Approaching capacitor circuit question

In summary: The thing about capacitors in DC circuits is that, when they reach steady state they also reach their final charge and potential difference; their current goes to zero as their charge stops changing.So you can analyze the circuit by pretending that the capacitor isn't there!Is there a way to determine the potential difference in the circuit without the capacitor?I have no idea.
  • #1
RoboNerd
410
11
part1.jpg
part2.jpg
1. Homework Statement


The problem is above, I am having a hard time figuring out why the right answer for part F is "greater than."

Homework Equations



Ucapacitor = 0.5 * C * V^2

The Attempt at a Solution


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My problem is figuring out the logic in how the capacitor's energy would increase. Now, I know that because I have a resistor with a smaller resistance that the total current in the circuit will increase. That is not a problem.

The constant of the capacitor remains the same, and because the R1 and C are in parallel, they have the same voltage drop across it. The battery's voltage remains the same so by Kirchoff, I would have:

EMF - (Itot * R2New) - (votlage drop across R1 or capacitor). The EMF remains the same. Itot increases while R2NEW decreases, so I do not know if the voltage drop across the capacitor will increase or decrease.

Could anyone please help in figuring out this problem? Thanks in advance!
 
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  • #2
What determines the final voltage across the capacitor?
 
  • #3
Voltage on capacitor = The charge on it divided by its capacitance.
 
  • #4
RoboNerd said:
Voltage on capacitor = The charge on it divided by its capacitance.
Allow me to clarify my question. What circuit elements determine the final voltage on the capacitor?
 
  • #5
the emf of the battery and the voltage drop across Resistor R2 by Kirchoff's voltage law
 
  • #6
RoboNerd said:
the emf of the battery and the voltage drop across Resistor R2 by Kirchoff's voltage law
Okay, how do you determine that voltage drop across R2 at steady state?
 
  • #7
R2 * Itotal
 
  • #8
RoboNerd said:
R2 * Itotal
And what is Itotal?
 
  • #9
EMF / R1?

IDK. ITOTAL varies with time
 
  • #10
RoboNerd said:
EMF / R1?

IDK. ITOTAL varies with time

Ah. No. The total current varies with time only until the circuit reaches steady state (which is why the problem statement uses words like "after a long time", or "the switch remains closed for a long time"). When the circuit reaches steady state all transient phenomena have finished and only steady currents and voltages remain. No more changes to currents or voltages anywhere in the circuit.

I'm getting the feeling that perhaps you're missing a key concept that would make this problem much clearer, and easier for you to figure out.

The thing about capacitors in DC circuits is that, when they reach steady state they also reach their final charge and potential difference; their current goes to zero as their charge stops changing. With no current flowing into or out of the capacitor it is effectively an open circuit. At that point you can in fact remove the capacitor from a circuit without disturbing the steady state of the circuit. So you can analyze the circuit by pretending that the capacitor isn't there! Just determine what the potential would be between nodes where the capacitor connects if the capacitor were not there.
 
  • #11
gneill said:
The total current varies with time only until the circuit reaches steady state

Yes, meant that, but I forgot to verbalize it specifically in words. Sorry about that.

When the total charge builds up on the capacitor, there is no current going across it, so we are going to have the "effective current" going through the battery and through R1 and R2.

I total is thus: EMF / (R1 + R2), right?

But then I do not understand how this would lead me to conclude that there is greater energy in the capacitor
 
  • #12
RoboNerd said:
But then I do not understand how this would lead me to conclude that there is greater energy in the capacitor
How does the energy stored in a capacitor relate to the potential difference across the capacitor? (What's the formula?)

RoboNerd said:
When the total charge builds up on the capacitor, there is no current going across it, so we are going to have the "effective current" going through the battery and through R1 and R2.

I total is thus: EMF / (R1 + R2), right?
Sure. So how does this relate to the potential across the capacitor? What potential difference in that string of components (EMF, R2, R1) is the same as that of the capacitor? How does it vary if R2 is varied?
 
  • #13
Take a look at the graph. It shows the capacitor is charging towards 12V rather than the 20V of the battery. Ask yourself what controls the final voltage on the capacitor.
 
