1 st Order Circuits. Objective of the Lecture Explain the transient response of a RC circuit As the capacitor stores energy when there is: a transition.

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Presentation transcript:

1 st Order Circuits

Objective of the Lecture Explain the transient response of a RC circuit As the capacitor stores energy when there is: a transition in a unit step function source, u(t-t o ) or a voltage or current source is switched into the circuit. Explain the transient response of a RL circuit As the inductor stores energy when there is: a transition in a unit step function source, u(t-t o ) or a voltage or current source is switched into the circuit. Also known as a forced response to an independent source

RC Circuit I C = 0A when t < t o V C = 0V when t < t o Because I1 = 0A (replace it with an open circuit).

RC Circuit Find the final condition of the voltage across the capacitor. Replace C with an open circuit and determine the voltage across the terminal. I C = 0A when t ~ ∞ s V C = V R = I 1 R when t ~ ∞ s

RC Circuit In the time between t o and t = ∞ s, the capacitor stores energy and currents flow through R and C.

RL Circuit

RL Circuit (con’t) Initial condition is not important as the magnitude of the voltage source in the circuit is equal to 0V when t ≤ t o. Since the voltage source has only been turned on at t = t o, the circuit at t ≤ t o is as shown below. As the inductor has not stored any energy because no power source has been connected to the circuit as of yet, all voltages and currents are equal to zero.

RL Circuit So, the final condition of the inductor current needs to be calculated after the voltage source has switched on. Replace L with a short circuit and calculate I L (∞).

Final Condition

RL Circuit

Electronic Response Typically, we say that the currents and voltages in a circuit have reached steady-state once 5  have passed after a change has been made to the value of a current or voltage source in the circuit. In a circuit with a forced response, percentage-wise how close is the value of the voltage across a capacitor in an RC circuit to its final value at 5  ?

Complete Response Is equal to the natural response of the circuit plus the forced response Use superposition to determine the final equations for voltage across components and the currents flowing through them.

Example #1 Suppose there were two unit step function sources in the circuit.

Example #1 (con’t) The solution for Vc would be the result of superposition where: I2 = 0A, I1 is left on The solution is a forced response since I1 turns on at t = t1 I1 = 0A, I2 is left on The solution is a natural response since I2 turns off at t = t2

Example #1 (con’t)

If t1 < t2

General Equations When a voltage or current source changes its magnitude at t= 0s in a simple RC or RL circuit. Equations for a simple RC circuit Equations for a simple RL circuit

Needed to Complete HW # 21

How to renew your MatLAB license If you would like to contact them directly, SWAT is located at: 2080 Torgersen Hall Office Hours: 12:00pm to 4:00pm Monday - Friday Phone: (540)

Introductory Tutorials MathWorks ( haswww.mathworks.com On-line tutorials including A Very Elementary MATLAB Tutorial ml Videos (look at the ones below Getting Started) Worked examples (further down the demos page) Textbook has a MatLAB tutorial in Appendix E.

Summary The final condition for: the capacitor voltage (V o ) is determined by replacing the capacitor with an open circuit and then calculating the voltage across the terminals. The inductor current (I o ) is determined by replacing the inductor with a short circuit and then calculating the current flowing through the short. The time constant for: an RC circuit is  RC and an RL circuit is  L/R The general equations for the forced response of: the voltage across a capacitor is the current through an inductor is

Summary General equations when the magnitude of a voltage or current source in the circuit changes at t = 0s for the: voltage across a capacitor is current through an inductor is Superposition should be used if there are multiple voltage and/or current sources that change the magnitude of their output as a function of time.