Can LC Oscillations Be Generated Using a DC Source?

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SUMMARY

The discussion focuses on generating LC oscillations using a DC source in an RLC circuit configuration. The sequence of events includes the charging of a capacitor by a battery, the role of the inductor in creating back electromotive force (emf), and the transformation of electric field energy into magnetic field energy. Key equations derived from Kirchhoff's Voltage Law (KVL) reveal that current and charge exhibit a 90-degree phase difference, with maximum charge equal to C*E and maximum current determined by the resonant angular frequency. The analysis emphasizes the need for a second-order differential equation to describe the circuit's behavior, particularly at t=0.

PREREQUISITES
  • Understanding of RLC circuit dynamics
  • Familiarity with Kirchhoff's Voltage Law (KVL)
  • Knowledge of differential equations and their applications in circuit analysis
  • Concept of phase difference in sinusoidal functions
NEXT STEPS
  • Study the derivation of the second-order differential equation for RLC circuits
  • Learn about the transient response of RLC circuits and its mathematical representation
  • Explore the concept of resonance in electrical circuits and its implications
  • Investigate the differences between AC and DC circuit behavior, particularly in energy storage components
USEFUL FOR

Electrical engineering students, circuit designers, and anyone interested in the principles of oscillatory behavior in RLC circuits.

saubhik
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Homework Statement



Suppose we have a circuit with the inductor, uncharged capacitor, ideal battery with emf E all in series. At t=0, the circuit is switched on. The following takes place sequentially:
1. Current at t=0 is max. Battery charges capacitor, current decreases.
2. inductor senses change in current, sets up back emf, decreasing the rate of current decay from exponential decay to a sinusoidal decay.
3. capacitor gets charged to max i.e. C*E. Current falls to 0.
4. inductor's back emf vanishes as current vanishes.
5. electric field energy tends to transform to magnetic field energy. Thus, capacitor discharges to the inductor.
6. the back emf set by inductor again describes the rate of change of current growth in opposite direction.
7. charge on capacitor falls to 0 and current reaches its max value, this time in opposite.
8. capacitor gets charged again and the whole process gets repeated in opposite direction for the next half cycle and so on.

Homework Equations



from above analysis, current and charge have phase diff of 90. Both sinusoidal functions.
max charge is C*E and max current is (resonant angular frequency)*(max charge).

We can get these by solving the differential equation obtained using KVL.

The Attempt at a Solution



we have an alternating current from a d.c. voltage.
Please see if my analysis is correct! also please point out if i am lacking in finer details...
I didn't know we could get AC from a DC supply.
Also i didnt find any transient characteristics of this circuit? which circuits have transient solutions?
 
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The inductor in the series circuit is not going to allow "Current at t=0 is max". So you've got a problem at step 1.

Have a look http://en.wikipedia.org/wiki/RLC_circuit" .
 
Last edited by a moderator:
yah...
that's right.
So the equations don't hold for t=0?
is that the DC transcience?

what then happens exactly at t=0; how to express this mathematically?
 
saubhik said:
yah...
that's right.
So the equations don't hold for t=0?
is that the DC transcience?

what then happens exactly at t=0; how to express this mathematically?

You just need the right equations. Write out the differential equation for the circuit and solve for the "step response". It's a second order system, characterized by containing two different passive energy storage components (the capacitor and the inductor), so you get a second order differential equation, which means it'll have characteristics like damping factors and resonance. The web page I linked to in my post above has the details.
 

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