Derive the governing equation for the voltage Vc across the capacitor

In summary: Can you explain explicitly? I still believe there can be current from a to b...There is no potential difference between a and b if the two circuits are not connected to the same ground.
  • #1
annamal
387
33
Homework Statement
Derive the governing equation for the voltage Vc across the capacitor
Relevant Equations
KCL and KVL
I was thinking about doing KVL around the circuit at the right but I noticed when the switch opens, the current through the circuit at the right is not the same throughout
-5 + Ic*2*1-^3 + Ic*10^3 = -Vc

Ic is not the same around the right circuit so I am stuck....

Screenshot 2023-04-23 at 4.41.25 PM.png
 
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  • #2
Hi,

I suppose you did part a and you have ##V_c## and ##I_L## at ##t\uparrow\infty## ?

annamal said:
-5 + Ic*2*1-^3 + Ic*10^3 = -Vc
Care to explain this ? In particular the second term ?
I can't even read it " ##I_c * 2 * 1 - ?^3 ## "?
Do you mean ##I_{b_2} * 2\ k\Omega## ?

I also think you need some more relevant equations ...

##\ ##
 
  • #3
BvU said:
I suppose you did part a and you have Vc and IL at t↑∞ ?
Please note that the problem is oddly stated and the time of interest (steady state) is t <0.
 
  • #4
hutchphd said:
Please note that the problem is oddly stated and the time of interest (steady state) is t <0.
I agree.
 
  • #5
BvU said:
Hi,

I suppose you did part a and you have ##V_c## and ##I_L## at ##t\uparrow\infty## ?Care to explain this ? In particular the second term ?
I can't even read it " ##I_c * 2 * 1 - ?^3 ## "?
Do you mean ##I_{b_2} * 2\ k\Omega## ?

I also think you need some more relevant equations ...

##\ ##
Yeah, I meant KVL:
-5 + Ic*2*10^3 + Ic*10^3 = -Vc

I know what part a is. I am wondering about part b.
 
  • #6
So the 1 and 2 ##k\Omega## resistors have the same current ?

And do you mean ##I_c = I_{b_2} ## ?

##\ ##
 
  • #7
BvU said:
So the 1 and 2 ##k\Omega## resistors have the same current ?

And do you mean ##I_c = I_{b_2} ## ?

##\ ##
I don't know if the resistors have the same current -- that is just an attempt of mine. In fact I think the resistors might have different current.
 
  • #8
Backing up: do you have ##V_C## and ##I_L## for ##t<0## ?
And for ##t\uparrow\infty## ?

##\ ##
 
  • #9
BvU said:
Backing up: do you have ##V_C## and ##I_L## for ##t<0## ?
And for ##t\uparrow\infty## ?

##\ ##
I only know Vc = 3 V; I_L =0.0015 A for t < 0
 
  • #10
Agreed. Now, when the switch is opened, can there still be a current through the 3 ##k\Omega## ?

##\ ##
 
  • #11
BvU said:
Agreed. Now, when the switch is opened, can there still be a current through the 3 ##k\Omega## ?

##\ ##
I think it can though...why can it not?
 
  • #12
Wouldn't the left circuit and the right circuit be isolated from each other ?

1682344794325.png


(thought experiment: imagine the 2 mH wasn't an inductor but a resistor)

##\ ##
 
  • #13
BvU said:
Wouldn't the left circuit and the right circuit be isolated from each other ?

View attachment 325426

(thought experiment: imagine the 2 mH wasn't an inductor but a resistor)

##\ ##
I still don't understand why the current in the middle is zero....if I do KCL at point a or b, it seems like there could be current there....
 
  • #14
annamal said:
I still don't understand why the current in the middle is zero....if I do KCL at point a or b, it seems like there could be current there....
Like here
1682345972722.png
?

##\ ##
 
  • #15
BvU said:
Like here
View attachment 325428 ?

##\ ##
Can you explain explicitly? I still believe there can be current from a to b...
 
