8. Damping and the Natural Response in RLC Circuits

7_2ndODE_damp__1.png

Consider a series RLC circuit (one that has a resistor, an inductor and a capacitor) with a constant driving electro-motive force (emf) E. The current equation for the circuit is

MATH MATH

[or the equivalent MATH]

Differentiating, we have

MATH

This is a second order linear homogeneous equation.

Its corresponding auxiliary equation is MATH with roots:

MATH

MATH


MATH

MATH

Now

α = R/2L is called the damping coefficient of the circuit

MATH is the resonant frequency of the circuit.

m1 and m2 are called the natural frequencies of the circuit.

The nature of the current will depend on the relationship between R, L and C.

There are three possibilities:

Case 1: R2 > 4L/C (Over-Damped)

7_2ndODE_damp__22.png

Here both m1 and m2 are real, distinct and negative. The general solution is given by

MATH

The motion (current) is not oscillatory, and the vibration returns to equilibrium.

Case 2: R2 = 4L/C (Critically Damped)

7_2ndODE_damp__28.png

Here the roots are negative, real and equal,

i.e. m1 = m2 = -R/2L.

The general solution is given by

MATH

The vibration (current) returns to equilibrium in the minimum time and there is just enough damping to prevent oscillation.

Case 3: R2 < 4L/C (Under-Damped)

7_2ndODE_damp__32.png

Here the roots are complex where

MATH

The general solution is given by

MATH

where

α = R/2L is called the damping coefficient

MATH

In this case, the motion (current) is oscillatory and the amplitude decreases exponentially, bounded by

plus minus

as we can see in the diagram above.

When R = 0, the circuit displays its natural or resonant frequency MATH.

Example

In a series RCL circuit driven by a constant emf, the natural response of the circuit is given by

MATH

for which the initial conditions are i(0) = 2 A and $\dfrac{di}{dt}$ at t = 0 is 4.

State the nature of response of the current and hence solve for i.

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