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 $R_\mathrm{2}$.
lab_electrical_engineering:non_inverting_schmitt_trigger_circuit.svg

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: $u_\mathrm{e}=-\frac{R_\mathrm{1}}{R_\mathrm{2}}\cdot u_\mathrm{a}=\mp\frac{R_\mathrm{1}}{R_\mathrm{2}}\cdot U_\mathrm{sat}$


lab_electrical_engineering:non_inverting_schmitt_trigger_characteristic_input_output_signal.svg

The image shows the input/output characteristic curve of the circuit known as a β€œnon-inverting Schmitt trigger.” 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:

lab_electrical_engineering:schmitt_trigger_circuit_experiment.svg


Supply voltages (from power supply unit):
UCC = + 3V, UEE = - 3V

Values of the components used:
R2 = 20kΩ, R3 = 27kΩ

  1. Calculate the switching thresholds using the given values.











  2. Roughly sketch the voltage curves that you expect at the SQ output when you apply a triangular signal to Ue whose amplitude just reaches the switching points.

    Output SQ

    lab_electrical_engineering:oscilloscope_screen.svg


    Channel 1:$\frac {Volt}{Div}=$


    Time basis: $\frac {T}{Div}=$


  3. Set up the Schmitt Trigger on the MEXLE-Board. Perform the following measurements on the Schmitt Trigger:
    • Connect channel 1 on the oscilloscope to π‘ˆπ‘’ and channel 2 to SQ.
    • Connect the function generator to the Ue input. Set it to triangle with a frequency of 1kHz and a voltage of 3 V (amplitude).
    • Sketch the oscilloscope screen image.

      Ue = 3 V (amplitude), f = 1 kHz

      lab_electrical_engineering:oscilloscope_screen.svg


      Channel 1: $\frac {Volt}{Div}=$

      Channel 2: $\frac {Volt}{Div}=$


      Time basis: $\frac {T}{Div}=$




  4. Sketch the oscilloscope screen image you would expect for 1 V (amplitude).

    Ue = 1 V (amplitude), f = 1 kHz

    lab_electrical_engineering:oscilloscope_screen.svg


    Channel 1: $\frac {Volt}{Div}=$

    Channel 2: $\frac {Volt}{Div}=$


    Time basis: $\frac {T}{Div}=$
  5. Compare your measurements with the calculation from sub-task 1 and the forecast from 2. Explain the results.