Chapter 5: Difference between revisions

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Revision as of 17:53, 19 March 2010

Metal-oxide semiconductor field effect transistor (MOSFET)

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Circuit symbols for various FETs

"In MOSFETs, a voltage on the oxide-insulated gate electrode can induce a conducting channel between the two other contacts called source and drain. The channel can be of n-type or p-type, and is accordingly called an nMOSFET or a pMOSFET (also commonly nMOS, pMOS)."<ref>http://en.wikipedia.org/wiki/MOSFET MOSFET - Wikipedia</ref>

  • Enhancement: The electric field from the gate voltage forms an induced channel allowing current to flow.
  • Depletion: The channel is physically implanted rather than induced. Thus, Vto is the opposite polarity of the Enhancement mode.
  • JFET: Charge flows through a semiconducting channel (between the source and drain). Applying a bias voltage to the gate terminal impedes the current flow (or pinches it off completely). Vto is the opposite polarity of the Enhancement mode.

Modes of operation

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NMOS & PMOS in Cutoff
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Triode (Linear) and Saturation (B.P.O = Beyond Pinch Off)
NMOS
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  • Cutoff
  • Triode:
  • The threshold voltage, Vto, is the minimum VGS needed to move the transistor from the Cutoff to Triode region. When is reached, a channel forms beneath the gate, allowing current to flow.
  • Vto is usually on the order of a couple of volts
  • For small values of VDS, iD is proportional to VDS. The device behaves as a resistor whose value depends on vGS
  • Saturation:
  • "Now consider what happens if we continue to increase VDS. Because of the current flow, the voltages between points along the channel and the source become greater as we move toward the drain. Thus, the voltage between gate and channel becomes smaller as we move toward the rain, resulting in a tapering of the channel thickness as illustrated in Figure 5.5. Because of the tapering of the channel, its resistance becomes larger with increasing vDS, resuling in a lower rate of increase of iD." <ref>Electronics p. 291</ref>

Device equations

Conditions for various modes of operation
Region vGS vDS
Cutoff vGS<Vto
Triode vGSVto vDSvGSVto
Saturation vGSVto vDSvGSVto
Boundry vGSvDS=Vto
Alternate (Frohne) method
Region vGS vDG
Cutoff vGS<Vto
Triode vGSVto vDGVto
Saturation vGSVto vDGVto
Drain current
Region iD K
(Enhancement/Depletion)
K
(JFET)
Cutoff 0 WLμnCox2=WLKP2 IDSSVto2
Triode K[2(vGSVto)vDSvDS2]
Saturation K(vGSVto)2
Boundry KvDS2
  • Device Parameters: KP=μnCox
  • Surface Mobility: μn, the electrons in the channel
  • Capacitance of the gate per unit area: Cox

Pros and Cons

Transistor Pros Cons
MOSFET Draws no gate current
Infinite input resistance
Gate protection needed to prevent static electricity from breaking down the insulation
JFET
BJT

Analysis

  1. Analyze the DC circuit to find the Q-point (using nonlinear device equations or characteristic curves)
  2. Use the small-signal equivalent circuit to find the impedance and gains

Small-signal equivalent circuits

  • "Transconductance, gm, is an important parameter in the design of amplifier circuits. In general, better performance is obtained with higher values of gm."<ref>Electroincs p. 310</ref>
  • Transconductance is defined as gm=2K(VGSQVto)=2KPW/LIDQ.
  • id=gmvgs+vdsrd, where rd is the drain resistance


Type Voltage Gain Current Gain Power Gain Input Impedance Output Impedance Frequency Response
Common-Source Av<1 Ai>1 G>1 High Low
Source Follower
Common-Gate

Questions

  • What's the difference between the enhancement and depletion modes?
  • NMOS and BJTs seem very similar. Why would you use one over the other?
  • How do you find rd?
  • Roughly what are the breakdown voltages for JFETs?
  • Learn how to check for operating regions via Vgs & Vds as compared to Vto.
  • CMOS nand/nor gates
  • JFET only goes to IDSS
  • Small signal model of mosfets

References

<references/>