The operation of an OPV in the saturation range can be enforced in the circuit by feeding
back the output signal, i.e., returning it to the non-inverting input (+ input).
In the circuit shown, the feedback is provided by resistor $R_\mathrm{2}$.
The output voltage $u_\mathrm{a}$ can only take two values, either $\mathrm{+}U_\mathrm{sat}$
or $\mathrm{-}U_\mathrm{sat}$. It switches between these two values when no voltage drops
at the differential input of the OPV, ($u_\mathrm{d}=0$).
Then $i_\mathrm{R2}=\frac{u_\mathrm{a}}{R_\mathrm{2}}$ and
$u_\mathrm{e}=-R_\mathrm{1} \cdot i_\mathrm{R1}$.
Since the OPV input current is $i_\mathrm{p}=0$, the currents through the
resistors must be equal, and the following relationship applies for the switching points:
$u_\mathrm{e}=-\frac{R_\mathrm{1}}{R_\mathrm{2}}\cdot u_\mathrm{a}=\mp\frac{R_\mathrm{1}}{R_\mathrm{2}}\cdot U_\mathrm{sat}$
The image shows the input/output characteristic curve of the circuit known as a
βnon-inverting Schmitt trigger.β The reaction to any input signal is shown on the right.
The circuit only switches to $\mathrm{+}U_\mathrm{sat}$, when the positive switching
threshold at the input is reached. It only switches to $\mathrm{-}U_\mathrm{sat}$, when the
negative switching threshold at the input is reached.
To analyze the behavior of the schmitt trigger, the following circuit is used:
Supply voltages (from power supply unit):
UCC = + 3V, UEE = - 3V
Values of the components used:
R2 = 20kβ¦, R3 = 27kβ¦
Ue = 3 V (amplitude), f = 1 kHz
Channel 1: $\frac {Volt}{Div}=$
Channel 2: $\frac {Volt}{Div}=$
Time basis: $\frac {T}{Div}=$