Title: Circuits with Energy Storage Elements
1Circuits with Energy Storage Elements
2Introduction
- Circuits with energy storage elements behave
significantly differently than circuits without
energy storage elements.
3Without Energy Storage
4With Energy Storage
5Why 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.
6Important 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
7The Order of the Circuit
- The number and configuration of the energy
storage elements determines the order of the
circuit. - n ? of energy storage elements
8The 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
9The 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.
10Example RL Circuit
Find the differential equation for v(t)
11Element Currents
12KCL at the Top Node
13Example-RLC Circuit
Find the differential equation for i(t)
14Element Voltages
15KVL Around the Loop
16Building 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
17The 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
18The 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.
19Particular Solution
20Thought 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
21The Complementary Solution
- The complementary solution is the solution to
22Complementary Solution
23Initial 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.
24Effect 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.
25Initial Capacitor Voltage of 0V
26Initial Capacitor Voltage of -1V
27Initial Capacitor Voltage of 1V
28Transients 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.
29What are the Transient and Steady State Responses?