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  • #14
Energy = 1/2 * C * V^2
gneill said:
Sure. So how does this relate to the potential across the capacitor?

I have no idea.

I do know that current through R1 multiplied by R1 equals voltage dropa cross capacitor.

If R2 varies, the potential across R1 and thus the capacitor varies. If the R2 decreases, the potential difference across it decreases, but potential difference across the capacitor increases?

CWatters said:
Take a look at the graph. It shows the capacitor is charging towards 12V rather than the 20V of the battery.
This discrepancy looks fishy. I noticed that but I do not know what to do about it
CWatters said:
Ask yourself what controls the final voltage on the capacitor.

I have no idea. The charge on it controls it. How do I move on with figuring it out?
 
  • #15
RoboNerd said:
I do know that current through R1 multiplied by R1 equals voltage dropa cross capacitor.

If R2 varies, the potential across R1 and thus the capacitor varies. If the R2 decreases, the potential difference across it decreases, but potential difference across the capacitor increases?

Correct, and that allows you to state how the energy stored on the capacitor changes and answer the question.

CWatters said:
Take a look at the graph. It shows the capacitor is charging towards 12V rather than the 20V of the battery. Ask yourself what controls the final voltage on the capacitor.

RoboNerd said:
This discrepancy looks fishy. I noticed that but I do not know what to do about it

It's not fishy at all. It tells you that the voltage at t=∞ on the junction of the two resistors is 12V. When a capacitor is fully charged no current flows into it so it can be removed from the circuit without effecting the voltage at the junction of the two resistors. If you are you familiar with the "potential divider" circuit (eg your circuit but without the capacitor) you can calculate R2.
 
  • #16
CWatters said:
If you are you familiar with the "potential divider" circuit (eg your circuit but without the capacitor) you can calculate R2.

Yes, I can calculate R2. Doing that led me to figure out that R2 = 1000 ohms because 12 volts = 15000 ohms * Itotal [considering that the total current does not flow through the cap. anymore because it has reached a steady state]

OK.

Now for my question in response to:
RoboNerd said:
If R2 varies, the potential across R1 and thus the capacitor varies. If the R2 decreases, the potential difference across it decreases, but potential difference across the capacitor increases?

I assume that my capacitor has reached steady state. we thus have a closed circuit composed of a battery and R2 and R1, where we have a current running through it and the voltage drop across R1 is a constant number.

I thus need to have a voltage drop of 8 volts across R2. Decreasing the resistance of R2 will increase the total current, so the voltage drop over R2 will be:

V = Itot * R2. But then with one variable decreasing in value and the other variable increasing in value, how can we know if the voltage drop across it will increase or decrease?

Thanks for putting up with me and I apologize if it takes me some time in trying to figure out the answer and why the other answers are wrong
 
  • #17
Can't you just use the voltage divider of R1 and R2?
To get the voltage drop across R2, you multiply the source voltage (20 V, in your case) times the divider ratio of (R2)/(R1 + R2).
When R2 decreases, both the numerator and the denominator of that ratio decreases. But which one decreases faster - the numerator or the denominator? That will tell you whether the voltage is increasing or decreasing.
 
  • #18
+1

Just use the potential divider rule. If R2 reduces the voltage at the junction of R1 and R2 increases. So the energy in the capacitor increases. It's that simple. No need to worry about the current...

Vc=20*R1/(R1+R2)

So if R2 gets smaller Vc gets bigger.
 
Last edited:
  • #19
TomHart said:
Can't you just use the voltage divider of R1 and R2?
To get the voltage drop across R2, you multiply the source voltage (20 V, in your case) times the divider ratio of (R2)/(R1 + R2).
When R2 decreases, both the numerator and the denominator of that ratio decreases. But which one decreases faster - the numerator or the denominator? That will tell you whether the voltage is increasing or decreasing.

CWatters said:
Just use the potential divider rule.

I can not say that I am familiar with the concept. Would you be so kind as to recommend a good resource that you know is the best for understanding this concept?
I think if I get this voltage divider concept, I can then progress and solve this problem. Please correct me if I am wrong.Thanks for putting up with me and my slow progress in trying to reach the goal of cracking this problem.
Thanks for the help and patience!
 
