ELEC 121 ELEC 121 Author unknown whsmsepiphany4.googlepages.com

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Presentation transcript:

ELEC 121 ELEC 121 Author unknown whsmsepiphany4.googlepages.com January 2004 Introduction to FET’s ELEC 121 Author unknown whsmsepiphany4.googlepages.com Introduction to FET's

Current Controlled vs Voltage Controlled Devices January 2004 ELEC 121

Types of FET’s JFET – Junction Field Effect Transistor MOSFET – Metal Oxide Semiconductor Field Effect Transistor D-MOSFET - Depletion Mode MOSFET E- MOSFET - Enhancement Mode MOSFET January 2004 ELEC 121

Transfer Characteristics The input-output transfer characteristic of the JFET is not as straight forward as it is for the BJT In a BJT,  (hFE) defined the relationship between IB (input current) and IC (output current). In a JFET, the relationship (Shockley’s Equation) between VGS (input voltage) and ID (output current) is used to define the transfer characteristics, and a little more complicated (and not linear): As a result, FET’s are often referred to a square law devices January 2004 ELEC 121

JFET Construction There are two types of JFET’s: n-channel and p-channel. The n-channel is more widely used. There are three terminals: Drain (D) and Source (S) are connected to n-channel Gate (G) is connected to the p-type material January 2004 ELEC 121

JFET Operating Characteristics There are three basic operating conditions for a JFET: JFET’s operate in the depletion mode only VGS = 0, VDS is a minimum value depending on IDSS and the drain and source resistance VGS < 0, VDS at some positive value and Device is operating as a Voltage-Controlled Resistor For an n channel JFET, VGS may never be positive* For an p channel JFET, VGS may never be negative* January 2004 ELEC 121

Specification Sheet (JFETs) January 2004 ELEC 121

N-Channel JFET Operation The nonconductive depletion region becomes thicker with increased reverse bias. (Note: The two gate regions of each FET are connected to each other.) January 2004 ELEC 121

N-Channel JFET Symbol January 2004 ELEC 121

Saturation At the pinch-off point: • any further increase in VGS does not produce any increase in ID. VGS at pinch-off is denoted as Vp. • ID is at saturation or maximum. It is referred to as IDSS. • The ohmic value of the channel is at maximum. January 2004 ELEC 121

ID  IDSS As VGS becomes more negative: • the JFET will pinch-off at a lower voltage (Vp). • ID decreases (ID < IDSS) even though VDS is increased. • Eventually ID will reach 0A. VGS at this point is called Vp or VGS(off). • Also note that at high levels of VDS the JFET reaches a breakdown situation. ID will increases uncontrollably if VDS > VDSmax. January 2004 ELEC 121

FET as a Voltage-Controlled Resistor The region to the left of the pinch-off point is called the ohmic region. The JFET can be used as a variable resistor, where VGS controls the drain-source resistance (rd). As VGS becomes more negative, the resistance (rd) increases. January 2004 ELEC 121

Transfer (Transconductance) Curve From this graph it is easy to determine the value of ID for a given value of VGS It is also possible to determine IDSS and VP by looking at the knee where VGS is 0 January 2004 ELEC 121

Plotting the Transconductance Curve Using IDSS and VP (or VGS(off)) values found in a specification sheet, the Family of Curves can be plotted by making a table of data using the following 3 steps: Step 1: Solve for VGS = 0V Step 2 Solve for VGS = VP ( aka VGS(off) ) Step 3: Solve for 0V VGS  VP in 1V increments for VGS January 2004 ELEC 121

Case Construction and Terminal Identification This information is found on the specification sheet January 2004 ELEC 121

p-Channel JFET’s p-Channel JFET operates in a similar manner as the n-channel JFET except the voltage polarities and current directions are reversed January 2004 ELEC 121

P-Channel JFET Characteristics As VGS increases more positively the depletion zone increases ID decreases (ID < IDSS) eventually ID = 0A Also note that at high levels of VDS the JFET reaches a breakdown situation. ID increases uncontrollably if VDS > VDSmax. January 2004 ELEC 121

MOSFET’s

MOSFETs MOSFETs have characteristics similar to JFETs and additional characteristics that make then very useful There are 2 types of MOSFET’s: Depletion mode MOSFET (D-MOSFET) Operates in Depletion mode the same way as a JFET when VGS  0 Operates in Enhancement mode like E-MOSFET when VGS > 0 Enhancement Mode MOSFET (E-MOSFET) Operates in Enhancement mode IDSS = 0 until VGS > VT (threshold voltage) January 2004 ELEC 121

MOSFET Handling MOSFETs are very static sensitive. Because of the very thin SiO2 layer between the external terminals and the layers of the device, any small electrical discharge can stablish an unwanted conduction. Protection: • Always transport in a static sensitive bag • Always wear a static strap when handling MOSFETS • Apply voltage limiting devices between the Gate and Source, such as back-to- back Zeners to limit any transient voltage January 2004 ELEC 121

D-MOSFET Symbols January 2004 ELEC 121

Specification Sheet January 2004 ELEC 121

Depletion Mode MOSFET Construction The Drain (D) and Source (S) leads connect to the to n-doped regions These N-doped regions are connected via an n-channel This n-channel is connected to the Gate (G) via a thin insulating layer of SiO2 The n-doped material lies on a p-doped substrate that may have an additional terminal connection called SS January 2004 ELEC 121

Basic Operation A D-MOSFET may be biased to operate in two modes: the Depletion mode or the Enhancement mode January 2004 ELEC 121

D-MOSFET Depletion Mode Operation The transfer characteristics are similar to the JFET In Depletion Mode operation: When VGS = 0V, ID = IDSS When VGS < 0V, ID < IDSS When VGS > 0V, ID > IDSS The formula used to plot the Transfer Curve, is: January 2004 ELEC 121

D-MOSFET Enhancement Mode Operation In this mode, the transistor operates with VGS > 0V, and ID increases above IDSS Shockley’s equation, the formula used to plot the Transfer Curve, still applies but VGS is positive: January 2004 ELEC 121

p-Channel Depletion Mode MOSFET The p-channel Depletion mode MOSFET is similar to the n-channel except that the voltage polarities and current directions are reversed January 2004 ELEC 121

Enhancement Mode MOSFET’s

n-Channel E-MOSFET showing channel length L and channel width W January 2004 ELEC 121

Enhancement Mode MOSFET Construction The Drain (D) and Source (S) connect to the to n-doped regions These n-doped regions are not connected via an n-channel without an external voltage The Gate (G) connects to the p-doped substrate via a thin insulating layer of SiO2 The n-doped material lies on a p-doped substrate that may have an additional terminal connection called SS January 2004 ELEC 121

Specification Sheet January 2004 ELEC 121

E-MOSFET Symbols January 2004 ELEC 121

Basic Operation The Enhancement mode MOSFET only operates in the enhancement mode. VGS is always positive IDSS = 0 when VGS < VT As VGS increases above VT, ID increases If VGS is kept constant and VDS is increased, then ID saturates (IDSS) The saturation level, VDSsat is reached. January 2004 ELEC 121

Transfer Curve To determine ID given VGS: where VT = threshold voltage or voltage at which the MOSFET turns on. k = constant found in the specification sheet The PSpice determination of k is based on the geometry of the device: January 2004 ELEC 121

p-Channel Enhancement Mode MOSFETs The p-channel Enhancement mode MOSFET is similar to the n-channel except that the voltage polarities and current directions are reversed. January 2004 ELEC 121

Summary Table JFET D-MOSFET E-MOSFET January 2004 ELEC 121 ELEC 121 Introduction to FET's