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SMV ELECTRIC TUTORIALS Aditya Kuroodi 2016 Relevant Course(s): EE121B, EE115A
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INTRODUCTION TO TRANSISTORS
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Transistors: BJTs & MOSFETs There are 2 main types of transistors: Bi-Polar Junction Transistors and Metal- Oxide Semiconductor Field Effect Transistor For each transistor type, there are 2 variations Combined effect of transistors revolutionzed electronics We will focus less on the semiconductor theory behind transistors and more on their functionality BJTsMOSFETs
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The PN Junction: Forward and Reverse Bias If you hook up + terminal of battery to P-Type, and – terminal to N-Type you will forward bias the junction Forward bias repels majority carriers back into depletion zone, causing depletion zone to shrink (due to recombination) and that lets current flow easily If you hook up – terminal of battery to P-Type, and + terminal to N-Type, you will reverse bias the junction Reverse bias attracts majority carriers to terminals, expanding the depletion zone and impeding current flow
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(Junction) Diodes A diode is a device that only allows current to flow in one direction, it is achieved through a PN junction The blue arrow represents conventional current flow (opposite of electron flow) + -
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Bi-Polar Junction Transistor (BJT) Add an extra semiconductor layer to a junction diode and you get BJT BJT is a 3 layered (doped) semiconductor sandwich, can either be PNP or NPN variety A BJT is a current-controlled current regulator The main current flows from Emitter to Collector (PNP) or Collector to Emitter (NPN) The controlling current flows from Emitter to Base (PNP) or Base to Emitter (NPN) You control the main current by varying how much base current you supply to the BJT The above arrows represent electron flow
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Bi-Polar Junction Transistor (BJT) The little arrow on Emitter always points in direction of conventional current flow Emitter current = Base current + Collecter current by KCL BJTs are “bi-polar” because they use both carrier types (electrons + holes) When base current is 0 (or less than threshold current), transistor is in cutoff (fully nonconducting) When base current at max, transistor is saturated (fully conducting) To conduct NPN: have to pull Base high relative to Emitter To conduct PNP: have to pull Base low relative to Emitter Since electron mobility > hole mobility, NPN is more common Controlled current flows through the 2 outer layers, not base layer How to differentiate the two BJTs: N ot- P ointing-i N = NPN PNP NPN
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BJT as a Switch Note: BJTs actually have 5 operating modes (not just cutoff or saturation) For our purposes we will deal mostly with cutoff and saturation regions, enabling us to use the BJT as a progressive switch The tiny signal picked up from microphone (imagine a clap), once rectified, can be used to bias the base of the transistor on and turn on the lamp Now we can use tiny current to control a much larger current (amplification) NOTE: The battery provides the larger current, not the transistor (no magic) The louder the clap, the brighter the bulb (active mode). That is, until we reach saturation
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The Field Effect Transistor (JFET, FET) FETs are voltage-controlled current regulators 3 terminals: Gate, Drain, Source 2 varieties: N-Channel (NMOS) and P-Channel (PMOS) FETs, unlike BJTs, are unipolar devices (one major carrier for main current) As you vary Gate voltage, current through Drain and Source will vary
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JFET (vs BJT) & MOSFETs JFETs have high input impedance, meaning little current flows through base in operation (minimum impact on rest of circuit, unlike BJT) JFETs have less amplification abilities than BJTs JFETs, unlike BJTs, are restrictive devices When left untouched, transistor will be normally closed As you throttle “base” voltage, main controlled current will decrease MOSFETs fall under the larger branch of Junction FETs MOSFETs are JFETs with even higher input impedance Come in either depletion mode or enhancement mode Enhancement mode MOSFETs act like BJTs (normally open, amplify current when throttled)
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The (Enhancement Mode) MOSFET N-Channel MOSFET Arrow points inwards ON when gate bias voltage (gate to source) > threshold voltage When gate votlage equal to 0, transistor is ON Source often connected to GND, load attached to Drain (low-side switching) Lower ON resistance than P-Channel P-Channel MOSFET Arrow points outwards ON when gate bias voltage < threshold voltage When gate voltage equal to 0, transistor is OFF Source often connected to load, Drain connected to GND (high-side switching)
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MOSFET as a Switch Suppose we want to turn a lamp (or LED) on and off with a MOSFET Using N-Channel, we connect Source to GND Load placed between voltage rail and the MOSFET Input voltage pulses, either biases gate- source to saturation or leaves transistor open When gate voltage high, lamp is on Special safety precautions must be taken if load is NOT purely resistive (for power switching) Inductive load requires voltage spike protection Capacitive load requires inrush current limitaion NOTE: VDD >> Vin
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MOSFET Power Switching Considerations Inductors, when quickly powered off, will generate huge voltage spike in opposition to decreasing current V = L *di/dt Use FlyBack Diode (Snubber, Supression, Flywheel, etc.) to protect circuitry (including the MOSFET!) Now current flows through diode, back through inductor and slowly dies down from resistive losses Capacitive loads will draw in large current when first connected to voltage rail (capacitors act like shorts initially) Simply place resistor in series with whatever you want to protect to limit inrush current (an NTC thermistor better than static resistor) NTC thermistors start with high resistance, then lower resistance as they heat up NOTE: by definition, motors are inductive loads!
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BJTs & MOSFETs BJT Superior for use in amplifiers Requires both voltage and current to drive Since current-controled, sometimes the additional current affects rest of circuit Bottom Line: BJTs usable (cheaper, stable) for lower power applications MOSFET Superior for power supply regulators Higher switching frequency, so better for high power applications Requires only voltage to drive Higher gate impedance (so draws in little current), little impact on rest of circuit Easier to use with MCUs that have digital outputs Bottom Line: MOSFETs preferrable for higher performance (aside from amplifiers) or high power applications
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OTHER TYPES OF DIODES
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Other Diodes + Applications So far we’ve discussed the general diode (a.k.a. junction diode) As you start to use transistors in circuits, you will start to see many more types and applications of diodes Each diode type has it’s own symbol and functionality, we will briefly cover a few of the common types now Zener Diode Schottky Diode Light Emitting Diode Schottky Diode + -
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Zener/Avalanche Diode Avalance breakdown: A semiconductor phenomona where large current flows in an otherwise insulating material (when you reverse bias A LOT) Zener diodes are built to safely operate in breakdown region, in addition to acting like a normal diode during forward biasing Zener votlage: a reduced breakdown voltage for Zener diodes The Zener diode, when in breakdown, will maintain its Zener voltage over a wide range of currents Ex: A 3V Zener will output 3V when in breakdown, (almost) regardless of current Applications: Voltage Regulation, Waveform Clipper, TVS
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Schottky Diode Schottky diodes charecterized by low forward voltage drop and fast switching Instead of ~.7V drop for a normal Silicon based diode, Schottkys have ~.15V to.45V drop However, their low voltage ratings make them unsuitable for high power applciations Small voltage drop means they are more power efficient Fast switching makes them suitable for high frequency applications (RF devices and SMPS)
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Light Emitting Diode (LED) LEDs are diodes that light up when forward biased Specially construct PN junction (not just Si) with materials that glow when current passed through them The long lead of an LED is the anode (+)
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