Mathematical Model of a Circuit.

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Discussion Overview

The discussion revolves around finding the mathematical model of a direct current circuit, specifically focusing on expressing the relationship between input voltage V(t) and the output voltage across a resistor VR(1). Participants explore various equations and concepts from circuit theory, including Kirchhoff's laws and differential equations, as they attempt to derive a transfer function for the circuit.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant describes the circuit and expresses the need to find a mathematical model relating V(t) and VR(1), while noting the challenge of expressing other variables in terms of VR(1).
  • Another participant suggests that in a DC circuit, the current through the capacitor is zero, leading to simplified equations for the circuit's behavior.
  • A different viewpoint proposes that the problem involves a constant voltage applied at t = 0, leading to a gradual charge build-up on the capacitor, which affects the output voltage.
  • Several participants attempt to derive equations using Kirchhoff's laws, with one expressing frustration over not being able to isolate VR(1) in the equations.
  • Another participant provides a detailed equation but acknowledges the need to incorporate the driving voltage V(t) to proceed further.
  • Multiple participants express uncertainty about how to eliminate the capacitor voltage VC from the equations, indicating a struggle to derive a general equation in terms of VR(1).
  • One participant suggests a specific form of the equation involving VC and proposes a solution for VC when V(t) is constant.
  • Another participant reflects on their misunderstanding of the problem's requirements, indicating that the expression does not need to be in the form V(t) = ... but rather focuses on the relationship between input and output terms.

Areas of Agreement / Disagreement

Participants do not reach a consensus on how to express the mathematical model in terms of VR(1). There are multiple competing views on the approach to take, and the discussion remains unresolved regarding the best method to isolate the desired variables.

Contextual Notes

Participants reference various equations derived from Kirchhoff's laws and express limitations in their understanding of how to manipulate these equations to achieve the desired form. There is a noted dependence on the definitions of the variables involved and the conditions of the circuit.

Something Dash
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Before i start i may point a few things:

I don't know if this is college level in other places, but around here it is.
And, English is not my Native language, so bear with my mistakes...

Anyway, my class is "Mathematical Models" AKA Control Systems. It is part of physics and math, anyways, while they give me a circuit kinda looking like THIS:

http://img94.echo.cx/img94/7059/circuito0gc.png

Well, that's the circuit. It is a Direct Current circuit, and i must find the "Mathematical Model" of this circuit,


As you can see, Entrada (Input) is V(t) and the output is VR(1). While i know acording Kirkchof laws,

V(t) = VR(1) + VR(2) or

V(t) = VR1 + VC

And in this case, the R1 and R2 Resistance are Equal, so R1 = R2 = R.

In order to write a math model i only need to express it on V(t) and VR(1) (Meaning, just the Output and Input) so i need to express VR(2) or VC in terms of VR1 ONLY and not V(t) cause that doesn't make sense.

This is when i go ballistic. While if the output is V(C) or VR(2) is piece of cake, here i cannot do nothing. All i can remember and investigate is that

IR1 = IR2 + IC

VR1/R = VR2/R + C . dVC/dt (Derivate) and while is in this position, i cannot put it into terms of VR1.

I KNOW i am missing something, but it was a long time ago when i saw physics... please, you are my last line of defense, i tried all my other exercises and this one is bothering me.

The meaning of doing that is finding the "Transference Function" i need to...

Laplace Output (In this circuit pic, Salida :D )
---------------
Laplace Input (In this circuit, Entrada)


Thx beforehand, S'-
 
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If Vt is constant (DC circuit), the current through the capacitor is 0 so it is just:

It = Vt/(R1+R2)

VR1 = ItR1

VR2 = ItR2

VC = VR2

AM
 
You are talking about an input voltage that varies with time in a DC circuit. I can only assume that what you are talking about is a consant voltage that is turned on at some time we can call t = 0 and looking for the response of the circuit from that time forward. This is a classic problem in circuit theory, so I'll bet this is it.

Let E be the magnitude of the applied voltage at t = 0

At t = 0 the capacitor will have been fully discharged through R2. Now the circuit sees the constant applied voltage E, but the potential difference across the capacitor is proportional to the charge on the capacitor. It will take time for that charge to build up. The voltage on the capacitor will reach a maximum when the current through R1 is the same as the current in R2, which will be E/2 if R1 = R2. Between t = 0 and any later time, the potential on the capacitor will approach E/2 asymptotically.

The mathematical description of this is a differenctial equation that includes the current flowing into the capacitor as dq/dt where q is tha capacitor's charge. The voltage on the capacitor is qC. Can you take it from there?
 
Thanks for the attention.

Actually i kinda know the theory. What i really need is an equation that is expresed as

V(t) = THE DIFERENCIAL EQUATION

The only variables that could go there is the Output, as VR1 on this case.

THis is where i can't advance. The idea is to make a general equation, and i really take it from there.

What equations can i get from Kirkchof laws?

V(t) = VR1(t) + VC(t)
IR = IR + IC ...(1)
VR2 = VC

If the output where in case, VC(t) the problem is easily solved.

