US2272066A - Ultra short wave system - Google Patents

Description

H. *0. PETERSON ULTRA SHORT WAVE SYSTEM Filed March C50, 1959 T0 FREQUENCY MEASUR/NG 5E T 0S C/LLA TOR FILTER BOX VOLTAGE REGULATOR 7 INVEN TOR. O. PETERSON v HAR LD BY Wmm/ ATTORNEY.

patented Feb. 3, 1942 ULTRA snoer WAVE sxzs'rEMv Harold 0. Peterson, Riverhead, N. Y., assigner to Radio Corporation of America,.a corporation of Delaware Application March 30, 1939, Serial No. 264,904

9 Claims.

This invention relates to ultra. 'short radio wave systems, and particularly to nove'l constructional arrangements therefor.

One of the objects of the present invention is to provide .an ultra short wave radio receiving system wherein all stages are thoroughly shielded from one another, and wherein al1 parts are easily accessible from the front panel without obstruction due to the presence of the shielding partition. s

Another object is to provide a highly efficient link circuit for magnetically coupling together two couplings coils of two tuned circuits. More specifically, it is an object to provide pure magnetic coupling between'two circuits by means of a high Q transfer or link circuit which is devoid of the usual capacitance present in customary types of link circuits.

A description of the invention follows in conjunction with a. drawing, whose single figure shows an ultra high frequency receiver and frequency measuring system. Although the invention is particularly described in connection with va frequency measuring System, it should be. clearly understood that the novel features thereof. are not limited either to a measuring system or to a receiver, but maybe employed wherever there is' need for the advantages provided by the circuits of the invention.

Referring to the drawing in more detail, there is shown an ultra high frequency receiver comprising first and second radio frequency amplifier stages I and 2, respectively, a regenerative detector '3, a local oscillator l, and an audio frequency amplifier 5, all of which are appropriately labeled. There is also provided a known type .of B supply voltage regulator 1 modified in a manner described hereinafter. The entire receiver is mounted within a grounded metallic container 8 which is divided into shielded compartments by means of metallic partitions 9, as shown.

The vacuum tubes of stages I and 2 comprise suitable acorn tubes II), each of which is supported and mounted in the shielding compartment between these stages in such manner that the input circuit is isolated from the output circuit, as shown. Thus, the input circuit to the first radio freq"ency amplifier I comprises a parallel tuned circuit II suitably coupled to a source of oscillations I2 located on the opposite side of one of the shielding walls 9 while the output circuit of amplifier stage I comprises a parallel tuned circuit I3 coupled not only to the anode oi the rst tube I0 but also coupled to the control grid of the second radio frequency stage.

The output circuit of the second radio frequency amplifier 2 comprises a parallel tuned circuit I4 which constitutes the operating circuit of the 5 detector stage 3. From an inspection of the drawing, it will be obvious that circuit II, which is in one shielded compartment, is isolated from circuit I3, both of which in turn are isolated from circuit I4. The suppressor grids, the l0 cathode and one side of the filament of each of the two amplifier tubes I0 vare grounded, while the screen grids of these tubes are by-passed to ground through a suitable condenser I5, as shown.

The regenerative detector stage 3 comprises a vacuum tube to whose grid and cathode electrodes is coupled a parallel tuned circuit Il. The inductance of circuit Il is of the plug-in coil type and is coupled to one side of a link or 20 transfer circrit I6 to whose other side is coupled the inductance coil I1 of the local oscillatorV stage l. By means of choke coils 20 in the detector circuit, and the resistances 2l -in series therewith which prevent parasitic oscillations at i5 frequencies determined by the inductances of the chokes, I have been able to provide a regenerative detector which requires only two terminals on the tuning inductance of the circuit Il.

The local oscillator 6 very generally follows 39 the known type of three point Hartley oscillator,

wherein the grid and anode are coupled to opposite sides of the inductance while the cathode is coupled to an intermediate point on the inductance. This oscillator may be energized at '3" will by means of a plate supply switch 26 for purposes of calibration and frequency measurement. The link circuit I6 comprises a single turn loop mounted on and supported by the partition between the detector stage 3 and the oscillator l,

m such that one-half of the loop is coupled to tuned circuit I4 while the other half of the loop is coupled to coil I1, as shown. It should be noted that the single turn loop I6 is dividedinto two 4r halves by means of the grounded partition 9, and that the both halves of the loop I6 are conneced together at one point and to the grounded partition 9 at the binding post I8, while the other ends of the halves are integral and connected together through a small hole I9 inthe partition 9 from which they are insulated, The link circuit I6 thus provides a highly efficient low loss (high` Q) pure magnetic coupling transfer circuit between the detector and the oscillator. The

, degree of coupling depends upon the spacing between the link circuit I6 and the circuits Il and wires between coupling loops; thus my link circuit may very efficiently transfer energy over a particular band of frequencies more efficiently than is possible by known types of transferl circuits.

