Differences
This shows you the differences between two versions of the page.
| Both sides previous revision Previous revision Next revision | Previous revision | ||
| lab_electrical_engineering:6_opamps_2 [2026/06/17 11:00] – mexleadmin | lab_electrical_engineering:6_opamps_2 [2026/06/17 13:08] (current) – mexleadmin | ||
|---|---|---|---|
| Line 1: | Line 1: | ||
| - | =====Combination of Integrator and Schmitt Trigger - Oscillator===== | + | <wrap onlyprint> |
| - | + | ||
| - | ====Background Information==== | + | |
| - | + | ||
| - | The circuits previously analyzed individually are now connected to form a complete system.\\ | + | |
| - | The integrator and the Schmitt trigger together form an oscillator. The output signal | + | |
| - | of the Schmitt trigger is fed back to the input of the integrator. Therefore, the output | + | |
| - | signal simultaneously acts as the input signal of the overall system.\\ | + | |
| \\ | \\ | ||
| - | {{drawio> | + | ====== Experiment 6: Operational Amplifier II - Pulse Width Modulation ====== |
| - | \\ | + | * Circuits on the breadboard |
| - | \\ | + | * Integrator |
| - | Due to this feedback, | + | * Non-inverting |
| - | input signal, apart from the supply voltages of the operational amplifiers.\\ | + | * Triangle–square-wave generator |
| - | \\ | + | * Pulse-width modulation |
| - | The Schmitt trigger | + | |
| - | until one of the switching thresholds is reached. At this point, the output state changes | + | |
| - | and the process repeats continuously, | + | |
| - | \\ | + | |
| - | When the circuit is first powered on, the oscillator starts due to small disturbances such | + | |
| - | as noise, offset voltages of the operational amplifiers, or slight asymmetries in the circuit. | + | |
| - | These small deviations move the system away from the unstable equilibrium point and initiate | + | |
| - | the oscillation. | + | |
| - | ====Experimental Tasks==== | + | < |
| - | To analyze the behavior of the oscillator (triangle-rectangle generator), the following circuit is used:\\ | + | {{page>.:6_opamps_2: |
| - | \\ | + | |
| - | < | + | |
| - | {{drawio>mexlefirst_intern:oscillator_circuit.svg}} | + | |
| </ | </ | ||
| - | \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ \\ | ||
| - | \\ | ||
| - | __Supply voltages (from power supply unit): | ||
| - | UCC = + 3V, UEE = - 3V\\ | ||
| - | \\ | ||
| - | __Values of the components used: | ||
| - | R1 = 200 kΩ, R1.3 = 10 kΩ, R2 = 20 kΩ, R3 = 27 kΩ, C1 = 10 nF\\ \\ | ||
| - | | + | <wrap # |
| - | * Connect channel 1 of the oscilloscope | + | {{page> |
| - | * Now try to generate a minimum and maximum frequency with your circuit by turning the potentiometer R1 to the left and right stops. Perform this experiment with two capacitance values: $C1=10~nF$ and $C1=1~nF$. Enter the measured frequency values in the following table.\\ \\ {{drawio>mexlefirst_intern: | + | |
| - | | + | {{page>Combination_of_Integrator_and_Schmitt_Trigger_(Oscillator)& |
| - | \\ | + | |
| - | + | {{page>LED_Brightness_Control_using_PWM& | |
| - | **C1 = 10 nF, f = ƒmin**\\ | + | |
| - | \\ | + | |
| - | <wrap left> | + | |
| - | {{drawio>mexlefirst_intern: | + | |
| </ | </ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Channel 1: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | Channel 2: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Time basis: $\frac {T}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ \\ \\ \\ | ||
| - | **C1 = 10 nF, f = ƒmax**\\ | ||
| - | \\ | ||
| - | <wrap left> | ||
| - | {{drawio> | ||
| - | </ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Channel 1: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | Channel 2: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Time basis: $\frac {T}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ \\ \\ \\ | ||
| - | **C1 = 1 nF, f = ƒmin**\\ | ||
| - | \\ | ||
| - | <wrap left> | ||
| - | {{drawio> | ||
| - | </ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Channel 1: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | Channel 2: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Time basis: $\frac {T}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ \\ \\ \\ | ||
| - | **C1 = 1 nF, f = ƒmax**\\ | ||
| - | \\ | ||
| - | <wrap left> | ||
| - | {{drawio> | ||
| - | </ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Channel 1: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | Channel 2: $\frac {Volt}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | Time basis: $\frac {T}{Div}=$\\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ | ||
| - | \\ \\ \\ \\ | ||
| - | 3. Explain how this circuit works in a few sentences.\\ | ||
| - | \\ | ||
| - | 4. Why is it useful to use R1 as a potentiometer to vary the frequency rather than R2 | ||
| - | or R3?\\ | ||
| - | \\ | ||
| - | ====Test Questions==== | + | ===== Preparation ===== |
| + | For this experiment, you should be able to apply and explain the following concepts: | ||
| + | - " | ||
| + | - deviating properties of the real operational amplifier (e.g., output swing range, slew rate) | ||
| + | - output-voltage waveform $U_A$ of the inverting integrator (inverting integrator) for different input voltages $U_E$, e.g. | ||
| + | - DC voltage | ||
| + | - square-wave voltage | ||
| + | - arbitrary voltage waveform | ||
| + | - integration time constant of the inverting integrator | ||
| + | - Schmitt trigger | ||
| + | - difference in feedback compared to the inverting integrator | ||
| + | - idealized relationship between $U_E$ and $U_A$ | ||
| + | - idealized line diagram: $U_E$ and $U_A$ as a function of time | ||
| + | - switching thresholds | ||
| + | - threshold voltage | ||
| + | - hysteresis | ||
| + | - real behavior: output "in saturation" | ||
| + | - structure of the triangle–square-wave generator | ||