From equation (1)

VR1/R = VR2/R + C . dVC/dt

VR1/R = VC/R + C . dVC/dt

VR1 = VC + RC . dVC/dt

Then i replace.

V(T) = VC + RC . dVC/dt + VC =>

V(T) = 2VC + RC . dVC/dt

As you see, this is the math model from the same circuit but the output is really VC. If it's VR2 it's easy using the same equations. Maybe i am missing some equations i cannot remember? I just need the equation...
 
How's this? Be sure to check my work, but I think this is it

V(t) = V1(t) + V2(t) = I(t)R1 + Vc(t)
I(t) = I1(t) = I2(t) + Ic(t)
I2(t) = Vc(t)/R2
Ic(t) = dq(t)/dt = CdVc(t)/dt
I(t) = Vc(t)/R2 + CdVc(t)/dt
V(t) = R1*[Vc(t)/R2 + CdVc(t)/dt] + Vc(t)
V(t) = Vc(t)*(R1+R2)/R2 + (R1*C)dVc(t)/dt

This is the same as yours for R1 = R2 = R

This is all you can do until you put in the driving voltage V(t). Then solve the DE for Vc(t)
 
Last edited:
:smile: Thanks for your help, but it isn't enough...

All those equations i knew them, all of them, and i can't really put the general V(t) equation in terms of VR1 or V1 as you put it only... all those equations i tried them, played with them and i cannot see another else... :rolleyes:

Well, i am going to keep researching till i get this done, and if you remember something up please post!
 
Something Dash said:
:smile: Thanks for your help, but it isn't enough...

All those equations i knew them, all of them, and i can't really put the general V(t) equation in terms of VR1 or V1 as you put it only... all those equations i tried them, played with them and i cannot see another else... :rolleyes:

Well, i am going to keep researching till i get this done, and if you remember something up please post!

There is no avoiding the dependence of V1(t) on Vc(t). If that is what you are trying to do, it will not happen.

V(t) = V1(t) + Vc(t)
V1(t) = V(t) - Vc(t)
dV1(t)/dt = dV(t)/dt - dVc(t)/dt

If you know the driving function V(t) then you can find the first term, but you are stuck with the dVc(t)/dt term. You can also replace dV(t)/dt by taking the derivative of the result already obtained.

V(t) = Vc(t)*(R1+R2)/R2 + (R1*C)dVc(t)/dt
dV(t)/dt = [(R1+R2)/R2]*dVc(t)/dt + (R1*C)d^2Vc(t)/dt^2

dV1(t)/dt = [(R1+R2)/R2]*dVc(t)/dt - (R1*C)d^2Vc(t)/dt^2 - dVc(t)/dt
dV1(t)/dt = [R1/R2]*dVc(t)/dt - (R1*C)d^2Vc(t)/dt^2
 
Something Dash said:
:smile: Thanks for your help, but it isn't enough...

All those equations i knew them, all of them, and i can't really put the general V(t) equation in terms of VR1 or V1 as you put it only... all those equations i tried them, played with them and i cannot see another else... :rolleyes:

Well, i am going to keep researching till i get this done, and if you remember something up please post!
I think Dan is right.

[tex]V(t) = V_c(t)\frac{(R1+R2)}{R2} + (R1*C)\frac{dV_c(t)}{dt}[/tex]

If R1=R2:

[tex]V(t) = 2V_c(t) + (RC)\frac{dV_c(t)}{dt}[/tex]

[tex]\frac{dV_c(t)}{dt} + \frac{2}{RC}V_c(t) = \frac{V(t)}{RC}[/tex]

You have to solve that for V_c. I get:

[tex]V_c = \frac{V(t)}{2}(1-e^{-2t/RC}) - \frac{1}{RCe^{2t/RC}}\int_0^t (V'(t)\frac{RC}{2}(e^{2t/RC}-1)dt[/tex]

If V(t) is constant = V:

[tex]V_c = \frac{V}{2}(1 - e^{-2t/RC})[/tex]

AM
 
Yes, i cannot find the way of killing Vc.

Tomorrow if i can i will try to solve this in a test, and one way or another i will bring the answer here (Maybe i am not expressing my problem correctly)

Thanks guys.

S'
 
  • #10
Something Dash said:
Yes, i cannot find the way of killing Vc.

Tomorrow if i can i will try to solve this in a test, and one way or another i will bring the answer here (Maybe i am not expressing my problem correctly)'
Just substitute the expression for V_c into the equation for total current:

[tex]I_t = V_1/R_1 = \frac{V(t)-V_c}{R_1}[/tex]

[tex]I_tR_1 = V(t) - (\frac{V(t)}{2}(1-e^{-2t/RC}) - \frac{1}{2e^{2t/RC}}\int_0^t (V'(t)(e^{2t/RC}-1)dt)[/tex]

AM
 
  • #11
Well i was wrong, it didn't have to be expresed into Vt =... just Input terms = Output. Hopfully i won the test.
 

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