The chassis is realized on a monocarrier completely based around discretes semiconductors.
All semiconductors circuits were made by:ates and PHILIPS.
SGS is Società Generale Semiconduttori - Aquila Tubi E Semiconduttori (SGS-ATES, "Semiconductor General Society - Tubes and Semiconductors Aquila"), later
SGS Microelettronica, a former Italian company now merged into STMicroelectronics
SGS
Microelettronica and Thomson Semiconducteurs were both
long-established semiconductor companies. SGS Microelettronica
originated in 1972 from a previous merger of two companies:
- ATES
(Aquila Tubi e Semiconduttori), a vacuum tube and semiconductor maker
headquartered in the Abruzzese city of l'Aquila, who in 1961 changed
its name into Azienda Tecnica ed Elettronica del Sud and relocated its manufacturing plant in the outskirts of the Sicilian city of Catania
- Società Generale Semiconduttori (founded in 1957 by Adriano Olivetti).
GENERAL BASIC TRANSISTOR LINE OUTPUT STAGE OPERATION:The
basic essentials of a transistor line output stage are shown in Fig.
1(a). They comprise: a line output transformer which provides the d.c.
feed to the line output transistor and serves mainly to generate the
high -voltage pulse from which the e.h.t. is derived, and also in
practice other supplies for various sections of the receiver; the line
output transistor and its parallel efficiency diode which form a
bidirectional switch; a tuning capacitor which resonates with the line
output transformer primary winding and the scan coils to determine the
flyback time; and the scan coils, with a series capacitor which provides
a d.c. block and also serves to provide slight integration of the
deflection current to compensate for the scan distortion that would
otherwise be present due to the use of flat screen, wide deflection
angle c.r.t.s. This basic circuit is widely used in small -screen
portable receivers with little elaboration - some use a pnp output
transistor however, with its collector connected to chassis.
Circuit Variations:
Variations
to the basic circuit commonly found include: transposition of the scan
coils and the correction capacitor; connection of the line output
transformer primary winding and its e.h.t. overwinding
in series; connection of the deflection components to a tap on the
transformer to obtain correct matching of the components and conditions
in the stage; use of a boost diode which operates in identical manner to
the arrangement used in valve line output stages, thereby increasing
the effective supply to the stage; omission of the efficiency diode
where the stage is operated from an h.t. line, the collector -base
junction of the line output transistor then providing the efficiency
diode action without, in doing so, producing scan distortion; addition
of inductors to provide linearity and width adjustment; use of a pair of
series -connected line output transistors in some large -screen colour
chassis; and in colour sets the addition of line convergence circuitry
which is normally connected in series between the line scan coils and
chassis. These variations on the basic circuit do not alter the basic
mode of operation however.
Resonance

The
most important fact to appreciate about the circuit is that when the
transistor and diode are cut off during the flyback period - when the
beam is being rapidly returned from the right-hand side of the screen to
the left-hand side the tuning capacitor together with the scan coils
and the primary winding of the line output transformer form a parallel
resonant circuit: the equivalent circuit is shown in Fig. 1(b). The line
output transformer primary winding and the tuning capacitor as drawn in
Fig. 1(a) may look like a series tuned circuit, but from the signal
point of view the end of the transformer primary winding connected to
the power supply is earthy, giving the equivalent arrangement shown in
Fig. 1(b).
The Flyback Period:
Since the operation of the
circuit depends mainly upon what happens during the line flyback period,
the simplest point at which to break into the scanning cycle is at the
end of the forward scan, i.e. with the

beam deflected to the right-hand side of the screen, see Fig. 2. At
this point the line output transistor is suddenly switched off by the
squarewave drive applied to its base. Prior to this action a linearly
increasing current has been flowing in the line output transformer
primary winding and the scan coils, and as a result magnetic fields have
been built up around these components. When the transistor is switched
off these fields collapse, maintaining a flow of current which rapidly
decays to zero and returns the beam to the centre of the screen. This
flow of current charges the tuning capacitor, and the voltage at A rises
to a high positive value - of the order of 1- 2k V in large -screen
sets, 200V in the case of mains/battery portable sets. The e

nergy
in the circuit is now stored in the tuning capacitor which next
discharges, reversing the flow of current in the circuit with the result
that the beam is rapidly deflected to the left-hand side of the screen -
see Fig. 3. When the tuning capacitor has discharged, the voltage at A
has fallen to zero and the circuit energy is once more stored in the
form of magnetic fields around the inductive components. One half -cycle
of oscillation has occurred, and the flyback is complete.
Energy Recovery:
First
Part of Forward Scan The circuit then tries to continue the cycle of
oscillation, i.e. the magnetic fields again collapse, maintaining a
current flow which this time would charge the tuning capacitor
negatively (upper plate). When the voltage at A reaches about -0.6V
however the efficiency diode becomes forward biased and switches on.
This damps the circuit, preventing further oscillation, but the magnetic
fields continue to collapse and in doing so produce a linearly decaying
current flow which provides the first part of the forward s

can,
the beam returning towards the centre of the screen - see Fig. 4. The
diode shorts out the tuning capacitor but the scan correction capacitor
charges during this period, its right-hand plate becoming positive with
respect to its left-hand plate, i.e. point A. Completion of Forward Scan
When the current falls to zero, the diode will switch off. Shortly
before this state of affairs is reached however the transistor is
switched on. In practice this is usually about a third of the way
through the scan. The squarewave applied to its base drives it rapidly
to saturation, clamping the vol

