lecture6 diode circuits applications.ppt

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Diode Circuits: Applications

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  • Diode Circuits:
    Applications

    *

  • Applications Rectifier Circuits

    Half-Wave Rectifier Circuits

    *

  • Applications Rectifier Circuits

    Battery-Charging Circuit

    *

  • Half-Wave Rectifier with Smoothing Capacitor

    Large Capacitance

    i=dq/dt or Q = IL T

    Q = Vr C

    then

    C ~ (ILT) / Vr

    *

  • Half-Wave Rectifier with Smoothing Capacitor

    Large Capacitance

    Forward bias

    charge cycle

    Reverse bias

    discharge cycle

    Start

    Vr Peak-to-peak riple voltage

    i=dq/dt or Q = IL T

    Q = Vr C

    then

    C ~ (ILT) / Vr

    typically :VL ~V m- (Vr /2)

    *

  • Full-Wave rectifier Circuits

    The sources are out of phase

    *

  • Wave Shaping Circuits Clipper Circuits

    Batteries replaced by Zener diodes

    Review examples:

    10.14

    10.15

    10.16

    10.17

    10.18

    *

  • Half-Wave Limiter Circuits

    Current flows thru the resistor until +600 mV is reached, then flows thru the Diode.

    The plateau is representative of the voltage drop of the diode while it is conducting.

    Voltage

    divider

    + 600 mV

    I flow below 600 mV

    I flow Above 600 mV

    - 600 mV

    *

  • Linear Small Signal Equivalent Circuits (1)

    When considering electronic circuits in which dc supply voltages are used to bias a nonlinear devices at their operating points and a small ac signal is injected into the circuit to find circuit response:

    Split the analysis of the circuit into two parts:

    analyze the dc circuit to find the operating pointconsider the small ac signal

    *

  • Linear Small Signal Equivalent Circuits (1)

    Since virtually any nonlinear ch-tic is approximately linear (straight) if we consider a sufficiently small segment

    THEN

    We can find a linear small-signal equivalent circuit for the nonlinear device to use in the ac analysis

    The small signal diode circuit can be substituted by a single equivalent resistor.

    *

  • Linear Small Signal Equivalent Circuits (2)

    dc supply voltage results in operation at Q

    An ac signal is injected into the circuit and

    swings the instantaneous point of operation

    slightly above and below the Q point

    For small changes

    DiD the small change in diode current from the Q-point

    DvD the small change in diode voltage from the Q-point

    (diD/dvD) the slope of the diode ch-tic evaluated at the point Q

    *

  • Linear Small Signal Equivalent Circuits (2)

    dc supply voltage results in operation at Q

    An ac signal is injected into the circuit and

    swings the instantaneous point of operation

    slightly above and below the Q point

    For small changes

    DiD the small change in diode current from the Q-point

    DvD the small change in diode voltage from the Q-point

    (diD/dvD) the slope of the diode ch-tic evaluated at the point Q

    Dynamic resistance of the diode

    *

  • From small signal diode analysis

    Differentiating

    the Shockley eq.

    and following the math on p.452 we can write that dynamic resistance of the diode is

    Linear Small Signal Equivalent Circuits (3)

    where

    *

  • Example - Voltage-Controlled Attenuator

    DC control signal

    C1, C2 small or large ?

    C in dc circuit open circuit

    C in ac circuit short circuit

    Find the operating point and perform the small signal analysis to obtain the small signal voltage gain

    *

  • Example - Voltage-Controlled Attenuator

    DC control signal

    Dc circuit for Q point (IDQ, VDQ)

    Compute at the Q point (IDQ, VDQ)

    *

  • Example - Voltage-Controlled Attenuator

    The dc voltage source is equivalent to a short circuit for ac signals.

    Voltage gain

    *

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