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EDN Flashback: Self-contained TV receiver uses 24 transistors

This transistorized TV design, which appeared in the September 1958 issue of EDN, is an early example of what we today call the reference design.



EDN's 50th AnniversaryEditor's note: The article reproduced below appeared in the September 1958 issue of EDN. For present-day analysis, see "Milestones That Mattered: Reference designs matter, as this TV design illustrates."

Twenty-four transistors and one high-voltage rectifier tube perform all of the functions required to develop a high-definition picture and accompanying sound in a completely self-contained portable television receiver [Editor's note: Click here for a schematic (PDF, 1.2 Mbytes) ]. Power is furnished by a ten-cell nickel-cadmium battery providing 12 volts at 700 ma, average current. The picture tube employed in this receiver is a 9QP4 whose filament has been modified to operate at 12 volts with 150 ma.

Two tuners were developed for this receiver. The more sensitive one uses tetrode transistors in the RF amplifier, mixer and oscillator. Its disadvantages lie in a much higher cost and a 12 to 14 db noise figure. The second tuner uses two 2N623 diffused-base transistors in the mixer and oscillator stages, with no RF amplifier. Noise figure is 9 to 11 db, but overall tuner gain is only 10 to 12 db on channel 13. This compares with an overall tuner gain of 20 to 22 db (channel 13) for the tetrode tuner. Cost is considerably lower for this unit and is said to compare favorably with current vacuum-tube tuners.

There are five grounded-base amplifier stages in the video IF system. All of the tuned circuits, with the exception of the one between the third and fourth stages, are synchronous tuned to 44.5 mc. The remaining circuit is double tuned and overcoupled in order to provide a flat top for the IF response curve. AGC is applied to the first two stages from an AGC system that employs a peak detector and a d-c amplifier. Two IN295 diodes in the emitter circuits of the first two stages serve to maintain input circuit loading constant as AGC voltage drives transistors to cutoff under strong signal conditions. Effectiveness of this control system is seen by the fact that 70 db power range at input results in only a 10 db variation at output of video detector. Overall video IF gain is 75 db. The remaining portion of the video system is straightforward, containing a diode detector and two high-frequency video transistor stages.

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Beyond the video system, the sound and sync signals follow their normal paths. Of particular interest are the vertical and horizontal output circuits. In the vertical system, a low-resistance 470-mh choke is shunted across the vertical deflection windings of the yoke in order to minimize the off-centering effect produced by the d-c current in this circuit. In the horizontal system, voltages are developed to drive the picture tube and the video amplifiers during beam retrace. With a 9QP4 picture tube, 6,500 volts proved sufficient to develop a satisfactory level of screen brightness.

This receiver was developed by Roger Webster and Harry Cooke of the Circuit Development branch of Texas Instruments Incorporated, Dallas, Tex. The purpose of this work was to determine the feasibility of designing a transistorized television receiver using Texas Instrument units. There is no intent by this firm to manufacture such receivers.

Circuit diagram of complete receiver

Editor's note: Click here for a schematic�(PDF, 1.2 Mbytes)�.

Triode transistor tuner must be operated with low side injection of oscillator frequency on high channels because of cutoff frequency of 2N623 diffused-base transistors. In alternate tetrode tuner, high side injection can be employed on all channels. Oscillator in triode tuner must provide 300 �watts to mixer; in tetrode tuner, only 40 to 60 �watts needed. Due to use of triode tuner, video IF response curve made symmetrical. 45.25 mc point is 5 db down from top while 41.25 mc is 20-22 db down. Without traps, adjacent channel sound and video rejection down about same extent as 41.25 mc. Capacitive neutralization is employed on all video IF stages. In first two stages, the 3.9 MMF capacitors are selected for minimum forward transmission of signal at maximum AGC. Remaining neutralizing capacitors are chosen for maximum neutralization. In the last video IF stage, two 50 MF capacitors serve to maintain the operating point of stage at modulation peaks because this stage does not operate strictly class A. Most of the circuit is not critical with respect to transistor replacement.

However, it is probable that replacement of 4th IF transistor would require readjustment of double tuned coupling circuit.

In the video detector, a small d-c bias voltage is applied to the cathode of the IN295 to maintain rectifying linearity at low signal levels. Maximum video signal made available to first video amplifier from detector is 3v P-P. However, maximum voltage fed to 9QP4 cathode if 40v P-P, limited by 48 volt d-c potential of output video amplifier. Maximum voltage gain of video amplifier section is 40 with a 3-mc passband. Contrast is controlled by 2,500-ohm potentiometer in emitter circuit of 2nd video amplifier in accordance with conventional practice.

The sound system is straightforward, with two 4.5-mc IF amplifiers, one of which serves as a reflex audio amplifier, a ratio detector, a 2N185 driver and a push-pull, class-B audio output stage. A series resonant 4.5-mc circuit links the emitter of the first video amplifier with the first sound IF stage. Input impedance of the sound amplifier is 300 ohms and the series resonant circuit enables this to match the emitter circuit impedance of the video amplifier. D5 serves as an AM limiter by clipping negative segment of signal at collector of 1st sound IF. Tuned circuit then acts to smooth out the positive half of signal to same level.

Sync pulse positive signal is applied to X11 from the first video amplifier. 0.7 volt P-P will drive this transistor from cutoff to saturation. X12 then serves as a sync amplifier for vertical pulses and an emitter follower for the horizontal deflection system. For the vertical pulses, the 1,000-ohm resistor and 0.1 MF capacitor between X12 and X13 provide the major portion of integration with additional integration occurring in the emitter of X13.

The vertical deflection system requires only two stages, a blocking oscillator and an alloy junction vertical output amplifier. The sawtooth deflection wave is developed across C1 and C2 in series, and then passed on to X15. C2 is also part of a feedback network from the emitter of X15 to improve the linearity of the deflection waveform. Separate vertical linearity and vertical size controls are available, but being part of the same network, tend to be interdependent in adjustment, together with the bias control. The latter potentiometer sets the operating current for the vertical output amplifier.

In the horizontal system, negative-going sync pulses from X12 are compared with a sawtooth wave developed from voltage pulses obtained from the output circuit of X24. The resulting d-c potential is then passed through a long time-constant filter, (.01 and .02 MF capacitors and 2.2K resistor) and anti-hunt network (1.5K resistor and 5 MF capacitor) to a blocking oscillator through a d-c amplifier. The driving signal fed to X23 is a square wave pulse. However, due to the inductive coupling, the a-c axis of this pulse provides enough forward bias to drive the transistor to saturation during conduction, while the positive-going pulse sharply cuts X23 off during retrace. A similar situation exists in the input circuit of X24, with a variable 50-ohm potentiometer in the base circuit to limit the d-c power consumption of the transistor.

The peak voltage developed across T6 during beam retrace is kept at about 80v by adjusting the self-resonant frequency of the secondary of this high-voltage transformer to approximately 100 kc. Without this adjustment, the voltage peak would rise to 110v and place an extra burden on transistor selection. Peak emitter current in X24 just prior to start of retrace is two amps.

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