• Source: Overdrive voltage

Overdrive voltage, usually abbreviated as VOV, is typically referred to in the context of MOSFET transistors. The overdrive voltage is defined as the voltage between transistor gate and source (VGS) in excess of the threshold voltage (VTH) where VTH is defined as the minimum voltage required between gate and source to turn the transistor on (allow it to conduct electricity). Due to this definition, overdrive voltage is also known as "excess gate voltage" or "effective voltage." Overdrive voltage can be found using the simple equation: VOV = VGS − VTH.




Technology


VOV is important as it directly affects the output drain terminal current (ID) of the transistor, an important property of amplifier circuits. By increasing VOV, ID can be increased until saturation is reached.
Overdrive voltage is also important because of its relationship to VDS, the drain voltage relative to the source, which can be used to determine the region of operation of the MOSFET. The table below shows how to use overdrive voltage to understand what region of operation the MOSFET is in:

A more physics-related explanation follows:
In an NMOS transistor, the channel region under zero bias has an abundance of holes (i.e., it is p-type silicon). By applying a negative gate bias (VGS < 0) we attract more holes, and this is called accumulation. A positive gate voltage (VGS > 0) will attract electrons and repel holes, and this is called depletion because we are depleting the number of holes. At a critical voltage called the threshold voltage (VTH) the channel will actually be so depleted of holes and rich in electrons that it will INVERT to being n-type silicon, and this is called the inversion region.
As we increase this voltage, VGS, beyond VTH, we are said to be then overdriving the gate by creating a stronger channel, hence the overdrive (often called Vov, Vod, or Von) is defined as (VGS − VTH).




See also


MOSFET
Threshold voltage
Electronic amplifier
Short-channel effect
Biasing




References

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