  • #20
It really is a simple concept so I will try to explain it. If the voltage across two series resistors is known, the voltage drop across each individual resistor can be calculated by this "voltage divider" calculation.

Let's say I have a circuit that consists of a DC voltage source at a voltage of Vdc Volts, connected to a resistor R2, that is connected to another resistor R1, which connects to the low potential side of the DC voltage source, thus completing the circuit. (It would be the exact circuit you have in your original problem statement if the switch and capacitor were removed.)

For that circuit, the voltage gets divided across those 2 resistors as follows:
The voltage across R2 will be VR2 = (Vdc)(R2)/(R1 + R2).
And the voltage across R1 will be VR1 = (Vdc)(R1)/(R1 + R2).

The voltage gets divided between the two resistors according to the size of the resistors - the larger resistor having the larger voltage drop.
 
  • #21
So it is sort of like the fraction of the resistor in question divided by the total resistance. Right?
Instead of having voltage drop across resistor 2 = Itotal * R2 we just solve for Itotal using the same expression for resistor 1 and plug it in.

I understand the concept. Thanks for explaining it!

voltage drop across r2 is thus = total voltage * R2 / (R1 + R2)
voltage drop across r1 is thus = total voltage * R1 / (R1 + R2)

Thus the voltage drop across r2 will decrease and voltage drop across r1 will increase as R2 decreases, so the voltage drop across the capacitor increases, increasing its energy.

Right?
 
  • #22
When the switch is closed and the circuit has reached steady state (in other words, when the capacitor is fully charged), there will be no current flowing to the capacitor and the voltage across the cap will be equal to the voltage across R1 - whatever that voltage happens to be.

NOTE: The voltage divider only applies when the circuit has reached steady state.
 
  • #24
Thanks for the help everyone.

So changing resistor R2 will make the voltage divider increase and the energy in the cap. thus increases!

Thanks a lot for the help everyone!
 
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  • #25
as stated the voltage divider rule looks like it came out of thin air. The point is the resistors are in series. They must carry the same current. The current across both together is

I = V / (R1+R2)

So that is also the current through each individually

V1 = I R1 = V R1 / (R1 + R2)

And there is your voltage divider rule.
 
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  • #26
Thanks a lot everyone!

I feel that it is safe to say that this thread is over!

Greatly appreciated!
 

What is a capacitor and how does it work?

A capacitor is a passive electronic component that stores electrical energy in an electric field. It consists of two conductive plates separated by an insulating material called a dielectric. When a voltage is applied across the plates, the capacitor stores energy in the form of an electric charge. This charge can be released when needed, making capacitors useful for a variety of applications such as filters, energy storage, and timing circuits.

What is the difference between a series and parallel capacitor circuit?

In a series capacitor circuit, the capacitors are connected end-to-end, with one plate of each capacitor connected to the other. In a parallel capacitor circuit, the capacitors are connected side-by-side, with all the positive plates connected together and all the negative plates connected together. The main difference between the two is the way in which the capacitors are connected to each other and how the total capacitance is calculated.

How do I calculate the total capacitance of a circuit with multiple capacitors?

In a series circuit, the total capacitance is calculated by adding the reciprocals of the individual capacitances. So, if you have three capacitors with capacitances C1, C2, and C3, the total capacitance (Ctotal) is equal to 1/(1/C1 + 1/C2 + 1/C3). In a parallel circuit, the total capacitance is simply the sum of the individual capacitances.

What happens if I connect a capacitor in reverse polarity?

If you connect a capacitor in reverse polarity, meaning the positive terminal is connected to the negative terminal and vice versa, it can lead to damage or failure of the capacitor. This is because the capacitor is designed to store energy in a specific direction, and reversing the polarity can cause the dielectric material to break down and the capacitor to short circuit.

What are some common applications of capacitors in circuits?

Capacitors have a wide variety of applications in electronic circuits. Some common uses include filtering noise from power supplies, smoothing voltage waveforms, tuning radio frequencies, and storing energy in flash cameras and defibrillators. They are also used in timing circuits, motor run circuits, and as sensors in touchscreens and accelerometers.

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