Overload protection circuit for switch type transistor
An overload protection circuit and protection circuit technology, applied in the direction of electronic switches, electrical components, pulse technology, etc., to achieve low power consumption, reduce costs, and achieve the effect of overload protection
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Embodiment 1
[0035] The working principle of the circuit of Embodiment 1 is:
[0036] ①. When the switch signal circuit 1 outputs a low level, the field effect transistor Q is cut off, and the first triode BG1 is cut off, because the resistance values of the fifth resistor R5 and the sixth resistor R6 are far greater than the resistance value of the load RL, therefore, The current flowing through the load RL is very small, the drain potential of the field effect transistor Q is close to the voltage of the power supply U, the voltage division ratio of the fifth resistor R5 and the sixth resistor R6, and the division ratio of the third resistor R3 and the fourth resistor R4 are set. The voltage ratio makes the potential of the negative input terminal B of the first operational amplifier IC1 higher than the potential of the positive input terminal A; at this time, the first operational amplifier IC1 is reverse-biased and outputs a low level, and the second transistor BG2 is also in the cut-o...
Embodiment 2
[0042] It also includes a delay discharge circuit composed of the second capacitor C2 and the eighth resistor R8, and the second capacitor C2 and the eighth resistor R8 are respectively connected in parallel between the base of the third triode BG3 and the negative pole of the power supply U .
[0043] The working principle of the circuit of embodiment two is:
[0044] ①. When the switch signal circuit 1 outputs a low level, the field effect transistor Q is cut off, and the third transistor BG1 is cut off, because the fifth transistor BG5 must be turned on when both the third transistor BG3 and the fourth transistor BG4 are turned on. It can only be turned on when it is turned on, so the fifth triode BG5 is cut off. At this time, because the field effect transistor Q is in the cut-off state, the current does not pass through the field effect transistor Q, no matter whether the load RL is short-circuited or overloaded, it will affect the field effect Tube Q has no effect.
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