The Schmitt trigger can be realized with a simple tunnel diode. The volt-ampere characteristic of this diode is an "N"-shaped curve in the first quadrant. The oscillating input will cause the volt-ampere characteristic of the diode to move from the rising branch of the "N"-shaped curve to another branch and then return to the starting point when the input value exceeds the rising and falling flip thresholds. However, the performance of this type of Schmitt trigger can be improved by using transistor-based components, because transistor-based components can directly use positive feedback to improve flipping performance.

Comparators

Schmitt triggers are often implemented by connecting positive feedback comparators. For this circuit, the flip occurs close to the ground, and the amount of hysteresis is controlled by the resistance of R1 and R2.

The comparator extracts the sign of the difference between the two inputs. When the voltage of the non-inverting (+) input is higher than the voltage of the inverting (-) input, the output of the comparator flips to the high operating voltage +Vs; when the voltage of the non-inverting (+) input is lower than the voltage of the inverting (-) input, the output of the comparator flips to the low operating voltage -Vs. The inverting (-) input here is grounded, so the comparator here implements the function symbol, which has the characteristics of a two-state output. There are only two states of high and low. When the non-inverting (+) terminal is continuously input, there will always be the same symbol.

Since the resistor network connects the input terminal of the Schmitt trigger with the output terminal of the comparator, the Schmitt trigger behaves like a comparator and can flip the level at different times. It depends on whether the output of the comparator is high or low. If the input is a negative input with a large absolute value, the output will be low; if the input is a positive input with a large absolute value, the output will be high, which realizes the function of a non-inverting Schmitt trigger. However, for an input whose value is between two thresholds, the output state depends on both the input and the output. For example, if the current state of the Schmitt trigger is high, the output will be on the positive power +Vs. At this time, V+ will become a voltage divider between Vin and +Vs. In this case, the comparator will flip to a low level only when V+=0 (grounded). From the conservation of current, it can be seen that the following relationship is satisfied at this time:

Therefore, it must be lowered below -R1Vs/R2 before the output will reverse. Once the output of the comparator flips to −Vs, the threshold for flipping back to the high level becomes +R1Vs/R2. In this way, the circuit forms a section of the switching voltage band around the origin, and the trigger level is ±R1Vs/R2. Only when the input voltage rises to the upper limit of the voltage band, the output will flip to a high level; only when the input voltage drops to the lower limit of the voltage band, the output will flip back to a low level. If R1 is 0, R2 is infinite (ie, open circuit). And the width of the voltage band will be compressed to 0. At this time, the circuit becomes a standard comparator. The output characteristics are shown on the right. The threshold T is given by R1Vs/R2, and the maximum value of the output M is the power rail. The actual configuration of the non-inverting Schmitt trigger circuit is shown in the Figure below.

The output characteristic curve has the same shape as the output curve of the above-mentioned basic configuration, and the threshold value also satisfies the same relationship as the above-mentioned configuration. The difference is that the output voltage of the above example depends on the power supply, while the output voltage of this circuit is determined by two Zener diodes. In this configuration, the output level can be changed by selecting an appropriate Zener diode, and the output level is resistant to power fluctuations, that is to say, the output level improves the power supply voltage rejection ratio (PSRR) of the comparator. The resistor R3 is used to limit the current through the diode, and the resistor R4 reduces the input offset voltage caused by the input leakage current of the comparator to a minimum.

Two transistors

In the Schmitt trigger implemented using the positive feedback configuration, most of the complex functions that the comparator itself can implement are not used. Therefore, the circuit can be implemented with two cross-coupled transistors. The Schmitt trigger circuit based on 2 transistors is shown in the Figure below. The path RC1 R1 R2 sets the base voltage of the transistor T2, but this voltage divider path will be affected by the transistor T1. If T1 is open, the path will provide a higher voltage. Therefore, the threshold voltage that flips between the two states depends on the current state of the flip-flop.

For the NPN transistor shown above, when the input voltage is much lower than the common-emitter voltage, T1 will not turn on. The base voltage of the transistor T2 is determined by the aforementioned voltage divider circuit. Due to the access to negative feedback, the voltage applied to the common emitter must be almost as high as the voltage determined on the voltage divider circuit, so that T2 can be turned on, and the output of the trigger is in a low-level state. When the input voltage (T1 base voltage) rises slightly higher than the voltage (emitter voltage) on the resistor RE, T1 will be turned on. When T1 starts to turn on, T2 is no longer turned on, because the voltage provided by the voltage divider path is lower than the base voltage of T2. And the emitter voltage will not decrease, because T1 consumes current through RE at this time. At this time, T2 is not turned on, and the flip-flop transitions to a high-level state.

At this time, the flip-flop is in a high-level state. If the input voltage drops sufficiently, the current through T1 will decrease, which will reduce the common emitter voltage of T2 and increase its base voltage. When T2 starts to conduct, the voltage on RE rises, and then the base-emitter potential of T1 is reduced, and T1 is no longer conducting.

In the high-level state, the output voltage is close to V+; but in the low-level state, the output voltage will still be much higher than V−. Therefore, in this case, the output voltage is not low enough to reach the logic low level, which requires an additional amplifier on the flip-flop circuit.

The above circuit can be simplified: R1 can be replaced by a short-circuit connection so that the base of T2 is directly connected to the collector of T1, and R2 can be removed and replaced with an open circuit. The key to circuit operation is that when T1 is turned on (the result of current input to the base), the current through RE is smaller than when T1 is turned off, because when T1 is turned on, T2 will be turned off. When T2 is turned on, compared to T1, it provides RE with a greater passing current. When the current flowing into the RE decreases, the voltage on it will decrease, so once the current starts to flow into T1, the input voltage must decrease to make T1 return to the off state, because the emitter voltage of T1 has dropped at this time. This Schmitt trigger buffer can also be turned into a Schmitt trigger inverter, and a resistor can be omitted in the process by replacing RK2 with a short circuit and connecting Vout to the emitter of T2 Instead of the collector.

However, in this case, the resistance of RE should be larger, because RE should act as a pull-down resistor at the output. Its function is that when the output should be low, it will reduce the voltage at the output. If the resistance of RE is small, only a small voltage can be produced on it. When the output should be a digital low level, this voltage will actually increase the output voltage.

Applications

1. Waveform transformation

Triangular waves, sine waves, periodic waves, etc. can be transformed into rectangular waves.

2. Shaping of pulse wave

In digital systems, rectangular pulses often undergo waveform distortion during transmission, and the rising and falling edges are not ideal. After shaping by Schmitt trigger, a more ideal rectangular pulse can be obtained.

3. Pulse amplitude discrimination

When pulse signals with different amplitudes and irregularities are applied to the input terminal of the Schmitt trigger, pulse signals with an amplitude greater than a preset value can be selected for output.

4. Form a multivibrator

Signals with different amplitudes will generate rectangular pulses after passing through a Schmitt trigger with a suitable capacitor. Rectangular wave pulse signals are often used as pulse signal sources and clock signals in sequential circuits.

Commonly used chips

74LS18 dual four-input NAND gate (Schmitt trigge)

74LS14 six inverters (Schmitt trigge)

74132, 74LS132, 74S132, 74F132, 74HC132 2-input four-and non-Schmitt trigger

74221, 74LS221, 74 HC221, 74 C221 double monostable multivibrators (with Schmitt trigger)

Schmitt trigger can be formed with 555 timer

CD4093 consists of four 2-input Schmitt triggers