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Transistor (BJT)

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Page 1: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor (BJT)

Page 2: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Introduction

• BJT (Bipolar Junction Transistor)• Vaccum tubes• It comes because it is most advantageous in amplification• Why it is called transistor?

Transistor = Transfer + Resistor• Why it is called BJT?• Types of BJT

Page 3: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Introduction(cont.)

npn pnp

n p n

B

C p n pE

B

C

Cross Section

B

C

E

Schematic Symbol

B

C

E

Schematic Symbol

• Collector doping is usually ~ 109

• Base doping is slightly higher ~ 1010 – 1011

• Emitter doping is much higher ~ 1017

Page 4: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Junction Transistor

• Sandwich structure.• Base is always in between E & C.• B is lightly doped.• E & C are heavily doped. E is more heavily doped than C and area of C

is more than E.• Two PN junctions.

E

B

C

BE CB

E

B

C

BE CB

N-P-N P-N-P

Page 5: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Unbiased transistor

• No external supply is applied.• Penetration of depletion region (less in E & C, more in B)

Page 6: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor Biasing

• Mode BE junction BC junction

• cutoff reverse biased reverse biased

• linear(active) forward biased reverse biased

• saturation forward biased forward biased

• Inverse active reverse biased forward biased

Page 7: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor Biasing (cont.)

• Transistor biasing in active region.• EB junction is forward biased and CB junction is reversed biased.

Page 8: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor operation in active region (NPN)

E

B

CN P N

v

Page 9: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

9

Large current

Page 10: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor operation (cont.)

• Electrons will flow from E to B.• Now electrons have three options

1. Recombine with holes (IB)2. Diffuse through base and out of the base connection.3. Remaining e- will go in C (Ic).

Page 11: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor operation (cont.)

E

B

CN P N

Electrons emitted

Electrons collected

Recombination current

Emitter current

Collector current

IE=IB+IC

Page 12: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor current

• Emitter current, Base current, Collector current.• IE = IB + IC. (IE ≈ IC)

• IE = IPE + INE (for NPN INE for PNP IPE).• IB = IPE - IPC.• Reverse saturation current (ICBO) : It is the reverse sat. current when EB

junction is open.• IC = IPC + ICBO.

Page 13: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Parameters relating to current components• Emitter efficiency (ɣ) = • Transport factor (ß) = • Large signal current gain (α) = • α = =• α = ß * ɣ

Page 14: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor as an amplifier

i i B

o L C

v R i

v R i

Discussion of an amplification effect

CEBEi L

B C

vvR R

i i

B Ci iWith i ov v

50 ~ 300ov

i

vA

v

E.g. for common-base configuration transistor:

Page 15: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor construction technologies

• Grown type.• Alloy type.• Electrochemically etched type.• Diffusion type• Epitaxial type.

Page 16: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor configuration

• Made one of three terminal common to i/p and o/p.• Depending on which terminal is made common. There are three

possibilities1. Common base configuration (CB).2. Common emitter configuration (CE).3. Common collector configuration (CC).

Page 17: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Common Base configuration (CB)

Vee Vcc

Re Rc

IE

IB

IC

Vee Vcc

Re Rc

IE

IB

IC

Common base configuration forNPN transistor

Common base configuration forPNP transistor

Page 18: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Common Base configuration (CB)• Input• Output• Current relations in CB configuration

1. Ic = IC(INJ) + ICBO

2. IC(INJ) (practically)3. ICBO (with emitter open)ICB= collector to base current IO = emitter is open

Page 19: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Common Base configuration (CB)

4. current amplification factor/current gain (αdc) αdc =IC(inj)/IE

So Ic = (αdc * IE ) + ICBO

Expression for IB: IB = (1- α)IE.

Page 20: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transistor char in CB configuration

1. Input char. 2. Output char. 3. Transfer char. • I/P char : graph of I/P current versus I/P voltage.• O/P char : graph of O/P current versus O/P voltage.• Transfer char: graph of O/P current versus I/P current

Page 21: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

CB I/P char.

• I/P current is emitter current(IE) and I/P voltage is emitter to base voltage(VBE).

1. Its identical to VI char of diode in FB.

2. Up to cut-in V3. I/P resistance4. Effect of VCB on I/P VI char (Early effect)

VCB = 4V

VCB = 8VIE (mA)

VBE

Page 22: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Early effect / Base width modulation

• Effect on β and α.

E B C E B C

Increase VCB

Total base width = width of depletion region at CB junction + width of region which contains free charge carriers

Page 23: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Output char of transistor in CB

IC

Active Region

Saturation RegionCutoff RegionIB = 0

IE

VCB

Operating region

1. Cutoff region2. Active region3. Saturation region

Page 24: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Output char of transistor in CB

• Cut off region : region below the curve IE =0• Active region : IC ≈ IE (Const. current source)• Dynamic O/P resistance• Saturation region • Current controlled current source.

