Linear Integrated Circuits: Unit III: Applications of Op-amp

Monostable Multivibrator using Op-amp

Working Principle, Pulse, Circuit Diagram

There are three types of multivibrator circuits in use, namely, a) Bistable multivibrator b) Monostable multivibrator c) Astable multivibrator Let us see the basic concept behind the operation of these three types of multivibrators.


Monostable Multivibrator using Op-amp

The monostable multivibrator circuit using op-amp is shown in the Fig. 3.14.1.


The diode D1 is clamping diode connected across C. The diode clamps the capacitor voltage to 0.7 V when the output is at +Vsat. A narrow negative triggering pulse Vt is applied to the noninverting input terminal, through diode D2.

Let us see the operation of the circuit.

To understand the operation of the circuit, let us assume that the output Vo is at +Vsat i.e. in its stable state. The diode D1 conducts and the voltage across the capacitor C i.e. VC gets clamped to 0.7 V. The voltage at the non-inverting input terminal is controlled by potentiometric divider of R1R2 to β Vo i.e. + 3 Vsat in the stable state.

Now if Vt, a negative trigger of amplitude Vt is applied to the non-inverting terminal, so that the effective voltage at this terminal is less than 0.7 V (+ β Vsat + (- Vt)) then the output of the op-amp changes its state from + Vsat to - Vsat.

The diode is now reverse biased and the capacitor starts charging exponentially to - Vsat through the resistance R. The time constant of this charging is τ = RC.

The voltage at the non-inverting input terminal is now - β Vsat. When the capacitor voltage VC becomes just slightly more negative than - β Vsat, the output of the op-amp changes its state back to + Vsat.

The capacitor now starts charging towards + Vsat through R until VC reaches 0.7 V as capacitor gets clamped to the voltage.

The waveforms are shown in the Fig. 3.14.2.


 

1. Expression for Pulse Width T

For a low pass RC circuit let,

Vi = Initial value of the voltage

Vf = Final value of the voltage

Then the general solution is given by,

Vo = Vf + (Vi - Vf) e-t/RC  ...(3.14.1)\

Now for the monostable multivibrator discussed above, the values of Vf  and Vi  are,

Vf = - Vsat and Vi = VD1 (diode forward voltage)

while Vo = Output = Capacitor voltage = VC

VC -Vsat + (VD1-[-Vsat])e-t/RC   …. (3.14.2)

at  t = T, VC = -β  Vsat …. (3.14.3)


This is obtained by absorbing negative sign inside the natural logarithm. The potential divider decides the value of 3 given by,

β = R2 / R1 + R2  … (3.14.6)

If Vsat >> VD1 and R1 = R2 so that β = 0.5, then

T = 0.69 RC  …. (3.14.7)

For monostable operation, the trigger pulse width Tp should be much less than T, the pulse width of the monostable multivibrator.

The diode D2 is not essential but it is used to avoid malfunctioning if any positive noise spikes are present in the triggering line. It can be seen from the waveform that the voltage VC does not reach its quiescent value VD1 until time T' > T. Hence it is necessary that a recovery time T' - T be allowed to elapse before the next triggering signal is applied.

Review Question

1. Draw the circuit of monostable multivibrator and obtain expression for pulse width.

Dec.-07, 09, Marks 8


Linear Integrated Circuits: Unit III: Applications of Op-amp : Tag: : Working Principle, Pulse, Circuit Diagram - Monostable Multivibrator using Op-amp