Second order ODE for RLC circuit

Click For Summary
SUMMARY

The discussion focuses on deriving the second-order ordinary differential equation (ODE) for an RLC circuit using Kirchhoff's voltage law. The equation is represented as L(Q''(t)) + R(Q'(t)) + (Q(t))/C = 0, leading to the characteristic equation LM² + MR + (1/C) = 0. The roots are calculated as m = [-R/L ± sqrt((R/L²) - 4(1)(1/LC))]/2, which influences the behavior of the charge on the capacitor over time. The expected solution involves a combination of decaying exponentials and sinusoidal functions, specifically Q(t) = Ae^(-Bt)cos(w't + θ), where B = R/2L, indicating that the discriminant determines the nature of the solution.

PREREQUISITES
  • Understanding of second-order ordinary differential equations (ODEs)
  • Familiarity with RLC circuit theory and components (Resistor, Inductor, Capacitor)
  • Knowledge of Kirchhoff's voltage law
  • Basic concepts of characteristic equations and their roots
NEXT STEPS
  • Study the derivation of the characteristic equation for second-order linear ODEs
  • Explore the impact of the discriminant on the solutions of second-order ODEs
  • Learn about the behavior of RLC circuits under different damping conditions
  • Investigate the application of Laplace transforms in solving RLC circuit equations
USEFUL FOR

Electrical engineers, physics students, and anyone interested in circuit analysis and differential equations will benefit from this discussion.

icesalmon
Messages
270
Reaction score
13
if I consider a circuit consisting of a capacitor, an inductor and a resistor and using kirchhoffs voltage rule for the circuit i come up with the following

L(Q''(t)) + R(Q'(t)) + (Q(t))/C = 0 I solve for the roots using a characteristic equation of the form
LM2 +MR +(1/C) = 0
solving this for m I obtain
m = [-R/L +/- sqrt((r/l2) - 4(1)(1/LC))]/2
i'm expecting an equation using both decaying exponentials and sinusoids so that the energy will tend towards zero after a long time. But this depends on the values of R, C and L. I'm having trouble moving forward from this point in deriving the equation for the charge on the capacitor as a function of time.
Q(t) = Ae-Btcos(w't+θ)
B = R/2L
 
Last edited:
Engineering news on Phys.org
so obviously the characteristic equation doesn't directly lead to that damped charge motion then, it depends on the discriminant. I thought I was SUPPOSED to get the decaying exponential out of it. Anyways, thanks.
 

Similar threads

  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 40 ·
2
Replies
40
Views
7K
Replies
14
Views
2K
Replies
44
Views
6K
  • · Replies 22 ·
Replies
22
Views
2K
  • · Replies 29 ·
Replies
29
Views
2K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 27 ·
Replies
27
Views
3K
  • · Replies 3 ·
Replies
3
Views
4K