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T EVIS i - AmericanRadioHistory.Com

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Fig. 3. The grid -dip meter. Top<br />

portion may serve as a wavemster.<br />

it is used as the tank circuit of an oscillator.<br />

This provides more than adequate<br />

range to cover the less than 2:1 frequency<br />

range required by the new 470-<br />

890 mc. u.h.f. band.<br />

Inductance of the cavity is varied by<br />

rotating a brass fin in the cavity field.<br />

This fin acts as a shorted turn and represents<br />

a convenient way of trimming<br />

the inductance of the tuned circuit.<br />

The practicability of this device lay<br />

in the ability to manufacture the dielectric<br />

sleeve with sufficient accuracy.<br />

Should the plunger have lateral motion<br />

in the dielectric once its position is set,<br />

the unit would be susceptible to micro -<br />

phonics and backlash, thus proving<br />

quite unsatisfactory for use in a u.h.f.<br />

tuning element. Production techniques<br />

for realizing almost unheard of accuracies<br />

have been developed exclusively for<br />

this application, making the device commercially<br />

feasible at a reasonable cost.<br />

Advantages<br />

The question now arises as to why<br />

this particular arrangement was finally<br />

chosen as the ideal u.h.f. tuning element<br />

for the new band of frequencies.<br />

Most important is (1) that the construction<br />

is simple, and the severe close<br />

tolerances required by u.h.f. are easily<br />

held. Then, (2) there are no moving<br />

electrical contacts. This results in a<br />

long, noise -free life, with no contact<br />

finger or plunger wiper wear. The fact<br />

Fig. 5.<br />

Diagram of sweep generator.<br />

that there are no moving electrical contacts<br />

also results in a considerably<br />

higher Q tuning element than would<br />

otherwise be possible.<br />

Extremely high Q's are attainable<br />

using this configuration (3) ; Q's of<br />

1000 or more have been achieved. The<br />

use of high Q circuits for the tuner element<br />

insures low noise figure and high<br />

gain. Also, trimming and padding of<br />

the unit is easily achieved (4), thus assuring<br />

three -point tracking.<br />

Rigid construction (5) assures excellent<br />

frequency stability. As a matter of<br />

fact, the unit lends itself admirably to<br />

virtual self -compensation of thermal<br />

drift. The completely shielded construction<br />

makes the unit independent of its<br />

environment (6) since its field is internal;<br />

and outside motion, such as<br />

hand capacitance, has practically no<br />

effect on resonant frequency. This construction<br />

also keeps radiation from the<br />

tuning element to a minimum.<br />

The reasons given above were all considered<br />

important in arriving at the<br />

choice of a tuning element. There is,<br />

however, another very important reason<br />

for its choice which is (7) that the<br />

Flq. 4. Capacitance tuning of cavity.<br />

whole unit lends itself admirably as a<br />

generic element for a line of u.h.f. test<br />

equipment.<br />

The following u.h.f. equipment is required<br />

in a well- equipped laboratory<br />

working to develop u.h.f. television receivers<br />

and associated products:<br />

1. Signal generator<br />

2. Sweep generator<br />

3. Wavemeter<br />

4. Grid -dip meter<br />

5. <strong>Com</strong>posite picture, sound and sync<br />

signal generator<br />

These instruments have recently been<br />

developed by Granco Products Inc. to<br />

fill its own growing need for laboratory<br />

and production instruments in the development<br />

and production of u.h.f. television<br />

products. The top unit in Fig. 3<br />

shows the wavemeter design using the<br />

tuning element described. A small plug -<br />

in coupling loop is brought out at one end<br />

of the "cavity" for use as a probe. The<br />

signal is rectified by a 1N72 crystal and<br />

the detected current read on a compact<br />

meter conveniently mounted in the end<br />

of the instrument. Provision is also<br />

made to plug in a more sensitive meter<br />

when required. Because of the high Q<br />

of the cavity, this wavemeter is unusually<br />

sensitive, and extremely weak<br />

signals can be detected with negligible<br />

reaction on the circuit under observation.<br />

The instrument as presently constituted<br />

has a 13" dial scale with accurate<br />

individual calibration from 380 to<br />

1000 mc. This unit is particularly useful<br />

in the design of any oscillator both<br />

as a wavemeter and relative power output<br />

meter. It can be used in the latter<br />

function by being placed in a fixed position<br />

relative to the circuit under test,<br />

making the meter reading a function of<br />

the power output of the oscillator.<br />

By converting the wavemeter into an<br />

oscillator, capable of either external or<br />

internal amplitude modulation, the versatile<br />

grid -dip meter (shown in Fig. 3)<br />

was developed. A switch is provided to<br />

turn off the oscillator for operation similar<br />

to the wavemeter. The addition of<br />

the oscillator has greatly extended the<br />

instrument's utility. Because of the accurate<br />

frequency dial, high output and<br />

stable operation, it may be used as a<br />

compact u.h.f. signal source for numerous<br />

applications - for example, as a<br />

marker source when sweeping a television<br />

receiver, as a probe for detection of<br />

parasitics and in determining the self -<br />

resonant frequency of circuit components.<br />

Provision is also made for earphones<br />

or other types of detection facilities.<br />

The power cable to the oscillator has<br />

been so designed that it will plug<br />

directly into the power connector of<br />

the Measurements Corporation's popular<br />

megacycle meter, thus extending the<br />

range of this instrument from 400 mc.<br />

through 1000 mc.<br />

A small, compact sweep generator<br />

covering the u.h.f. television band, and<br />

having a sweep width of approximately<br />

±80 me., is shown in block diagram<br />

form in Fig. 5. This instrument uses a<br />

resonant cavity circuit mounted so that<br />

the cavity rides on a smooth rod, the<br />

position of which is controlled by the<br />

center frequency knob. As the cavity is<br />

moved, a plunger moves in to the cavity<br />

to change its frequency. This plunger<br />

(Continued on page 30)<br />

Fig. 6. Block diagram and waveforms<br />

for the picture signal generator.<br />

470 MINUS VN. F SIGNAL<br />

TO<br />

ego MINUS VHF SIGNAL<br />

CENTER FREQUENCY<br />

VARIABLE FROM 470 -890 MC.<br />

4MC.<br />

K<br />

;gg<br />

o<br />

I (t<br />

R A D I O - E L E C T R O N I C E N G I N E E R I N G APRIL 1953

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