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October 11, 2005ME 6405 Transistors ME 6405 Mechatronics In Order of Presentation: Jonathan Jobe David Malphurs Isaac Penny 0000 0001
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October 11, 2005ME 6405 Transistors Contents Brief History Properties of Transistors Types of Transistors Characteristics and Applications Engineering Selection 0000 0010
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October 11, 2005ME 6405 Transistors History Vacuum Tube 1879Edison Invents Light Bulb 1883Edison found that he could detect electrons flowing through the vacuum from the lighted filament to a metal plate mounted inside the bulb. “Edison Effect” John Fleming implements Edison Effect as first diode. 1906Lee DeForest introduced a third electrode called the grid into the vacuum tube. The resulting triode could be used as both an amplifier and a switch. 0000 0011
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October 11, 2005ME 6405 Transistors Predecessors 0000 0100 Diode Triode
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October 11, 2005ME 6405 Transistors First Transistors Bell Labs 1947 Invented First Transistor Application: replace vacuum tubes Smaller, more durable, no warm up Made of Germanium Current Transistors Silicon based Doped with phosphorus (n-type) Doped with boron (p-type) 0000 0101
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October 11, 2005ME 6405 Transistors The PN Junction Forward Biasing The external Voltage lowers the potential barrier at the junction, allowing the electrons to flow. Reverse Biasing The external voltage raises the potential barrier at the junction, preventing electrons from flowing. 0000 0110
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October 11, 2005ME 6405 Transistors Transistor Types BJTBipolar Junction Transistor FETField Effect Transistor JFET(Junction FET) MOSFET (Metal Oxide Semiconducting FET) 0000 0111
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October 11, 2005ME 6405 Transistors B J T s 2 types NPN (most common) When I B ≠0, V CE forward biased & V BC reverse biased PNP When I B ≠0, V CE reverse biased & V BC forward biased 0000 1000 NPN bipolar junction transistor PNP bipolar junction transistor
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October 11, 2005ME 6405 Transistors npn-B J T Voltage Characteristic Cutoff:Base-Emitter starts to conduct with V BE =0.6V Saturation: Increasing I B causes I C to rise exponentially. Active: Breakdown: I c approaches infinity due to breakdown at both junctions 0000 1001
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October 11, 2005ME 6405 Transistors B J T Operational Characteristics Operation Region I B or V CE Char. V CE & V BE Junctions Mode CutoffI B = Very small Reverse & Reverse Open Switch SaturationV CE = SmallForward & Forward Closed Switch Active Linear V CE = Moderate Reverse & Forward Linear Amplifier Break- down V CE = LargeBeyond Limits Overload 0000 1010
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October 11, 2005ME 6405 Transistors Equations of npn-B J T s 0000 1011 Definitions Kirchoff’s Current Law In Active region Common values for ß are 20 to 200
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October 11, 2005ME 6405 Transistors Point of Operation 0000 1100 The existence of RC means that I C and V CE are no longer independent. V CE = V cc – I C *R C After solving for I C,
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October 11, 2005ME 6405 Transistors Point of Operation 0000 1101 Load-line constraint Q point for I B =100μA Selecting V BB and V CC, we can find the operating point, or Q point. I B = (V BB -V BE )/R B
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October 11, 2005ME 6405 Transistors B J T resistor sizing ß and I C,max are specified by the catalog We need to choose Values for R B and R C to keep I C and I B within specifications 0000 1110
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October 11, 2005ME 6405 Transistors Three Types of Field Effect Transistors MOSFET (metal-oxide-semiconductor field-effect transistors) Enhancement mode I DS α V GS Depletion mode I DS α 1/V GS JFET (Junction Field-effect transistors) Available in n or p Channel n-Channel activated by V GS > 0 for MOSFET and V GS < 0 for JFET p-Channel activated by V GS 0 for JFET Most Common Types n-Channel Enhancement Mode MOSFET (NMOS) n-Channel JFET Field Effect Transistors (FET) 0000 1111
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October 11, 2005ME 6405 Transistors Enhanced MOSFET Depleted MOSFET FET Architecture BJTFET BaseGate CollectorDrain EmitterSource JFET Analogous BJT Terminals Conducting Region Nonconducting Region Nonconducting Region 0001 0000
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October 11, 2005ME 6405 Transistors NMOS Voltage Characteristic Active Region Saturation Region V GS < V th I DS =0 V GS > V th : 0 < V DS < V Pinch off Active Region I DS controlled by V GS V DS > V Breakdown I DS approaches I DSShort Should be avoided V DS > V Pinch off Saturation Region I DS constant V DS = Constant V Pinchoff 0001
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October 11, 2005ME 6405 Transistors Junction Field Effect Transistor V GS > V th I DS =0 V GS < -V th : 0 < V DS < V Pinch off Active Region I DS controlled by V GS V DS > V Pinch off Saturation Region I DS constant V DS > V Breakdown I DS approaches I DSShort Should be avoided Difference from NMOS V Pinchoff Active Region Saturation Region 0001 0010
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October 11, 2005ME 6405 Transistors Transistor Selection 0001 0011
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October 11, 2005ME 6405 Transistors Applications of Transistors Switch Voltage Amplifier Current Amplifier 0001 0100
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October 11, 2005ME 6405 Transistors Transistor as a Switch Many times you just need to switch a signal on or off Ex. Digital Logic, LED’s, PWM Relays can perform this same function They can usually handle higher currents than can transistors Not Solid State, so shorter life and less durable Slower activation time 0001 0101
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October 11, 2005ME 6405 Transistors Other times you want to amplify an analog signal Ex. Sensor input, audio, Op-amps can perform the same function Higher gains Can’t handle nearly as much current. Thus Op-amps are better for signal amplification, while Transistors are better for power amplification. Transistor as a Voltage Amplifier 0001 0110
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October 11, 2005ME 6405 Transistors Transistor as a Current Amplifier Other times you want to amplify an analog signal Ex. Sensor input, audio, Op-amps can perform the same function Higher gains Can’t handle nearly as much current. Thus Op-amps are better for signal amplification, while Transistors are better for power amplification. 0001 0111
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October 11, 2005ME 6405 Transistors Example Problem Refer to your first handout 0001 1000
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October 11, 2005ME 6405 Transistors Questions Refer to your second handout Candy!! 0001 1001
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