The basic principle of this kind of transistor was first patented by Julius Edgar Lilienfeld in 1925. Note: threshold voltage for this device lies around 0.45 V History Simulation of formation of inversion channel (electron density) and attainment of threshold voltage (IV) in a nanowire MOSFET. Since MOSFETs can be made with either p-type or n-type semiconductors, complementary pairs of MOS transistors can be used to make switching circuits with very low power consumption, in the form of CMOS logic. The MOSFET is by far the most common transistor in digital circuits, as billions may be included in a memory chip or microprocessor. Similarly, 'oxide' in the name can also be a misnomer, as different dielectric materials are used with the aim of obtaining strong channels with smaller applied voltages. The 'metal' in the name MOSFET is sometimes a misnomer, because the gate material can be a layer of polysilicon (polycrystalline silicon). In depletion mode transistors, voltage applied at the gate reduces the conductivity.

In an enhancement mode MOSFET, voltage applied to the gate terminal increases the conductivity of the device. The main advantage of a MOSFET is that it requires almost no input current to control the load current, when compared with bipolar transistors (bipolar junction transistors/BJTs). Operating as switches, each of these components can sustain a blocking voltage of 120 V in the off state, and can conduct a continuous current of 30 A in the on state, dissipating up to about 100 W and controlling a load of over 2000 W. Two power MOSFETs in D2PAK surface-mount packages.

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