Chapter 4
Bipolar junction transistor
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Bipolar junction transistor 1 Objectives Describe the basic - - PowerPoint PPT Presentation
Chapter 4 Bipolar junction transistor 1 Objectives Describe the basic structure of the bipolar junction transistor (BJT) Explain and analyze basic transistor bias and operation operation Discuss the parameters and
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There are two types of transistors:
The terminals are labeled:
pnp
npn
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Biasing:
transistor properly.
active operation as an amplifier.
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Transistor Voltages:
collector of transistor.
ground connection.
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Transistor Voltages:
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Transistor Voltages:
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Emitter current is the sum of the collector and base currents:
Current gain (β) factor by which current increases from base of transistor to its collector.
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Cutoff region
transistor junctions are reverse biased.
large depletion region between C-B and E-B, reverse current, ICEO passes from emitter to collector and can be neglected.
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Saturation region
transistor junctions are forward-biased.
determined by VCC and total resistance in C-E circuit. resistance in C-E circuit.
is independently from relationship of β and IB.
VCE < VBE.
E C CC C
R R V I + =
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Active region
junction is forward biased and the BC junction is reverse biased.
measurable value. measurable value.
the values of β and IB.
and VCE falls in ranges VBE<VCE<VCC.
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Transistor Operating Regions: 1.Cutoff region:
to zero. Since ICEO neglected, VCE = VCC 2.Active region:
3.Saturation:
the component in the CE circuit, and independent
β β
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Emitter and collector currents:
I ≅ I C E
Base-emittervoltage:
VBE = 0.7 V (for Silicon)
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Alpha (α) is the ratio of IC to IE :
IE α I = C dc
Ideally: α = 1 Ideally: α = 1 In reality: α is between 0.9 and 0.998
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In DC mode: β represents the amplification factor of a transistor. (β is sometimes referred to as hfe, a term used in transistor modeling calculations) β = IC I B
dc
Relationship between amplification factors β and α
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β β + 1 α = α α −1 β = Relationship Between Currents
IC = βIB
IE = (β + 1)IB
Current and Voltage Analysis:
When the BE junction is forward-biased, like a forward biased
diode and the voltage drop is
Since the emitter is at ground (0V), by Kirchhoff’s voltage law, the
voltage across is: …….(1)
B
R
BE BB R
V V V
B
− =
voltage across is: …….(1)
Also, by Ohm’s law:
……..(2)
From (1) ->(2) : Therefore, the dc base current is:
B
R
BE BB R
V V V
B
− =
B B R
B =
B B BE BB
B BE BB B
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Current and Voltage Analysis:
is:
C
R CC CE
C C RC
is:
C C CC CE
BE CE CB
C
C C RC
B DC C
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DC Load Line:
Cutoff and saturation can be illustrated in relation to the collector characteristic curves by the use of a load line. DC load line drawn on the connecting cutoff and saturation point. The bottom of load line is ideal cutoff where IC=0 & VCE=VCC. The top of load line is saturation
The top of load line is saturation where IC=IC(sat) & VCE =VCE(sat) In between cutoff and saturation is the active region of transistor’s
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Collector Characteristic Curve:
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A transistor when used as a switch is simply being biased so that it is in:
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Conditions in Cutoff
CC cutoff CE
) (
Neglect leakage current and all currents are zero. BE junction is reverse biased.
C sat CE CC sat C
) ( ) (
DC sat C B
) ( (min) =
Conditions in Saturation Since VCE(sat) is very small compared to VCC, it can be neglected.
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Provides a graph of the characteristic curves.
Some DMMs measure βDC or hFE.
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