tage
at point A at a small positive value - the collector emitter saturation
voltage of the transistor. Current now flows via the transistor and the
primary winding of the line output transformer, the scan correction
capacitor discharges, and the resultant flow of current in the line scan
coils drives the beam to the right-hand side of the screen see Fig. 5.
Efficiency:
The
transistor is then cut off again, to give the flyback, and the cycle of
events recurs. The efficiency of the circuit is high since there is
negligible resistance present. Energy is fed into the circuit in the
form of the magnetic fields that build up when the output transistor is
switched on. This action connects the line output transformer primary
winding across the supply, and as a result a linearly increasing current
flows through it. Since the width is
dependent on the supply voltage, this must be stabilised.
Harmonic Tuning:
There
is another oscillatory action in the circuit during the flyback period.
The considerable leakage inductance between the primary and the e.h.t.
windings of the line output transformer, and the appreciable self
-capacitance present, form a tuned circuit which is shocked into
oscillation by the flyback pulse. Unless this oscillation is controlled,
it will continue into and modulate the scan. The technique used to
overcome this effect is to tune the leakage inductance and the
associated capacitance to an odd harmonic of the line flyback
oscillation frequency. By doing this the oscillatory actions present at
the beginning of the scan cancel. Either third or fifth harmonic tuning
is used. Third harmonic tuning also has the effect of increasing the
amplitude of the e.h.t. pulse, and is generally used where a half -wave
e.h.t. rectifier is employed. Fifth harmonic tuning results in a
flat-topped e.h.t. pulse, giving improved e.h.t. regulation, and is
generally used where an e.h.t. tripler is employed to produce the e.h.t.
The tuning is mainly built into the line output transformer, though an
external variable inductance is commonly found in colour chassis so that
the tuning can be adjusted. With a following post I will go into the
subject of modern TV line timebases in greater detail with other models
and technology shown here at Obsolete Technology Tellye !
- The EHT Output is realized with a selenium rectifier.
The EHT selenium rectifier which is a Specially designed selenium rectifiers were once widely used as EHT
rectifiers in television sets and photocopiers. A layer of selenium
was applied to a sheet of soft iron foil, and thousands of tiny discs
(typically 2mm diameter) were punched out of this and assembled as
"stacks" inside ceramic tubes. Rectifiers capable of supplying tens of
thousands of volts could be made this way. Their internal resistance
was extremely high, but most EHT applications only required a few
hundred microamps at most, so this was not normally an issue. With the
development of inexpensive high voltage silicon rectifiers, this
technology has fallen into disuse.

Power supply is realized with mains transformer and
Linear transistorized power supply stabilizer, A DC power supply
apparatus includes a rectifier circuit which rectifies an input
commercial AC voltage. The rectifier output voltage is smoothed in a
smoothing capacitor. Voltage stabilization is provided in the
stabilizing circuits by the use of Zener diode circuits to provide
biasing to control the collector-emitter paths of respective
transistors.A linear regulator circuit according to an embodiment of
the present invention has an input node receiving an unregulated
voltage and an output node providing a regulated voltage. The linear
regulator circuit includes a voltage regulator, a bias circuit, and a
current control device.
In one embodiment, the
current control device is implemented as an NPN bipolar junction
transistor (BJT) having a collector electrode forming the input node
of the linear regulator circuit, an emitter electrode coupled to the
input of the voltage regulator, and a base electrode coupled to the
second terminal of the bias circuit. A first capacitor may be coupled
between the input and reference terminals of the voltage regulator and
a second capacitor may be coupled between the output and reference
terminals of the voltage regulator. The voltage regulator may be
implemented as known to those skilled in the art, such as an LDO or
non-LDO 3-terminal regulator or the like.
The bias circuit may
include a bias device and a current source. The bias device has a
first terminal coupled to the output terminal of the voltage regulator
and a second terminal coupled to the control electrode of the current
control device. The current source has an input coupled to the first
current electrode of the current control device and an output coupled
to the second terminal of the bias device. A capacitor may be coupled
between the first and second terminals of the bias device.
In the
bias device and current source embodiment, the bias device may be
implemented as a Zener diode, one or more diodes coupled in series, at
least one light emitting diode, or any other bias device which develops
sufficient voltage while receiving current from the current source.
The current source may be implemented with a PNP BJT having its
collector electrode coupled to the second terminal of the bias device,
at least one first resistor having a first end coupled to the emitter
electrode of the PNP BJT and a second end, a Zener diode and a second
resistor. The Zener diode has an anode coupled to the base electrode
of the PNP BJT and a cathode coupled to the second end of the first
resistor. The second resistor has a first end coupled to the anode of
the Zener diode and a second end coupled to the reference terminal of
the voltage regulator. A second Zener diode may be included having an
anode coupled to the cathode of the first Zener diode and a cathode
coupled to the first current electrode of the current control device.

A
circuit is disclosed for improving operation of a linear regulator,
having an input terminal, an output terminal, and a reference terminal.
The circuit includes an input node, a transistor, a bias circuit, and
first and second capacitors. The transistor has a first current
electrode coupled to the input node, a second current electrode for
coupling to the input terminal of the linear regulator, and a control
electrode. The bias circuit has a first terminal for coupling to the
output terminal of the linear regulator and a second terminal coupled
to the control electrode of the transistor. The first capacitor is for
coupling between the input and reference terminals of the linear
regulator, and the second capacitor is for coupling between the output
and reference terminals of the linear regulator. The bias circuit
develops a voltage sufficient to drive the control terminal of the
transistor and to operate the linear regulator. The bias circuit may be
a battery, a bias device and a current source, a floating power
supply, a charge pump, or any combination thereof. The transistor may
be implemented as a BJT or FET or any other suitable current controlled
device.