Chapter 4 dc biasing bjts
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Chapter 4 DC Biasing–BJTs. Biasing. Biasing: T he DC voltages applied to a transistor in order to turn it on so that it can amplify the AC signal. Operating Point. The DC input establishes an operating or quiescent point called the Q-point . The Three States of Operation.

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Chapter 4 DC Biasing–BJTs

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Chapter 4 dc biasing bjts

Chapter 4DC Biasing–BJTs


Chapter 4 dc biasing bjts

Biasing

Biasing: The DC voltages applied to a transistor in order to turn it on so that it can amplify the AC signal.


Chapter 4 dc biasing bjts

Operating Point

The DC input establishes an operating or quiescent point

called the Q-point.


Chapter 4 dc biasing bjts

The Three States of Operation

  • Active or Linear Region Operation

  • Base–Emitter junction is forward biased

    • Base–Collector junction is reverse biased

  • Cutoff Region Operation

  • Base–Emitter junction is reverse biased

  • Saturation Region Operation

  • Base–Emitter junction is forward biased

  • Base–Collector junction is forward biased


  • Chapter 4 dc biasing bjts

    DC Biasing Circuits

    • Fixed-bias circuit

    • Emitter-stabilized bias circuit

    • Collector-emitter loop

    • Voltage divider bias circuit

    • DC bias with voltage feedback


    Chapter 4 dc biasing bjts

    Fixed Bias


    Chapter 4 dc biasing bjts

    The Base-Emitter Loop

    From Kirchhoff’s voltage law:

    +VCC – IBRB – VBE = 0

    Solving for base current:


    Chapter 4 dc biasing bjts

    Collector-Emitter Loop

    Collector current:

    From Kirchhoff’s voltage law:


    Chapter 4 dc biasing bjts

    Saturation

    When the transistor is operating in saturation, current through the transistor is at its maximum possible value.


    Chapter 4 dc biasing bjts

    ICsat

    IC = VCC / RC

    VCE = 0 V

    VCEcutoff

    VCE = VCC

    IC = 0 mA

    where the value of RB sets the value of IB

    that sets the values of VCE and IC

    Load Line Analysis

    The end points of the load line are:

    The Q-point is the operating point:


    Chapter 4 dc biasing bjts

    Circuit Values Affect the Q-Point

    more …


    Chapter 4 dc biasing bjts

    Circuit Values Affect the Q-Point

    more …


    Chapter 4 dc biasing bjts

    Circuit Values Affect the Q-Point


    Chapter 4 dc biasing bjts

    Emitter-Stabilized Bias Circuit

    Adding a resistor (RE) to the emitter circuit stabilizes the bias circuit.


    Chapter 4 dc biasing bjts

    Base-Emitter Loop

    From Kirchhoff’s voltage law:

    Since IE = (b + 1)IB:

    Solving for IB:


    Chapter 4 dc biasing bjts

    Collector-Emitter Loop

    From Kirchhoff’s voltage law:

    Since IE IC:

    Also:


    Chapter 4 dc biasing bjts

    Improved Biased Stability

    Stabilityrefers to a circuit condition in which the currents and voltages will remain fairly constant over a wide range of temperatures and transistor Beta () values.

    Adding RE to the emitter improves the stability of a transistor.


    Chapter 4 dc biasing bjts

    Saturation Level

    The endpoints can be determined from the load line.

    VCEcutoff:

    ICsat:


    Chapter 4 dc biasing bjts

    Voltage Divider Bias

    This is a very stable bias circuit.

    The currents and voltages are nearly independent ofany variations in .


    Chapter 4 dc biasing bjts

    Approximate Analysis

    Where IB << I1 and I1 I2 :

    Where bRE> 10R2:

    From Kirchhoff’s voltage law:


    Chapter 4 dc biasing bjts

    Transistor Saturation Level

    Voltage Divider Bias Analysis

    • Load Line Analysis

      • Cutoff:Saturation:


    Chapter 4 dc biasing bjts

    DC Bias with Voltage Feedback

    Another way to improve the stability of a bias circuit is to add a feedback path from collector to base.

    In this bias circuit the Q-point is only slightly dependent on the transistor beta, .


    Chapter 4 dc biasing bjts

    Base-Emitter Loop

    From Kirchhoff’s voltage law:

    Where IB << IC:

    Knowing IC = IB and IE IC, the loop equation becomes:

    Solving for IB:


    Chapter 4 dc biasing bjts

    Collector-Emitter Loop

    Applying Kirchoff’s voltage law:

    IE + VCE + I’CRC – VCC = 0

    Since IC IC and IC = IB:

    IC(RC + RE) + VCE – VCC =0

    Solving for VCE:

    VCE = VCC – IC(RC + RE)


    Chapter 4 dc biasing bjts

    Transistor Saturation Level

    • Load Line Analysis

      • Cutoff:Saturation:

    Base-Emitter Bias Analysis


    Chapter 4 dc biasing bjts

    Transistor Switching Networks

    Transistors with only the DC source applied can be used as electronic switches.


    Chapter 4 dc biasing bjts

    Switching Circuit Calculations

    Saturation current:

    To ensure saturation:

    Emitter-collector resistance at saturation and cutoff:


    Chapter 4 dc biasing bjts

    Switching Time

    Transistor switching times:


    Chapter 4 dc biasing bjts

    Troubleshooting Hints

    • Approximate voltages

      • VBE .7 V for silicon transistors

      • VCE 25% to 75% of VCC

    • Test for opens and shorts with an ohmmeter.

    • Test the solder joints.

    • Test the transistor with a transistor tester or a curve tracer.

    • Note that the load or the next stage affects the transistor operation.


    Chapter 4 dc biasing bjts

    PNP Transistors

    The analysis for pnp transistor biasing circuits is the same as that for npn transistor circuits. The only difference is that the currents are flowing in the opposite direction.


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