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PULSE AND DIGITAL CIRCUITS
A. ANAND KUMAR
Advisor to
Dean Academics and Dean Quality
K.L. University
Green Fields, Vaddeswaram
Guntur District
Andhra Pradesh
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© PHI Learning Private Limited
Chapter 1
Linear Wave Shaping
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LOW-PASS RC CIRCUIT
 Transmits only low-frequency signals and attenuates or stops high-
frequency signals
• Sinusoidal Input
 This curve is obtained by keeping the amplitude of the input
sinusoidal signal constant and varying its frequency and noting
the output at each frequency.
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 The upper cut-off frequency is 70.7%, of its maximum value.
 the magnitude of the steady-state gain A is given by
 Step-Voltage Input
 The expression for the voltage across the capacitor of an RC
circuit excited by a step input is given by
vo(t) = Vfinal – (Vfinal – Vinitial)e–t/RC
 Rise time tr is proportional to the time constant RC of the
circuit.
 Rise time is inversely proportional to the upper 3-dB frequency
LOW-PASS RC CIRCUIT (Contd.)
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 Pulse Input
 A pulse shape will be preserved if the 3-dB frequency is
approximately equal to the reciprocal of the pulse width.
 Square-Wave Input
 Ramp Input
 When a low-pass RC circuit is excited by a ramp input, we have
LOW-PASS RC CIRCUIT (Contd.)
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 Exponential Input
Figure: Exponential input Figure: The low-pass RC circuit.
LOW-PASS RC CIRCUIT (Contd.)
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LOW-PASS RC CIRCUIT
 LOW-PASS RC CIRCUIT AS AN INTEGRATOR
 If the time constant of an RC low-pass circuit is very large in
comparison with the time required for the input signal to
make an appreciable change, the circuit acts as an
integrator.
 An RC integrator converts a square wave into a triangular
wave.
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HIGH-PASS RC CIRCUIT
 This circuit, also called the capacitive coupling circuit, is used to provide
dc isolation between the input and the output.
 As the frequency increases, the reactance of the capacitor decreases and
hence the output and gain increase.
Figure: The high-pass RC circuit.
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HIGH-PASS RC CIRCUIT (Contd.)
 Sinusoidal Input
 The magnitude of the steady-state gain A, and the angle q by
which the output leads the input are given by
Fig: Gain versus frequency plot.
 Step Input
 The expression for the output voltage for t > 0 is given by
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HIGH-PASS RC CIRCUIT (Contd.)
 Pulse Input
 Square-Wave Input
 A square wave may be treated as a series of positive and
negative steps.
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HIGH-PASS RC CIRCUIT (Contd.)
Figure: A square wave input.
 Ramp Input
 A waveform which is zero for t < 0 and which increases linearly
with time for t > 0 is called a ramp or sweep voltage.
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HIGH-PASS RC CIRCUIT (Contd.)
Figure: Response of the high-pass circuit for a ramp input when (a) RC >> T
and (b) RC << T.
 Exponential Input
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HIGH-PASS RC CIRCUIT (Contd.)
Figure: Response of high-pass circuit for exponential input.
 HIGH-PASS RC CIRCUIT AS A DIFFERENTIATOR
 The high-pass RC circuit acts as a differentiator provided the RC time
constant of the circuit is very small in comparison with the time
required for the input signal to make an appreciable change.
 An RC differentiator converts a triangular wave into a square wave.
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ATTENUATORS
 Attenuators are used to reduce the amplitude of the input signal.
• The decay or rise of the output (when the attenuator is not perfectly
compensated) from the initial to the final value takes place
exponentially with a time constant t = RC.
Figure: Cont.
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ATTENUATORS
Figure: Response of compensated attenuator: (a) perfect compensation,
(b) over compensation, and (c) under compensation.
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RL CIRCUITS
 RL low-pass circuit
 At very low frequencies the reactance of the inductor is small, so the
output across the resistor R¢ is almost equal to the input.
 As the frequency increases, the reactance of the inductor increases
and so the signal is attenuated.
 At very high frequencies the output is almost equal to zero.
 RL high-pass circuit
 At low frequencies, since the reactance of the inductor is small, the
output across the inductor is small
 At high frequencies the output is almost equal to the input.
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RL CIRCUITS (Contd.)
Figure: (a) RL low-pass circuit and (b) RL high-pass circuit.
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RLC CIRCUITS
 RLC Series Circuit
Figure: A series RLC circuit.
 The transfer function of the circuit is
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RLC CIRCUITS (Contd.)
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RLC CIRCUITS (Contd.)
Figure: (a) Current response and (b) voltage response of series RLC circuit to
a step voltage.
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RLC CIRCUITS (Contd.)
 RLC Parallel Circuit
 The transfer function of the network is
 The circuit is overdamped if R < 1/2 L/C, critically damped if R =
1/2 L/C and underdamped if R > 1/2 L/C.
Fig 1.77
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RINGING CIRCUIT
 A circuit, which can provide as nearly undamped oscillations as
possible is called a ringing circuit.
 If the damping is very small the circuit will ring for many cycles.
 A ringing circuit may be used to generate a sequence of pulses
regularly spaced in time.
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Puls And switching digital circuits ppt.pptx

  • 1.
    © PHI LearningPrivate Limited
  • 2.
    © PHI LearningPrivate Limited PULSE AND DIGITAL CIRCUITS A. ANAND KUMAR Advisor to Dean Academics and Dean Quality K.L. University Green Fields, Vaddeswaram Guntur District Andhra Pradesh © PHI Learning Private Limited
  • 3.
    © PHI LearningPrivate Limited Chapter 1 Linear Wave Shaping
  • 4.
