Justin Chow Jacob Huang Daniel Soledad ME 4447/6405 Student Lecture
History Properties Types BJT JFET MOSFET Applications Overview Daniel Soledad
Transistor History “Transistor” is combination of “transconductance” and “variable resistor” How Transistors Are Made ▪ Vacuum tubes ▪ Inefficient, fragile, bulky, generated a lot of heat ▪ First Transistors ▪ Semiconductors – Bell Labs 1947 Introduction
Packaging Surface Mount or Through Hole Usually 3 or 4 terminal device ▪ Can be packaged into ICs General Applications Amplification/Regulation Switches Introduction
Current Controlled i.e: BJT The output current is proportional to input current Voltage Controlled i.e.: JFET, MOSFET The output current is proportional to input voltage
Bipolar Junction Transistor 3 semiconductor layers sandwiched together Comes in two flavors NPN BJT PNP BJT BJT Transistor Justin Chow
Diodes Forward BiasedReverse Biased current flowsno current flows when V PN >.6-.7V BJT Transistor
BJT Basics (NPN) BE Forward Biased BC Reversed Biased β=I B / I c ≈ 100 I E = I B + I C BJT Transistor emitter base collector Electron Flow
Things to remember PNP, biasing opposite Conventional current vs electron flow A small input current controls a much larger output current. BJT Transistor
Operating Regions BJT Transistor Operating RegionParameters Cut Off V BE <0.7 V I B = I C = 0 Linear V BE >0.7 V I C = β*I B Saturated I B > 0, I C > 0 V BE >0.7 V, V CE 0.2 V
Operating Regions BJT Transistor
From 3 rd Exercise Turns on/off coils digitally
Common Emitter Amplifier BJT Transistor β=100
Common Emitter Amplifier BJT Transistor I B = (V in − V B ) / 10000Ω = (V in − 0.7) / 10000Ω I C = β(V in − 0.7) / 10000Ω V out =10000*(V in -0.7)/1000 When V CE = 0.2V I C = 9.8 / 1000Ω = 9.8mA I B = I C / β = 0.098mA V in − 0.7 = (0.098mA)(10000Ω) V in = 1.68V or greater.
Power Dissipation P BJT = V CE * i CE Should be below the rated transistor power Important for heat dissipation as well BJT Transistor
Darlington Transistors Increased Gain β = β 1 * β 2 V BE = V BE1 + V BE2 Slower Switching 2N6282
FET Transistors Analogous to BJT Transistors Output is controlled by input voltage rather than by current 4 Pins vs. 3 BJTFET CollectorDrain BaseGate EmitterSource N/ABody
FET Transistors FET (Field Effect Transistors) MOSFET (Metal-Oxide-Semiconductor Field-Effect Transistor) JFET (Junction Field-Effect Transistor) MESFET HEMT MODFET Most common are the n-channel MOSFET or JFET Jacob Huang
FET Transistors – Circuit Symbols In practice the body and source leads are almost always connected Most packages have these leads already connected B S G D B S G D S G D MOSFET JFET
MOSFET Metal-Oxide Semiconductor F.E.T. A.K.A. Insulated-Gate FET (IGFET) 2 Modes: Enhancement/Depletion
Depletion Mode N-Channel + V gs -> More electrons -> More Current - V gs -> Less electrons -> Less current P-Channel – Reversed Different from BJT
Characteristic Curves for D-type Current flow B S G D
Enhancement Mode N-Channel V GS > V th -> Turns on device V GS No Current P-Channel Reversed Only E-type used now
Modes of Operation RegionCriteriaEffect on Current Cut-offV GS < V th I DS =0 LinearV GS > V th And V DS <V GS -V th Transistor acts like a variable resistor, controlled by V gs SaturationV GS > V th And V DS >V GS -V th Essentially constant current Current flow B S G D
Characteristic Curve for E-type Current flow B S G D
Power MOSFET Used in high-power applications Heat Sink Vertical layout Not Planar like other transistors
Junction gate FET Reverse Bias V GS => Reduces channel size => Reduced Current Defaults “on”
JFET as Switch V gs = 0 “on” |V gs |> |V p | “off” V p = Pinch-off or Cut-off Voltage
JFET Properties Internal Capacitance Bi-directional Cut-off voltage is varying for each JFET 0.3V – 10V N-Channel – Negative V GS P-Channel – Positive V GS Do not Forward Bias JFET – burn out
JFET Characteristic Curve
Comparison PropertyBJTMOSFETJFET GmBestWorstMedium SpeedHighMediumLow NoiseModerateWorstBest Good Switch NoYes High-Z GateNoYes ESD Sensitivity LessMoreLess
CMOS Complementary MOS Used in Logic Gates P-channel (PMOS) to high N-channel (NMOS) to low HIGH usually +5 V LOW usually ground Q is high when A = 0, Q is low when A = 1
References Spring 2007/2008 Slides bjt.gif&imgrefurl= bridge/bjt_theory.html mon_Emitter_Amplifier_Circuit