Page 25: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Breakdown voltage and punch-through effect• Increasing VCB causes CB junction to breakdown.• Reach through / Punch through effect

VCB

IC

E B C

Page 26: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Potential variation through transistor

Without biasing

With external bias

Page 27: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transfer characteristic

• Linear rela.tionship IC

IE

Page 28: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Common Emitter (CE) configuration

VccVcc

VBEVCE

RBRC

VBB VBBVBE

VCE

RC

RB

Common emitter config. for NPN transistor

Common emitter config. for PNP transistor

Page 29: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

CE Configuration

• Input• Output• Current relation

IE = IB + IC IC = α * IE + ICBO

IC = IB (α/1- α) + ICBO / (1- α)But (α/1- α) = β

So IC = IB * β + (β+1) ICBO

IC = IB * β + ICEO

Page 30: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

CE Configuration

• Reverse leakage current in CE configuration (ICEO)• Thermal instability, so thermal stabilizing circuit is required.• Relation between α and β. α = β/(1+ β) and β = α /(1- α)

Page 31: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

CE characteristics (Input)

• Same as conventional PN junction diode• Dynamic i/p resistance• Base current reduces as VCE

increases.VCE = 8V

VCE = 4VIB (μA)

VBE

Page 32: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

CE characteristics (output)

VCE (V)

IC(mA)

IB = 50 A

IB = 0

30

5 10 15 20 0

0

IB = 100 A

IB = 150 A

IB = 200 A

22.5

15

7.5

Saturation Region

Active Region

Cutoff Region

1. Cut off region2. Active region3. Saturation region4.Dynamic O/P resistance5. Definition of β6. Maximum VCE and breakdown

Page 33: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transfer characteristic

• Why CE o/p char is more sloping than CB o/p char???

IC

IB

VCE = 2V

VCE = 5V

Page 34: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Typical transistor junction voltage values• Cutoff region• Short-circuited base• Open-circuited base• Cut-in voltage• Saturation voltage

Voltage Si transistor Ge transistor

VBE (Cutoff)

0 -0.1

VBE (Cut in)

0.5 0.1

VBE (active)

0.7 0.2

VBE (sat.) 0.8 0.3

VCE (sat.) 0.2 0.1

Page 35: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Standard test for regions

• Saturation region1. find IC, IB then check IB >= IC/ β

2. measure VCB, positive for PNP and negative for NPN.

• Active regionmeasure VBE = 0.7 and measure VCB is negative (reverse biased)

• CutoffVBE is < 0.5 and VCB is negative

Page 36: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Common collector configuration

VccVcc

VBCVEC

RBRE

VBB VBBVBC

VECs

RERB

Page 37: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Practical way to draw CC config.

VCC

O/P voltage

I/P voltage

Page 38: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Current relation

• IE = IB + IC IC = α * IE + ICBO

IE = (β+1) * IB

Current gain γ = IE /IBMaximum use of CC is for impedance matching (I/P is high and O/P is low).

Page 39: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

I/P char. And O/P char.

VEC = 2V

VEC = 1VIB (μA)

VBC

IE

Active Region

Saturation RegionCutoff RegionIB = 0

IB

VEC

Page 40: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Transfer char.

IE

IB

VCE = 2V

VCE = 5V

Page 41: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Comparison of configurations

parameter CB CE CC

Common terminal between i/p and o/p

Base Emitter Collector

I/P current IE IB IB

O/P current IC IC IE

Current gain α = IC/IE β= IC/IB Γ= IE/IB

I/P voltage VEB VBE VBC

O/P voltage VCB VCE VEC

Page 42: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Analytic expression for transistor char.• IC = -αN * IE – ICO ()

subscript N to α is transistor is being used in normal mode.For the inverted mode of operation

IE = -αI * IC – IEO ()

Page 43: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Base spreading resistance

E

B

C

VCE

VEBVCB

VCB = VC + rbb * IBVE VC

Page 44: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Ebers – moll model

VE VC

IE

IB

IC

αI IC αN IE

Page 45: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Ebers – moll model (cont.)

• I = IC + αN IE

IC = - αN IE + I(I is diode current)

VC

αN IE

IC

I

I = I0 ()

Now Take, I0 = -ICO , V = VC and n=1

So I = -ICO ()

Page 46: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Why can’t we construct a transistor by connecting back to back diodes?

VE VC

Page 47: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Photo transistor

Dark current

20 mW/(cm* cm)

40 mW/(cm* cm)

60 mW/(cm* cm)

80 mW/(cm* cm)

Page 48: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Photo transistor (cont.)

• Advantages: • Photo current multiplied by β• High sensitivity• Good switching speed• No memory effect.

Page 49: Transistor (BJT). Introduction BJT (Bipolar Junction Transistor) Vaccum tubes It comes because it is most advantageous in amplification Why it is called

Phototransistor (cont.)

• Disadvantages• Not so fast as conventional transistor because of photo-

conducting material• Poor linearity• Temperature sensitive device• External voltage source is needed for operation