is connected to the control grid electrode of the mixer tube 5l'.
It will be noted that the modulated intermediate frequency currents from the oscillator 83 are combined in the mixer tube 5l With the locally generated oscillations of the receiver. The plate circuit of the mixer tube 5l, therefore, includes sum and difference components. If the oscillator is operating above the signal frequency to produce the receiver intermediate frequency, then the difference component appearing in the plate circuit Will necessarily be equal to the signal frequency to which the receiver will respond for the given setting of the oscillator. If the oscillator is operating below the signal frequency, as is the case in said receivers in high frequency bands, the sum component will then be equal to the signal frequency to which the receiver Will respond for the particular oscillator frequency. Thus if the signal frequency circuits 0f the receiver are adjusted to the signal frequency component produced in the output of the mixer tube, and this throughout the entire operating range of the receiver, the desired alignment and tracking Will have been achieved.
The actual alignment of the receiver is conventional, and need not be described in detail. By setting the tuning knob 8l to the desired aligning point, the frequency of the local oscillator is first adjusted and then the signal frequency circuits are adjusted until their resonant peaks, illustrated in Fig. '7, fall upon the vertical line fu which corresponds to the signal frequency. For the sake of simplicity, only one curve for each resonant circuit has been indicated in Fig. 7 but it is to be understood that the double system similar to that illustrated in Fig. 3 may also be used.
Having completed the alignment of the receiver in the preselected points, the tracking of the two signal frequency circuits is determined by slowly rotating the tuning knob 3l throughout its entire range. Since the signal frequency itself is varied, since it is derived from the local oscillator, the center line fo on the cathode ray screen represents the correct frequency at all points. Consequently, the degree and direction of the deviation of the antenna and amplifier circuits are instantly observed. If the receiver has been improperly aligned this fact may be immediately determined, since in that case the signal frequency circuits Will not track properly and will deviate Widely from the normal frequency fo. Normal deviations may be marked directly on the cathode ray screen so that the operator may check the accuracy of the alignment in a minimum of time.
I claim as my invention:
1. In a device having a plurality of circuits tunable over a range of frequencies in response to common control means, the method of indicating the alignment of said circuits throughout their tuning range which includes the steps of generating a radio frequency voltage the nominal frequency of which is variable over said range of frequencies, modulating the frequency of said radio frequency voltage throughout a range less than said range of frequencies, applying said frequency modulated voltage to said resonant circuits, producing separate indications of the resonant rise of voltage in said circuits, and simultaneously varying the nominal frequency of said frequency modulated voltage and the resonant frequency of said circuits, the difference between said indications being a measure of the alignment of said circuits.
2. In a device having a plurality of resonant circuits tunable over a range of frequencies in response to a common control means, the method of indicating the alignment of said circuits which includes the steps of generating a radio frequency Voltage the nominal frequency of which is variable over a range of frequencies, modulating the frequency of said voltage at a constant rate throughout a range less than said range of frequencies, applying said frequency modulated voltage to said resonant circuits, producing separate indications of the resonant rise of voltage in said circuits, and simultaneously varying the resonant frequency of said circuits and the nomiynal frequency of said radio frequency voltage through similar frequency ranges to indicate the relative alignment of said circuits throughout their operating range.
3. In a radio device having a plurality of resonant circuits tunable over a range of frequencies in response to a common control means, the method of indicating the relative resonant frequencies of said circuits throughout said range which includes the steps of generating an alternating voltage the nominal frequency of which is variable over a range in response to said common control means, modulating the frequency of said voltage above and below said nominal frequency s at a constant rate, applying said modulated voltage simultaneously to said resonant circuits, adjusting the nominal frequency of said voltage to a value substantially equal to the resonant frequency of said circuits at a given point in said range, indicating the resonant rise of voltage of said Ycircuits at said point, and operating said control means to tune said circuits throughout said range, While correspondingly varying the nominal frequency of said alternating voltage.
4. In a radio device having a plurality of resonant circuits tunable over a range of frequencies in response to a common control means, the method of indicating the relative resonant frequencies of said circuits throughout said range which includes the steps of generating an alternating voltage the nominal frequency of which is variable over a range corresponding to the range covered by said tunable circuits, cyclically modulating the frequency of said Voltage, impressing said modulated voltage simultaneously on said resonant circuits, adjusting the nominal frequency of said voltage to a value substantially equal to the resonant frequency of said circuits at a given point in said range, indicating the resonant rise of voltage of said circuits at said point, and operating said control means to tune said circuits throughout said range while correspondingly varying the nominal frequency of said voltage.
