RLC Circuit Differential Equation problem

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Discussion Overview

The discussion revolves around deriving the differential equation for an RLC circuit with given parameters. Participants explore the relationships between input and output voltages using Kirchhoff's Voltage Law, addressing both theoretical and practical aspects of circuit analysis.

Discussion Character

  • Homework-related
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents an initial attempt at deriving the differential equation using Kirchhoff's Voltage Law, expressing relationships between voltages across the resistor, capacitor, and inductor.
  • Another participant questions the correctness of the substitution made for the inductor current and suggests that the resulting equation is not correct, indicating that a second-order equation is expected for an RLC circuit.
  • A participant expresses confusion about the nature of second-order systems compared to first-order systems, questioning the feasibility of rearranging the relationships to derive a second-order differential equation solely based on voltage and time.
  • Several participants engage in clarifying the relationships between current and voltage across the components, with one stating that the current is equal across all parts in a series connection, referencing Kirchhoff's current law.
  • Another participant proposes a specific form of the second-order differential equation, confirming the expected structure of the equation involving derivatives of the output voltage.

Areas of Agreement / Disagreement

Participants express differing views on the correctness of the initial derivation and the substitutions made. There is no consensus on the initial approach, but some participants agree on the form of the second-order differential equation that should result from the analysis.

Contextual Notes

Participants note that the derivation involves assumptions about the relationships between current and voltage in the circuit, and there is acknowledgment of potential mistakes in earlier substitutions. The discussion reflects the complexity of transitioning from first-order to second-order systems in circuit analysis.

MathsDude69
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Homework Statement



For a RLC circuit with RC = 1/2 and LC = 1/16 determine the differential equation that describes the relationship between the input and output voltages. An image of the circuit is shown with RLC all in series with the input voltage Vi(t) across all 3 components. The voltage drop across the capacitor is labelled Vo(t)

Homework Equations



Kirchoff's Voltage Law

The Attempt at a Solution



From Kirchoff's voltage law:

Vi(t) = Vr(t) + Vc(t) + Vl(t)

Vr(t) = Rir(t) = RC(Vc(t))' = RC(Vo(t))' Using the prime to indicate differentiation

The voltage drop across the resistor can now be descirbed as above henceforth we now have:

Vi(t) = RC(Vo(t))' + Vc(t) + Vl(t)

Given that Vc(t) = Vo(t) we can also write:

Vi(t) = RC(Vo(t))' + Vo(t) + Vl(t)

The voltage drop across the inductor can be expressed as:

Vl(t) = L(il(t))' and as ir = ic = il Vl(t) = LC(Vo(t))'

Henceforth the differential equation is:

Vi(t) = RC(Vo(t))' + Vo(t) + LC(Vo(t))'Is this solution correct or have I flamingo'd up somewhere?

Homework Statement


Homework Equations


The Attempt at a Solution

 
Last edited:
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Can you upload the image of the circuit?
 
Sure. Here you go.
 

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I hate these questions. Have you considered that V = L(di/dt) and i = C(dv/dt)?
 
MathsDude69 said:
The voltage drop across the inductor can be expressed as:

Vl(t) = L(il(t))' and as ir = ic = il Vl(t) = LC(Vo(t))
You made a mistake here when you substituted for il.
Henceforth the differential equation is:

Vi(t) = RC(Vo(t))' + Vo(t) + LC(Vo(t))'
This isn't correct either. You will get a second-order equation for an RLC circuit.
 
Im guessing then that it should be along the lines of:

L*d2i/dt2 + R*di/dt + 1\C*i

what is confusing is that all the information I have pertains to RL/RC circuits which are first order systems.

Is it even possible to rearrange a second order system such as this to obtain a second order differential equation using only the relationship between voltage and time?

The whole purpose of this exercize is to find the laplace transform and then the laplace frequency response H(s). :-s
 
You almost had it with your original attempt. Just go back and do the math a little more carefully.

How did you go from VL(t)=L(iL(t))', which is correct, to VL(t)=LC(Vo(t)), which is incorrect?
 
Last edited:
vela said:
You almost had it with your original attempt. Just go back and do the math a little more carefully.

How did you go from VL(t)=L(iL(t)), which is correct, to VL(t)=LC(Vo(t)), which is incorrect?

I assumed that in a series connection that the current was equal between all parts, thus the magnitude of the current given by the voltage drop across the capacitor would also indicate the level of current in the inductor. But then again you know what they say about assumption :-p

The only other example I have is an LR circuit which stipulates that:

iL(t) = iL(0-) + 1/L * integral between 0- and t of VL(tau)d(tau) .. (sorry I am not too sure how to do the mathematical signs)

Should I sustitue this into the original equation??
 
MathsDude69 said:
I assumed that in a series connection that the current was equal between all parts
This is right. It's a consequence of Kirchoff's current law.
thus the magnitude of the current given by the voltage drop across the capacitor would also indicate the level of current in the inductor.
What you mean by this part isn't so clear to me. Could you provide an equation for what you mean?
 
  • #10
Sure. I figured ic(t) = C*(VC(t))'

In my case VC(t) and VO(t) are the same quantity.
 
  • #11
OK, so VL(t)=L(iL(t))'=L(iC(t))'=...?
 
  • #12
vela said:
OK, so VL(t)=L(iL(t))'=L(iC(t))'=...?

...erm... L(C*(Vc(t))'') ??
 
  • #13
Right, so you end up with

Vi = LC V''o + RC V'o + Vo

which is the second-order differential equation you want.
 
  • #14
Awsome. Thanks a lot!
 

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