Already-charged Capacitor Voltage time function

In summary, the problem involves finding V(a) as a function of time in a circuit with a charging capacitor and a switch. The general expression for the voltage of a charging capacitor is used, but is modified to account for an initial non-zero charge on the capacitor. The Thevenin equivalent model is also used to find the effective resistance and initial potential in the circuit.
  • #1
libelec
176
0

Homework Statement



Find V(a) as a function of time in the following circuit when the switch is opened. Originally, the capacitor is charged to Vc = 1/101 * V1.

WerE1Ls.png


The Attempt at a Solution



I know that when the switch is opened, the capacitor is going to get charged again, and V(a) is going to be the same as its voltage. I know the general expression for the voltage of a charging capacitor is:

Vc(t) = V0 + V * (1 - e-t/RC)

Where Vc is the voltage of the capacitor, V0 is its original voltage, V is the voltage of the source, R the resistance and C its capacitance.

So, V(a)(t) is going to be the same as that. The problem is that I know that, in its stationary, Vc has to be equal to V, yet the expression I found doesn't do that. In this problem, I found that V0 = 0,29V, V = 30V, C = 2200μF and R... is it 100Ω? 100100Ω?

In an experiment I made (from which this questions comes), after 160 seconds V(a) was around 30V, but if I replace 160s in t in that expression, I get something closer to 17V. I thought that it has to be because I'm not calculating the R of the equivalent RC circuit right. Is that it?

Thanks
 
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  • #2
Circuit makes no sense. Opening the switch does nothing since it's permanently shorted by a wire in parallel with it.

Also, Va is shown as a source on top of the output voltage which also makes no sense.
 
  • #3
Yeah, sorry. V(a) isn't supposed to be a a source, it was just the only way I had to draw it.

This is the circuit written on the assignment, I'll edit it:

WerE1Ls.png


Pay no attention to the rest of the circuit. Just the bottom half.
 
  • #4
Nobody?
 
  • #5
I moved your thread to "Introductory Physics Homework", see the pinned thread for the difference.Concerning your question: V0 and V should be the same if the final voltage is V0. If your capacitor starts with a non-zero charge, modify the exponential instead of the prefactors:
$$V_c(t)=V_0 \left(1-e^{\frac{t-t_0}{RC}}\right)$$
Alternatively, let t=0 refer to some unknown point before the experiment starts, and determine t where the capacitor is charged to its initial voltage.
 
  • #6
The problem is that the previous voltage over the capacitor is the one it has in its stationary while the switch L1 is closed. Then when its opened, is when the experiment begins. So that rule for the voltage over the capacitor isn't valid for the previous situation while it is loading at the beginning, only when it is after the switch is opened.

Is this OK?
 
  • #7
If I understand your problem, you're worried about how the initial potential across the capacitor will affect the expression that describes the potential after the switch opens. Your equivalent circuit would look something like this:
attachment.php?attachmentid=58878&stc=1&d=1369061728.gif


The thing to do is to find the ΔV that will applies. That is, suppose the capacitor potential starts at V1 and and will head towards a final value of V2. Then ΔV = V2 - V1, and the capacitor potential will follow the curve:
$$Vc(t) = V1 + ΔV e^{-t/\tau}$$
 

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  • #8
I understand. So it would be something like:

Vc = V1 + (V2 - V1) * e-t/τ

Is this correct? One final question: the total R in this circuit, is it 10100ohm?
 
  • #9
libelec said:
I understand. So it would be something like:

Vc = V1 + (V2 - V1) * e-t/τ
Yes, see my post above
Is this correct? One final question: the total R in this circuit, is it 10100ohm?

No, the resistance that the capacitor "sees" will depend upon the position of the switch. When the switch is open, the 100Ω resistor effectively disappears from the circuit. While the switch is closed, there is a voltage divider situation. You should be able to work out the effective resistance and initial potential by finding the Thevenin equivalent model for the source and resistor network.
 
  • #10
Thank you very much.
 

Related to Already-charged Capacitor Voltage time function

1. What is an already-charged capacitor voltage time function?

An already-charged capacitor voltage time function is a mathematical representation of the voltage across a capacitor that has already been charged to a certain voltage. It shows how the voltage decreases over time as the capacitor discharges.

2. How is the already-charged capacitor voltage time function calculated?

The already-charged capacitor voltage time function is calculated using the formula V(t) = V0 * e^(-t/RC), where V(t) is the voltage at time t, V0 is the initial voltage, t is time, R is the resistance in the circuit, and C is the capacitance of the capacitor.

3. What factors affect the already-charged capacitor voltage time function?

The already-charged capacitor voltage time function is affected by the initial voltage, the resistance in the circuit, and the capacitance of the capacitor. Any changes in these factors will result in a different voltage-time relationship.

4. How does the already-charged capacitor voltage time function relate to real-life circuits?

In real-life circuits, capacitors are often used to store and discharge electrical energy. The already-charged capacitor voltage time function helps us understand how the voltage across a capacitor changes over time, which is important in designing and analyzing circuits.

5. Can the already-charged capacitor voltage time function be used for multiple capacitors in a circuit?

Yes, the already-charged capacitor voltage time function can be used for multiple capacitors in a circuit as long as they are connected in series or parallel. In series, the same current flows through each capacitor, so the voltage-time relationship will be the same. In parallel, the voltage across each capacitor will be the same, but the current will be divided among them, resulting in a different voltage-time relationship.

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