  • #16
There is no potential difference between a and b if the two circuits are not connected to the same ground.

[edit] or do KVL for each of the loops ....
 
  • #17
A circuit is called a circuit because there is a return path that completes the circle.
Without the return path, there can be no current in R=3k.
The value of R=3k becomes irrelevant and may as well be a short circuit.
Nodes a and b will then have the same voltage.
 
  • Like
Likes BvU
  • #18
Baluncore said:
A circuit is called a circuit because there is a return path that completes the circle.
Without the return path, there can be no current in R=3k.
The value of R=3k becomes irrelevant and may as well be a short circuit.
Nodes a and b will then have the same voltage.
I don't understand. I drew the circle and currents in blue below:
1682344794325.png
 
  • #19
annamal said:
I don't understand. I drew the circle and currents in blue below:
Would you expect a light globe to work if you only connected one wire to the battery?
 
  • #20
Another tack: what do you find for ##V_C## and ##I_L## for ##t>>0## ?

##\ ##
 
  • #21
First, if the start process is finished the current through L will be d.c. that means ω=2*π*f=0 then the voltage drop through L will be 0.

On the capacitor eventually, after infinite time, the current will be 0 since Zcap=1/ ω/cap and if ω=0 Zcap=∞

Second, if sw1 is open that it is like instead sw1 a resistance of ∞ ohms is inserted here. So, in the loop between a and b the current it is total voltage drop [what ever it is] in the loop divided by ∞ [no current will flow here].
 

Attachments

  • Infinite resistance.jpg
    Infinite resistance.jpg
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  • #22
By-the-way, if between two points in a circuit the voltage drop is 0 then the potential V1=V2. The voltage drop =Z*I. If Z=0 or I=0 the voltage drop is 0.:smile:
 
  • #23
It is not so complicate. You have to find Vc=-(5-Vo)*e^(-γ*t)+5 like formula where Vo it is Vc before sw1 opening.
 

Related to Derive the governing equation for the voltage Vc across the capacitor

What is the basic form of the governing equation for the voltage across a capacitor?

The basic form of the governing equation for the voltage Vc across a capacitor is derived from the relationship between current, capacitance, and voltage. It is given by the differential equation: I = C(dVc/dt), where I is the current through the capacitor, C is the capacitance, and dVc/dt is the rate of change of voltage across the capacitor.

How do you derive the governing equation for Vc in an RC circuit?

To derive the governing equation for Vc in an RC (resistor-capacitor) circuit, you start with Kirchhoff's voltage law (KVL), which states that the sum of voltages around a closed loop is zero. For a series RC circuit, this gives: V - IR - Vc = 0. Using Ohm's law (V = IR) and the capacitor current equation (I = C(dVc/dt)), you can rewrite this as V - R(C(dVc/dt)) - Vc = 0. Simplifying, you get the governing differential equation: V = RC(dVc/dt) + Vc.

What initial conditions are needed to solve the governing equation for Vc?

To solve the governing equation for Vc, you need the initial voltage across the capacitor, Vc(0). This initial condition is crucial because it allows you to integrate the differential equation and find the specific solution that fits the physical scenario of your circuit.

How does the governing equation change for an AC circuit involving a capacitor?

In an AC circuit, the voltage and current are time-dependent and typically sinusoidal. The governing equation for the voltage across a capacitor in an AC circuit involves complex impedance. The voltage Vc(t) can be found using phasor analysis, where Vc(t) = Vc_peak * sin(ωt + φ), and the governing equation in the frequency domain is Vc = I/(jωC), where ω is the angular frequency, and j is the imaginary unit.

Can the governing equation for Vc be applied to non-linear capacitors?

The governing equation I = C(dVc/dt) assumes a linear relationship between charge and voltage. For non-linear capacitors, where capacitance varies with voltage, the equation must be modified to account for the variable capacitance. This is often expressed as I = d(Q(Vc))/dt, where Q(Vc) is the charge as a function of voltage. The differential equation then becomes more complex and may require numerical methods to solve.

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