5. In a device having a plurality of circuits tunable over a range of frequencies in response to common control means, the method of indicating the tracking of said circuits which includes the steps of generating an alternating voltage, cyclically varying the frequency of said voltage over a range of frequencies less than the tunable range of said circuits, applying said cyclically varying voltage to said circuits, producing indications of the resonant rise of voltage in said circuits, and simultaneously varying the average frequency of said alternating voltage and the resonant frequency of said circuits throughout said range, the difference between said indications at any point being an indication of the tracking of said circuits.
6. In a device having a plurality of resonant circuits tunable over a range of frequencies in response -to common controlA means, the method of indicating the tracking of said circuits which includes the steps of generating an alternating voltage whose frequency is also variable over said range of frequencies in response to said common control means, cyclically varying the frequency of said voltage over a range of frequencies inclusive of the range covered by the resonance curve of said tunable circuits, applying said Voltage to said tunable circuits, Visually and separately indicating the resonant rise of voltage vs. frequency characteristic of said tunable circuits, and operating said common control means to vary the resonant frequency of said circuits and the frequency of said voltage throughout said range, the difference between said indications being a measure of the error in tracking of said circuits.
'7. In a device having a plurality of resonant circuits tunable over a range of frequencies in response to common control means, the method of indicating the tracking of said circuits which includes the steps of generating an alternating voltage whose average frequency is tunable over said range in response to said common control means, separately varying the frequency of said voltage over a range of frequencies which includes the range covered by the resonance curve of said tunable circuits, applying said voltage to said circuits, deriving output voltages from said resonant circuits, commutating said voltages, producing a beam of electrons, deflecting said beam in a first direction in accordance with said commutated voltages, deflecting said beam in a second direction in synchronism with the cyclic varia-tion of the frequency of said voltage, utilizing said beam to produce luminous traces of the resonance characteristic of said circuits, and simultaneously varying the average frequency of said voltage and the resonant frequencies of said tunable circuits throughout said range, the distance between the peaks of said traces being an indication of the tracking of said circuits.
8. In a device having a plurality of resonant circuits tunable over a rst range of frequencies in response to common control means, the method of determining the tracking of said circuits which includes the steps of generating an alternating voltage whose nominal frequency is variable over said first range of frequencies, cyclically modulating the frequency of said voltage throughout a second range smaller than said rst range, applying said modulated Voltage to said circuits, deriving output voltages from said circuits, producing a beam of electrons, deflecting said beam in a first direction alternately and successively in accordance with said output voltages, deflecting said beam in a second direction in synchronism with the cyclic modulation of said alternating voltage, utilizing said beam to produce traces representing the resonance characteristic of said circuits, tuning said circuits over said first range of frequencies While simultaneously varying the nominal frequency of said alternating voltage over the same range of frequencies, the distance between the peaks of said traces at any point being a measure of the tracking of said circuits at that point.
9. In a superheterodyne receiver having a local oscillator tunable over a iirst range of frequencies and a resonant circuit simultaneously tunable over a second range of frequencies displaced from saidrrst range' by a fixed interme d-iate frequency, the method of checking the tracking between saidl tunable circuit and said oscillator Which includes the steps `of generating an alternating voltage of said intermediate frequency, combining said voltage with oscillations produced by said local oscillator to produce a signal-frequency voltage, applying said vsignalfrequencyvvoltage to said resonant circuit, and indicating the deviation of the resonant frequency of said circuit from the frequency of said signal frequency voltage.
10. In a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit and common means for tuning said oscillator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency, the method of checking the tracking of said oscillator and said signal frequency circuit which includes the steps of generating intermediate frequency oscillations, combining said intermediate frequency oscillations with oscillations produced by said local oscillator to produce signal frequency oscillations, applying said signal frequency oscillations to said signal frequency circuit, and indicating the deviation of the resonant frequency of said circuit from said signal frequency.
11. In a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit, and common means for tuning said oscil lator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency, the method of checking the tracking of said oscillator and said circuit which includes the steps of generating a current of said intermediate frequency, combining said current with currents of said oscillator frequency to produce signal frequency currents, applying said signal frequency currents to said circuit, and indicating the deviation of the resonant frequency of said circuit from said signal frequency.
12. In a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit, and common means for tuning said oscillator and said circuit throughout frequency ranges Which differ by a substantially constant intermediate frequency, the method of checking the tracking of said oscillator and said circuit which includes the steps of generating a frequency modulated current the average frequency of which is equal to said intermediate frequency, combining said current With currents of said oscillator frequency to produce signal frequency currents, applying said signal frequency currents to a circuit, and visually indicating the deviation of the resonant frequency of said circuit as said oscillator and said circuit are tuned throughout their respective ranges.
13. In a superheterodyne receiver having a variable frequency oscillator, a signal frequency circuit, and common means for tuning said oscillator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency, the method of checking the tracking of said oscillator and said circuit which includes the steps of generating a frequency modulated current the average frequency of which is equal to said intermediate frequency, combining said currents with other currents of said oscillator frequency to produce frequency modulated signal frequency currents, applying said signal frequency currents to said circuit, deriving rectified output currents proportional to the resonant rise -in voltage in said circuit, and utilizing'said output currents to indicate visually the deviation of the resonant frequency of saidvcircuit from said signal frequency as said oscillator Vand said circuit. are tuned throughout their respective ranges.