    © PHI LearningPrivate Limited LOW-PASS RC CIRCUIT  Transmits only low-frequency signals and attenuates or stops high- frequency signals • Sinusoidal Input  This curve is obtained by keeping the amplitude of the input sinusoidal signal constant and varying its frequency and noting the output at each frequency.
  • 5.
    © PHI LearningPrivate Limited  The upper cut-off frequency is 70.7%, of its maximum value.  the magnitude of the steady-state gain A is given by  Step-Voltage Input  The expression for the voltage across the capacitor of an RC circuit excited by a step input is given by vo(t) = Vfinal – (Vfinal – Vinitial)e–t/RC  Rise time tr is proportional to the time constant RC of the circuit.  Rise time is inversely proportional to the upper 3-dB frequency LOW-PASS RC CIRCUIT (Contd.)
  • 6.
    © PHI LearningPrivate Limited  Pulse Input  A pulse shape will be preserved if the 3-dB frequency is approximately equal to the reciprocal of the pulse width.  Square-Wave Input  Ramp Input  When a low-pass RC circuit is excited by a ramp input, we have LOW-PASS RC CIRCUIT (Contd.)
  • 7.
    © PHI LearningPrivate Limited  Exponential Input Figure: Exponential input Figure: The low-pass RC circuit. LOW-PASS RC CIRCUIT (Contd.)
  • 8.
    © PHI LearningPrivate Limited LOW-PASS RC CIRCUIT  LOW-PASS RC CIRCUIT AS AN INTEGRATOR  If the time constant of an RC low-pass circuit is very large in comparison with the time required for the input signal to make an appreciable change, the circuit acts as an integrator.  An RC integrator converts a square wave into a triangular wave.
  • 9.
    © PHI LearningPrivate Limited HIGH-PASS RC CIRCUIT  This circuit, also called the capacitive coupling circuit, is used to provide dc isolation between the input and the output.  As the frequency increases, the reactance of the capacitor decreases and hence the output and gain increase. Figure: The high-pass RC circuit.
  • 10.
    © PHI LearningPrivate Limited HIGH-PASS RC CIRCUIT (Contd.)  Sinusoidal Input  The magnitude of the steady-state gain A, and the angle q by which the output leads the input are given by Fig: Gain versus frequency plot.  Step Input  The expression for the output voltage for t > 0 is given by
  • 11.
    © PHI LearningPrivate Limited HIGH-PASS RC CIRCUIT (Contd.)  Pulse Input  Square-Wave Input  A square wave may be treated as a series of positive and negative steps.
  • 12.
    © PHI LearningPrivate Limited HIGH-PASS RC CIRCUIT (Contd.) Figure: A square wave input.  Ramp Input  A waveform which is zero for t < 0 and which increases linearly with time for t > 0 is called a ramp or sweep voltage.
  • 13.
    © PHI LearningPrivate Limited HIGH-PASS RC CIRCUIT (Contd.) Figure: Response of the high-pass circuit for a ramp input when (a) RC >> T and (b) RC << T.  Exponential Input
  • 14.
    © PHI LearningPrivate Limited HIGH-PASS RC CIRCUIT (Contd.) Figure: Response of high-pass circuit for exponential input.  HIGH-PASS RC CIRCUIT AS A DIFFERENTIATOR  The high-pass RC circuit acts as a differentiator provided the RC time constant of the circuit is very small in comparison with the time required for the input signal to make an appreciable change.  An RC differentiator converts a triangular wave into a square wave.
  • 15.
    © PHI LearningPrivate Limited ATTENUATORS  Attenuators are used to reduce the amplitude of the input signal. • The decay or rise of the output (when the attenuator is not perfectly compensated) from the initial to the final value takes place exponentially with a time constant t = RC. Figure: Cont.
  • 16.
    © PHI LearningPrivate Limited ATTENUATORS Figure: Response of compensated attenuator: (a) perfect compensation, (b) over compensation, and (c) under compensation.
  • 17.
    © PHI LearningPrivate Limited RL CIRCUITS  RL low-pass circuit  At very low frequencies the reactance of the inductor is small, so the output across the resistor R¢ is almost equal to the input.  As the frequency increases, the reactance of the inductor increases and so the signal is attenuated.  At very high frequencies the output is almost equal to zero.  RL high-pass circuit  At low frequencies, since the reactance of the inductor is small, the output across the inductor is small  At high frequencies the output is almost equal to the input.
  • 18.
    © PHI LearningPrivate Limited RL CIRCUITS (Contd.) Figure: (a) RL low-pass circuit and (b) RL high-pass circuit.
  • 19.
    © PHI LearningPrivate Limited RLC CIRCUITS  RLC Series Circuit Figure: A series RLC circuit.  The transfer function of the circuit is
  • 20.
    © PHI LearningPrivate Limited RLC CIRCUITS (Contd.)
  • 21.
    © PHI LearningPrivate Limited RLC CIRCUITS (Contd.) Figure: (a) Current response and (b) voltage response of series RLC circuit to a step voltage.
  • 22.
    © PHI LearningPrivate Limited RLC CIRCUITS (Contd.)  RLC Parallel Circuit  The transfer function of the network is  The circuit is overdamped if R < 1/2 L/C, critically damped if R = 1/2 L/C and underdamped if R > 1/2 L/C. Fig 1.77
  • 23.
    © PHI LearningPrivate Limited RINGING CIRCUIT  A circuit, which can provide as nearly undamped oscillations as possible is called a ringing circuit.  If the damping is very small the circuit will ring for many cycles.  A ringing circuit may be used to generate a sequence of pulses regularly spaced in time.
  • 24.
    WANT TO READMORE? Get Your Copy Today from: www.phindia.com E-book at 30% OFF P-book at 20% OFF
  • 25.
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