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Chi tiết về transistor BJT

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Tiêu đề BJT – Bipolar Junction Transistors
Chuyên ngành Electronics
Thể loại Lecture
Định dạng
Số trang 58
Dung lượng 2,01 MB

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Nội dung

Chi tiết về transistor BJT. dành cho sinh viên kỹ thuật điện-điện tử.

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Intro to Systems

Transfer function

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Transfer functions

Poles, Zeros factorization

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Response function of poles

Response function

Stable operation ==> No poles on right half-plane

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Block Diagrams

Output is integral of inputIntegrator

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Laplace Transforms

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Inverse Laplace Transforms

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Application to Linear Systems

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Frequency Domain Analysis

• Step 1: Obtain Transfer function of circuit H(s)

• Step 2: Apply Laplace Transform to vin(t) to obtain Vin(s)

• Step 3: Multiply Vin(s) by H(s) to obtain Vout(s)

• Step 4: Apply Inverse Laplace Transfom to Vout(s) to obtain vout(t)

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BJT – Bipolar Junction Transistors

• p+ > p, n+ > n  emitter, collector NOT interchangeable!!!

• base width small compared to minority

carrier diffusion length

 NOT just back to back diodes:

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Transistor Band Structure:

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Applying VBC:

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Forward Biasing Base-Emitter Diode:

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Currents in Forward Active Mode:

IE = IB + IC

VEB + VBC + VCE = 0

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Currents in Forward Active Mode:

pnptransistor

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Configurations:

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Transistor Uses:

Switch: cut-off, saturation Amplifier: forward-active

VCE (V) 0

5 10 15

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Transistor Ratings:

• Power Dissipation

– Power generated from transistor currents

• AC Current Gain

– Gain calculated under AC signal conditions

• Maximum Emitter-Base Voltage

– Maximum reverse voltage before breakdown

• Maximum Collector Current

– Maximum allowable continuous current

• Maximum Collector-Emitter Voltage

– Maximum current before breakdown

• Maximum Collector-Base Voltage

– Maximum reverse bias before breakdown

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Common Packagings:

Looking from below:TO-92 examples when seen as to the left:

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forward voltage drop

 0.7 Vreverse current

~ nAreverse breakdown voltage

I = I0 e

e kT

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Diode - Dynamic Impedance:

V >> nTk/e Voltage input signal change  impedance:

Room temperature  kT/e  25mV

V n

V n = I enkT

dV

dI = Zd = kT

eI = 25mV

I

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What region?

Given: npn with  = 100

1.) IB = 50 μA, IC = 3 mA?

 saturation: IC < IB2.) IB = 50 μA, VCE = 5V?

 active: IB > 0 and VCE > 0.2 V3.) VBE = -2V, VCE = -1V?

cut off: VBE < 0 and VBC = VBE –VCE = -1V < 0

i.e both reverse biased…

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BJT circuit analysis:

guess operating mode: active, saturated, cut off?

i.e.: is BE forward or reverse biased?

reverse biased  cut off

forward biased  assume active: vBE = 0.7V

use: iE = iC + iB, iC = iB; compute: vCE

if vCE < 0.2V  saturation; redo calculation with vCE = 0.2V

vBE = 0.8V

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BJT amplifier biasing:

1.) choose a collector current IC:

typical: 1 – 10mA (small signal: 0.1 mA)2.) determine the supply voltage vs (5V, 9V, 12V, …)

amplifier  active region!!!

3.) choose an operating point:

typical: 10% of vs  RE = 0.1vs/IC4.) base voltage: VB = ICRE + 0.7V (Si)

 RC = (vs – VC)/IC

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Review of BJT Equations:

iE = iC + iB VCE = VCB + VBEKirchhoff:

iC = ISe

VBE

VT

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Cutoff and Saturation

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Cutoff

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Transistor as amplifier

Vary Input voltage > Vary IbaseCauses VCE to move along load line > Amplification

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Transistor as a switch

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