Finding the Resonant frequency in an LC circuit

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Homework Help Overview

The discussion revolves around deriving an expression for the resonance frequency in an LC circuit, specifically addressing a configuration involving two capacitors and one inductor. Participants are exploring the implications of the circuit setup and the relationships between charge, current, and voltage in the context of oscillatory motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants attempt to set up differential equations using Kirchhoff's Voltage Law and question the impact of having two capacitors in the circuit. There is a discussion on the significance of initial conditions and the polarities of the capacitors. Some participants suggest modifications to the equations to account for the two capacitors, leading to different expressions for ω².

Discussion Status

There is an ongoing exploration of the correct expression for the resonance frequency, with some participants providing guidance on the implications of the circuit configuration. Questions about the meaning of variables, such as charge (q), are raised, indicating a productive inquiry into the underlying concepts.

Contextual Notes

Participants note the significance of the polarities of the capacitors and the initial conditions, which may affect the current and voltage relationships in the circuit. There is an acknowledgment of the complexity introduced by having two capacitors instead of one.

bsr25
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Homework Statement


The figure opposite shows a free oscillator composed of an LC circuit. Derive an expression for the resonance frequency. Show all of your working.



Homework Equations



d2x/dt2 + ω2x = 0


The Attempt at a Solution


First I tried using Kirchoffs Voltage Law to set up a differential equation defining the circuit.

L(d2q/dt2) + Q1/C + Q2/C = 0

I then combined the two voltages across the capcitor, and divided by L

(d2q/dt2) + QTotal/LC = 0

Comparing this to the equation for SHM:

d2x/dt2 + ω2x = 0

shows that ω2= 1/LC.

But I figure this cannot be the case as that is the result expected for a simple LC circuit with one inductor and one capcitor. As this is two capcitors and one inductor I figure the rsult must be different.

One thing I notice on the diagram is the Capcitors have both negative plates facing each other, I wasnt sure what effect if any this would have on the circuit.

Other than this attempt at a solution which I am fairly sure if way off, I am a bit lost. Any help towards reahcing the right answer would be greatly appreciated!

Thanks
 

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bsr25 said:

Homework Statement


The figure opposite shows a free oscillator composed of an LC circuit. Derive an expression for the resonance frequency. Show all of your working.



Homework Equations



d2x/dt2 + ω2x = 0


The Attempt at a Solution


First I tried using Kirchoffs Voltage Law to set up a differential equation defining the circuit.

L(d2q/dt2) + Q1/C + Q2/C = 0

Q1 and Q2 are meant to be initial conditions.

Replace Q1 and Q2 with q and away you go.

P.S. yes there is significance to the polarities of Q1 and Q2. If Q1 = Q2 there would be no current unless an initial current were also specified. The two capacitors would buck each other's voltage out like two batteries connected back-to-back.
 
So if isntead I said:

L(d2q/dt2) + q/C + q/C = 0

(d2q/dt2) + q*(2/LC) = 0

ω2 = 2/LC

Would that be correct?
 
bsr25 said:
So if isntead I said:

L(d2q/dt2) + q/C + q/C = 0

(d2q/dt2) + q*(2/LC) = 0

ω2 = 2/LC

Would that be correct?

It surely would! :smile:
 
Sweet. Many thanks for your help!

My next query would be as to what q is exactly. For example in a mass on a spring, the equation of motion is d2x/dt2 + ω2x = 0 and x is the displacement of the mass. Is q the charge across the inductor or one fo the capcitors or ... ?
 
bsr25 said:
Sweet. Many thanks for your help!

My next query would be as to what q is exactly. For example in a mass on a spring, the equation of motion is d2x/dt2 + ω2x = 0 and x is the displacement of the mass. Is q the charge across the inductor or one fo the capcitors or ... ?

Charge q is defined by i = dq/dt = current. Current is the same everywhere around the loop.
And therefore in any given time interval t, total charge flowing past any point along the circuit is also the same.

Let's call the left-hand capacitor C1 and the right-hand one C2. Then we sum voltage drops around the loop = 0:

V(C1)0 - (1/C1)∫0ti(t')dt' - Ldi/dt - V(C2)0 - (1/C2)∫0ti(t')dt' = 0. Note that current is leaving C1 and entering C2 which explains the polarities I used. V(C1)0 and V(C2)0 are the initial voltages on the two capacitors.

So looking at this, what is the first intergal ∫tidt'? It's just charge q leaving C1 in time t since current is flowing OUT OF C1. And the second integral is charge entering C2 in time t, which is the same charge q. And both those charge quantities must flow thru L, but the voltage across L is Ldi/dt = Ld2q/dt2. So, in time t, q leaves C1, flows thru L, and enters C2 and we wind up with

-q/C1 - Ld2q/dt2 -q/C2 = V(C2)0 - V(C1)0.

which is the full diff. eq. including the initial conditions on C1 and C2.

I can't give you a good picture why mass should be analogous to inductance, etc. etc. except to point out that the mathematical equations are similar.
 

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