' l14. The method of determining the alignment of a superheterodyne receiver having a variable frequency local oscillator, at least one signal frequency circuit and means for simultaneously tuning said oscillator and said circuit throughout frequency ranges which differ by a substantially constant intermediate frequency, Which includes the steps of generating a current of said intermediate frequency, modulating the frequency of said current throughout a range of the order of the bandwidth of said circuit, combining said modulated intermediate frequency current with oscillatory currents from said local oscillator to produce frequency modulated signal frequency currents, applying said signal frequency currents to said signal frequency circuit, deriving rectified output currents from said circuit and utilizing said output currents to produce a trace corresponding to the resonance curve of said circuit, the deviation of the resonant frequency of said circuit from the average frequency of said signal frequency currents being a measure of the tracking of said circuit.
l5. A device for indicating the alignment of a superheterodyne receiver having a Variable frequency local oscillator and at least one tuned signal frequency circuit, said receiver also having common means for tuning said oscillator and said circuit throughout frequency ranges which differ by a substanti-ally constant intermediate frequency, comprising in combination means for producing a frequency modulated current of said intermediate frequency, means for combining said current with current from said local oscillator to produce modulated combination currents of signal frequency, means for applying said signal frequency currents to said circuit, and means for indicating the difference between the average frequency of said modulated signal frequency currents and the resonant frequency of said circuit.
16. A device for indicating the alignment of a receiver having a pair of tunable signal frequency circuits which includes, in combination, means for producing a frequency-modulated current of said signal frequency, means for applying said signal frequency currents to said circuits, means for simultaneously varying the resonant frequency of said tunable circuits and the average frequency of said signal frequency currents, and means for indicating the deviation of the resonant frequency of said circuits from the average frequency of said signal frequency currents.
17. A device for indicating the alignment of a superheterodyne receiver having a pair of tunable signal frequency circuits and a tunable local oscillator which includes, in combination, means including said local oscillator for producing a frequency-modulated signal frequency current,
the average frequency of which is determined by the frequency of said local oscillator, means for applying said signal frequency current to said tunable circuits, means for simultaneously varying the resonant frequency of said circuits and the frequency of said oscillator, and means for indicating the deviation of the resonant frequency of said circuits from the average frequency of said signal frequency currents at desired points Within the tuning range of said circuits.
18. A device for indicatingv the alignment of a superheterodyne receiver having a pair of tunable sign-a1 frequency circuits and a tunable local oscillator which includes, in combination, an intermediate frequency oscillatorgvmeans for periodi--v cally varying the frequency of said oscillator, means for combining currents from said intermediate frequency oscillator With currents from said local oscillator to produce a frequency modulated signal frequency current, means for ap- 10
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Cited By (27)

* Cited by examiner, † Cited by third party
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US2419527A (en) * 1943-02-27 1947-04-29 Gen Electric Radio frequency transmitter monitoring system and method
US2449621A (en) * 1942-09-30 1948-09-21 Rca Corp Comparison of radio frequency circuit losses
US2471432A (en) * 1944-08-11 1949-05-31 Lewis F Jaggi Wavemeter to calibrate panoramic receivers
US2471530A (en) * 1945-09-12 1949-05-31 Air King Products Company Inc System for comparing synchronized wave signals
US2495997A (en) * 1944-10-31 1950-01-31 Philco Corp Radio receiver aligning apparatus and method
US2510074A (en) * 1946-05-14 1950-06-06 Int Standard Electric Corp Display arrangement for electric oscillographs
US2525675A (en) * 1946-05-07 1950-10-10 Panoramic Radio Corp Signal comparing system
US2567587A (en) * 1945-12-10 1951-09-11 Zigmond W Wilchinsky Method and apparatus for measuring capacitance
US2574470A (en) * 1946-03-01 1951-11-13 William J Finney Frequency determination
US2580968A (en) * 1945-11-28 1952-01-01 Rca Corp Method of and means for measuring microwave frequencies
