Figure shows the circuit diagram of a Miller sweep generator/integrator or a sweep generator circuit, in which two transistors Q1 and Q2 are used. The function of miller sweep generator is to convert step or square waveform into ramp waveform.
In the
circuit, transistor Q1 acts as a switch and transistor Q2 acts a high gain common
emitter amplifier. Initially consider Q1 is ON and Q2 is OFF. At this
condition, the voltage across the capacitor C and the output voltage V0 is
equal to voltage of +Vcc. When a negative pulse is applied to the base of Q1, it
will turn OFF due to reverse biasing of emitter-base junction and hence the
collector voltage of Q1 increases which increases the bias to Q2 and turned it ON.
Now transistor Q2 conducts, output voltage V0 starts to decrease because of capacitor
is coupled to the base of transistor Q2.
The rate of decrease of output voltage V0 is
controlled by rate of discharge of capacitor and time constant of the discharge
is given by
td = RB2*C.
Since
value of time constant is very large, the discharge current remains constant and
the rundown of the collector voltage is linear as shown in following figure. When the
input pulse is removed, Q1 turns ON and Q2 turns OFF. The capacitor charges
quickly to +Vcc through collector resistor Rc with the time constant
t =RC*C
First figure
shows simple circuit of miller sweep generator where practical circuit includes
more stages with emitter follower and diodes (in place of collector resistor
Rc). Miller sweep generator is considered the best sweep generator among the
available other circuits due to its excellent sweep linearity. You can see the
multisim simulation of the miller circuit in following video.
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