resultant feedback signal from a frequency to voltage con-
Output signal from the oscillator is tapped across the
verter and ramp generator. Any differential between the
partial winding of L314 and capacitively coupled to trans-
two signals is a voltage output that controls the bias on
frequency-determining capacitance diode D314. D314 is part
up about 2:1 and converts the single-ended signal to a bal-
of the swept oscillator circuit which shifts the swept oscil-
anced push-pull drive signal for the output amplifier Q340
lator frequency by an amount proportional to the signal
and Q350.
output from the comparator.
Fig. 3-6 is a
simplified drawing of the
transformer circuit.
The oscillator is the signal source or generator which supplies
Q240 is the constant current source for the sweep com-
the signal voltage (e). The input windings of T330 and T331
parator. About 3.4 mA of current through the comparator
are connected in series; therefore, the voltage across each
is set by the bias of Q240. Output DC level at the collector
winding equals e/2 (assuming an ideal transformer). The
of Q230 is set by the IF Center Freq Range adjustments in
polarity of the signal at a particular instant of time is shown
the collector circuit of Q260.
in Fig. 3-6. This voltage, across the input windings, produces
an equal voltage (e/2) across the output windings with the
S w e e p O s c i l l a t o r . The oscillator frequency is primarily
a function of the L (L314) and C (diode D314 in series with
The generator, or source, is in series with the output wind-
blocking capacitor C314) in the collector circuit of Q310.
ing for T331, therefore, the voltage ot the output with refer-
Capacitance of diode D314 is varied by the signal from
ence to point A equals 3e/2. This voltage adds to the volt-
comparator Q230-Q220. An increase in back bias decreases
age output of T330 to provide a total output signal of 4e/2
or 2e.
If the reference point is changed to the common side of
not proportional to the voltage ramp, but high gain in the
the input windings of T330 and T331 (shown os a phantom
discriminator feedback loop to the comparator reduce this
ground on the simplified drawing) the impedance looking
non-linearity. At maximum dispersion, the oscillator sweeps
into the output terminals of the transformers is balanced,
from 225 MHz to 325 MHz.
3-6