The audio frequency amplifier 5 comprises three vacuum tubes, each of the ARCA 6-F-5 type, the first stage of which is coupled to the anode of regenerative detector 3 while the last stage is coupled to the audio frequency transformer 22, in turn coupled to a suitable output circuit, here shown as a pair of jacks to which a loud speaker or telephone head-set may be coupled.

The B supply voltage regulator is an electronic type for stabilizing all of the B supply voltages and is similar to the circuit used in the type 'I'MV-118B regulated power supply unit manufactured by the RCA Manufacturing Co., Inc., except for the use of an RCA type SLG beam power tube instead of the usual RCA type 2A3 type. It should be noted that there is added a small 0.02 mf. condenser 23 in shunt of the 50,000 ohm resistor 24 from the grid of the RCA type 77 tube to ground, in order to prevent 'a parasitic type of oscillation which sometimes occurs at s'uper audible frequencies.

In order to cover a wide frequency range, the inductances of tuned circuits II, I3 and Il may be of the plug-in coil type. With a circuit of this type actually tried out in practice the receiver was built to cover a frequency range from 22 to 150 megacycles.

For achieving ready access to all of the tuned circuits without obstruction by the presence of the shielding compartments when the front panel of the receiving unit is removed, it is proposed to build the tuned circuits II, I3, Il and I'I on submountlngs attached to the front panel, and to couple the screen, cathode and heater supply leads to the tubes by means of clips which are built on the partitions of the shielding boxes. In this way the heater and screen voltages may. be brought to the vacuum tube terminals through grounded metal ducts 25 which are bonded to the partitions of the box l. It will thus be appreciated that the vacuum tube mounting is in fact a part of the shielding box. For removing the front panel and associated radio frequency circuits, it is only necessary to unclamp the plate and grid leads from the amplifier vacuum tubes I 0 in order to allow these tubes to remain in their places in the shielding partitions.

In order to measure the frequency of any signal heard with this type of receiver, the oscillator 4 is adjusted so that a harmonic from it has the same frequency as the incoming signal by observing the condition of zero beat in the receiver output. The tuning of the detector circuit 3 is approximately calibrated in terms of dial reading and frequency, and the oscillator circuit is quite accurately calibrated in terms of dial reading and frequency. From these calibrations, it is readily possible to determine which harmonic of the oscillator 4 is beating against the signal to give zero beat. An output connection is provided in the oscillator shielded compartment whereby the oscillator frequency can be transferred to one of the constant frequency measuring sets, not shown, and the oscillator frequency thus very accurately measured. The signal frequency is thereby accurately determined since it is only necessary now to multiply the exact frequency of the oscillator 4 by the order of the harmonic of the oscillator which is being used to beat against the signal.

What is claimed is:

l. The combination with a rst inductance coil located in a shielded compartment and a second inductance coil located in an adjacent shielded compartment, there being a shielding partition between said compartments. of a link circuit comprising a single turn coil one-half of which is located in the same compartment as said first` coil and coupled thereto and the other half of which is located in the same compartment as said second coil and coupled thereto, said halves being separated by said partition and connected together through a hole therein.

2. The combination with a first inductance coil located in a shielded compartment and a second inductance coil located in an adjacent shielded compartment, there being a shielding partition between said compartments, of a link circuit comprising a single turn coil one-half of which is located in the same compartment as said first coil and coupled thereto and the other half of which is located in the same compartment as said second coil and coupled theret-o, one end of one half of said single turn coil and the correspondingly located end of said other half of said single turn coil being connected to said partition, the other ends of said halves being connected together through a hole in said partition from which they are insulated.

3. An energy transfer circuit for magnetically coupling together two circuits separated by a shielding wall, comprising a single turn coil having parallel elements on opposite sides of said wall, one of said parallel elements being coupled to one of said circuits while the other of said parallel elements is coupled to the other of said circuits.

4. An energy coupling circuit for magnetically coupling together two circuits separated by a shielding partition, comprising a fraction of a coil located on one side of said partition and coupled to one of said circuits, and a fraction of a coil located on the other side of said partition and coupled to the other circuit, one end of one of said fractions and the correspondingly located end of the other fraction being connected to said partition, the other ends of said fractions being connected together through a hole in said partition.

5. An energy coupling circuit for `magnetically coupling together two circuits separeted by a shielding partition, comprising a fraction of a coil located on one side of said partition and coupled to one of said circuits, and a fraction of a coil located on the other` side of said partition and coupled to the other circuit, one end of one of said fractions and an end of the other fraction being connected to said partition, the other ends of said fractions being connected together through a hole in said partition.

6. An energy transfer circuit for magnetically coupling together two circuits separated by a shielding wall, comprising a single turn coil having parallel elements on opposite sides of and parallel to said Wall, one of said parallel elements being coupled to one of said circuits While the other of said parallel elements is coupled to vthe other of said circuits.

'7. Coupling apparatus comprising a, pair of wire elements connected together to form a sin- 'gle turn loop, and a shielding surface located between said wire elements.

8. Coupling apparatus comprising a pair of parallel Wire elements connected together to form HAROLD O. PETERSON.

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