## Square Wave Generator using Op-Amp

## How to make an Astable or Free running Multi vibrator using 741 Op-Amp ?

The non-sinusoidal waveform generators are also called relaxation oscillators. The op-amp relaxation oscillator shown in figure is a square wave generator. In general, square waves are relatively easy to produce. Like the** UJT relaxation oscillator**, the circuit’s frequency of oscillation is dependent on the charge and discharge of a capacitor C through feedback resistor R,. The “heart” of the oscillator is an **inverting op-amp comparator **

The comparator uses positive feedback that increases the gain of the amplifier. In a comparator circuit this offer two advantages. First, the high gain causes the op-amp’s output to switch very quickly from one state to another and vice-versa. Second, the use of positive feedback gives the circuit hysteresis. In the op-amp square-wave generator circuit given in figure, the output voltage v_{out} is shunted to ground by two Zener diodes Z_{1} and Z_{2} connected back-to-back and is limited to either V_{Z 2} or –V_{Z }_{1}. A fraction of the output is fedback to the non-inverting (+) input terminal. Combination of IL and C acting as a low-pass R-C circuit is used to integrate the output voltage v_{out} and the capacitor voltage v_{c} is applied to the inverting input terminal in place of external signal. The differential input voltage is given as **v**_{in }**= v**_{c }**- β v**_{out}

When v_{in} is positive, v_{out} = – V_{z1} and when v_{in} is negative v_{out} = + V_{z }2. Consider an instant of time when v_{in} < 0. At this instant v_{out} = + V_{z 2} , and the voltage at the non-inverting (+) input terminal is β V_{z 2} , the capacitor C charges exponentially towards V_{z 2}, with a time constant R_{f} C. The output voltage remains constant at V_{z 2 }until v_{c} equal β V_{z 2}.

When it happens, comparator output reverses to – V_{z} _{1}. Now v_{c} changes exponentially towards -V_{z1} with the same time constant and again the output makes a transition from -V_{z1 }to + V_{z 2. }when v_{c } equals -βV_{z 1}

**Let V**_{z1}** = V**_{z 2 }

The time period, T, of the output square wave is determined using the charging and discharging phenomena of the capacitor C. The voltage across the capacitor, v_{c} when it is charging from – B V_{z} to + V_{z} is given by

**V**_{c }**= [1-(1+β)]e**^{-T/2τ}

Where τ = R_{f}C

The waveforms of the capacitor voltage v_{c} and output voltage v_{out} (or v_{z}) are shown in figure.

When t = t/2

**V**_{c }**= +β V**_{z or }**+ β V**_{out}

Therefore β V_{z} = V_{z }[1-(1+β)e^{-T/2τ}]

**Or e**^{-T/2τ }**= 1- β/1+ β**

**Or T = 2τ log**_{e }**1+β/1- β = 2R**_{f }**C log**_{e }**[1+ (2R**_{3}**/R**_{2}**)]**

** The frequency, f = 1/T **, of the square-wave is independent of output voltage V

_{out}.

**. The output remains in one state for time T**

*This circuit is also known as free-running or astable multivibrator because it has two quasi-stable states*_{1}and then makes an abrupt transition to the second state and remains in that state for time T

_{2}. The cycle repeats itself after time

**T = (T**

_{1}

**+ T**

_{2}

**)**where T is the time period of the square-wave.

The op-amp square-wave generator is useful in the frequency range of about 10 Hz -10 kHz. At higher frequencies, the op-amp’s slew rate limits the slope of the output square wave. The symmetry of the output waveform depends on the matching of two Zener diodes Z_{1} and Z_{2}. The unsymmetrical square-wave (T_{1} not equal to t_{2}) can be had by using different constants for charging the capacitor C to +V_{out} and -V_{out}

im needing a square wave generator that will produce a square wave of 1,604,000hz, im on a tight budget ,can you assist?

Hi its very useful for me but i need more information than this…

how to design the same for duty cycle of 25%..?

what are the values of capacitors and rasistances.

Old Chips like the 741 never die they only get better!!! Nice Design,,,MR.OHM likes it!!!

What is the possible solution to generate a squarewave of frequency 1Hz with output oscillating between +3v and -3v with refrence to ground (i need it to feed a 200mA moter)

Pls Send me The Components list for this ckt in detail.

Advantage very simple with very few component count.

disadvantage limitted to audio frequency range only, you have to use additional buffer stage to avoid loading of the oscillator.

IC741

plz send me advantages.disadvantages,application

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