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Circuits with Energy Storage Elements

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Title: Circuits with Energy Storage Elements


1
Circuits with Energy Storage Elements
2
Introduction
  • Circuits with energy storage elements behave
    significantly differently than circuits without
    energy storage elements.

3
Without Energy Storage
4
With Energy Storage
5
Why is This?
  • In a circuit with energy storage elements,
    voltages and currents are the solutions to
    linear, constant coefficient differential
    equations.
  • Real engineers almost never solve the
    differential equations directly.
  • It is important to have a qualitative
    understanding of the solutions.

6
Important Concepts
  • The order of the circuit
  • Forced and natural (homogeneous) responses
  • Transient and steady state responses
  • 1st order circuits-the time constant
  • 2nd order circuits-natural frequency and the
    damping ratio

7
The Order of the Circuit
  • The number and configuration of the energy
    storage elements determines the order of the
    circuit.
  • n ? of energy storage elements

8
The Differential Equation
  • Every voltage and current is the solution to a
    differential equation.
  • In a circuit of order n, these differential
    equations have order n.
  • Equations are linear, constant coefficient

9
The Differential Equation
  • The coefficients an through a0 depend on the
    component values of circuit elements.
  • The function f(t) depends on the circuit elements
    and on the sources in the circuit.

10
Example RL Circuit
Find the differential equation for v(t)
11
Element Currents
12
KCL at the Top Node
13
Example-RLC Circuit
Find the differential equation for i(t)
14
Element Voltages
15
KVL Around the Loop
16
Building Intuition
  • Even though there are an infinite number of
    differential equations, they all share common
    characteristics that allow intuition to be
    developed
  • Particular and complementary solutions
  • Effects of initial conditions
  • Roots of the characteristic equation

17
The Solution to the Differential Equation
  • The solution to any differential equation
    consists of two parts
  • v(t) vp(t) vc(t)
  • Particular (forced) solution is vp(t)
  • Response particular to a given source
  • Complementary (natural) solution is vc(t)
  • Response common to all sources

18
The Particular Solution
  • The particular solution is a solution to
  • The particular solution is usually has the form
    of a sum of f(t) and its derivatives.

19
Particular Solution
20
Thought Question
  • What form for the particular solution would you
    expect for the following functions?
  • f(t) 10 cos(2p 377t)
  • f(t) 20 e-0.001t

21
The Complementary Solution
  • The complementary solution is the solution to

22
Complementary Solution
23
Initial Conditions
  • The particular and complementary solutions have
    constants that cannot be determined without
    knowledge of the initial conditions.
  • The initial conditions are the initial value of
    the solution and the initial value of one or more
    of its derivatives.
  • Initial conditions are determined by initial
    capacitor voltages, initial inductor currents,
    and initial source values.

24
Effect of Initial Conditions
  • I computed vc(t) in the IF Amplifier filter in
    response to a step input.
  • The initial inductor current is zero.
  • Three initial capacitor voltages were used 0V,
    -1V, and 1V.

25
Initial Capacitor Voltage of 0V
26
Initial Capacitor Voltage of -1V
27
Initial Capacitor Voltage of 1V
28
Transients and Steady State
  • The steady state response of a circuit is the
    waveform after a long time has passed.
  • DC SS if response approaches a constant.
  • AC SS if response approaches a sinusoid.
  • The transient response is the circuit response
    minus the steady state response.

29
What are the Transient and Steady State Responses?
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