By Kenneth L. Ashley
Publication by means of Ashley, Kenneth L.
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Additional resources for Analog electronics with LabVIEW
1. 9 Therefore, the condition for linearity is that Vgs << 2Veff, with Veffn = VGS = Vtno and using . With this condition not satisfied, an output signal is distorted. 10 In the parabolic relationship, the squared terms cancel entirely. In general, though, the output signal contains harmonic content (distortion) when Vgs is too large compared to Veffn. 2. Nonlinearity Referred to the Output The discussion above of limits imposed on Vgs assumes that the transistor remains in the active mode. To clarify this point, reference is made to the output characteristics of Fig.
When VG (with respect to the semiconductor body) exceeds the threshold voltage, Vtno, a channel of free-carrier electrons forms under the oxide; that is, the onset of the channel occurs when VG = Vtno. The substrate is n type for the PMOS and the channel is made up of free-carrier holes. 1. MOS transistor consisting of a metal – oxide – semiconductor layered structure (plus a metal body contact on the bottom). A positive gate voltage, VG > Vtno, induces a conducting channel under the oxide, which connects the two n regions, source and drain.
Subscripts are for NMOS. All equations are the same for PMOS with "p" subscript substitution and subscript-order reversal for bias-voltage variables. Unit 5. Common-Source Amplifier Stage Two types of common-source amplifiers will be investigated in lab projects. One is with the source grounded and the other is with a current-source bias (dual power supply). 4 we cover the basics of the dual-power-supply amplifier. Both amplifiers are based on the PMOS, as in the projects. The first two units are mostly a review of the basic amplifier as presented in previous units, to reinforce the basic concepts.
Analog electronics with LabVIEW by Kenneth L. Ashley