US2582247A (en) * 1945-10-16 1952-01-15 Jr Hunter C Goodrich Standard impulse noise generator
US2614153A (en) * 1948-05-18 1952-10-14 Tesla Nat Corp Method of and device for measuring and controlling the quality factor and damping factor of electric circuits and components thereof
US2649570A (en) * 1950-06-29 1953-08-18 Bell Telephone Labor Inc Test equipment and method for measuring reflection coefficient
US2671198A (en) * 1951-04-12 1954-03-02 Sperry Corp Method and apparatus for measuring the frequency response of translating devices
US2691098A (en) * 1945-12-14 1954-10-05 Selove Walter Automatic noise figure meter
US2714657A (en) * 1945-09-14 1955-08-02 James H Stein Apparatus for obtaining r.-f. response curves
US2744247A (en) * 1950-01-24 1956-05-01 Padevco Inc System for deriving the modulation of one frequency modulated wave in the presence of another co-channel frequency modulated wave
DE946351C (en) * 1952-09-11 1956-08-02 Max Grundig Circuit arrangement for examining the frequency response of television receivers using a wobble oscilloscope
US2774034A (en) * 1945-12-11 1956-12-11 Louis B Young Frequency comparator
US2778993A (en) * 1945-12-10 1957-01-22 Louis B Young Impedance bridge
US2978655A (en) * 1957-10-01 1961-04-04 Rca Corp Automatic alignment system
US2978646A (en) * 1957-08-21 1961-04-04 Rca Corp Automatic alignment system
US2991436A (en) * 1958-09-11 1961-07-04 Western Electric Co Adjustment of frequency sensitive transmission networks
US3002089A (en) * 1944-09-16 1961-09-26 Itt Method and apparatus for accurate comparison of frequencies
US3051896A (en) * 1958-05-06 1962-08-28 Rca Corp Frequency detector
US3210656A (en) * 1960-03-07 1965-10-05 Lear Siegler Inc Swept frequency circuit testing system
US3622889A (en) * 1969-08-29 1971-11-23 Standard Kollsman Ind Inc Bandpass response display

Cited By (27)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2449621A (en) * 1942-09-30 1948-09-21 Rca Corp Comparison of radio frequency circuit losses
US2419527A (en) * 1943-02-27 1947-04-29 Gen Electric Radio frequency transmitter monitoring system and method
US2471432A (en) * 1944-08-11 1949-05-31 Lewis F Jaggi Wavemeter to calibrate panoramic receivers
US3002089A (en) * 1944-09-16 1961-09-26 Itt Method and apparatus for accurate comparison of frequencies
US2495997A (en) * 1944-10-31 1950-01-31 Philco Corp Radio receiver aligning apparatus and method
US2471530A (en) * 1945-09-12 1949-05-31 Air King Products Company Inc System for comparing synchronized wave signals
US2714657A (en) * 1945-09-14 1955-08-02 James H Stein Apparatus for obtaining r.-f. response curves
US2582247A (en) * 1945-10-16 1952-01-15 Jr Hunter C Goodrich Standard impulse noise generator
US2580968A (en) * 1945-11-28 1952-01-01 Rca Corp Method of and means for measuring microwave frequencies
US2567587A (en) * 1945-12-10 1951-09-11 Zigmond W Wilchinsky Method and apparatus for measuring capacitance
US2778993A (en) * 1945-12-10 1957-01-22 Louis B Young Impedance bridge
US2774034A (en) * 1945-12-11 1956-12-11 Louis B Young Frequency comparator
US2691098A (en) * 1945-12-14 1954-10-05 Selove Walter Automatic noise figure meter
US2574470A (en) * 1946-03-01 1951-11-13 William J Finney Frequency determination
US2525675A (en) * 1946-05-07 1950-10-10 Panoramic Radio Corp Signal comparing system
US2510074A (en) * 1946-05-14 1950-06-06 Int Standard Electric Corp Display arrangement for electric oscillographs
US2614153A (en) * 1948-05-18 1952-10-14 Tesla Nat Corp Method of and device for measuring and controlling the quality factor and damping factor of electric circuits and components thereof
US2744247A (en) * 1950-01-24 1956-05-01 Padevco Inc System for deriving the modulation of one frequency modulated wave in the presence of another co-channel frequency modulated wave
US2649570A (en) * 1950-06-29 1953-08-18 Bell Telephone Labor Inc Test equipment and method for measuring reflection coefficient
US2671198A (en) * 1951-04-12 1954-03-02 Sperry Corp Method and apparatus for measuring the frequency response of translating devices
DE946351C (en) * 1952-09-11 1956-08-02 Max Grundig Circuit arrangement for examining the frequency response of television receivers using a wobble oscilloscope
US2978646A (en) * 1957-08-21 1961-04-04 Rca Corp Automatic alignment system
US2978655A (en) * 1957-10-01 1961-04-04 Rca Corp Automatic alignment system
US3051896A (en) * 1958-05-06 1962-08-28 Rca Corp Frequency detector
US2991436A (en) * 1958-09-11 1961-07-04 Western Electric Co Adjustment of frequency sensitive transmission networks
US3210656A (en) * 1960-03-07 1965-10-05 Lear Siegler Inc Swept frequency circuit testing system
US3622889A (en) * 1969-08-29 1971-11-23 Standard Kollsman Ind Inc Bandpass response display

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