# Charging capacitors in series with another capacitor

• LeoWongFromHK
In summary: Hence, statement (3) is wrong, as a combination of any values may lead to ΔE≠ 0." is not quite correct. The last sentence should read "Hence, statement (3) is wrong, as a combination of any values may not lead to ΔE≠ 0."
LeoWongFromHK
This question was taken from the public examination in my country/region.
The answer from the marking scheme is, only statement 1 is correct and the others are wrong. Can anyone explain why the other statements are wrong?
1. Homework Statement

The following components are connected in series in a circuit in the following order:
a charged capacitor C, two uncharged capacitors C1 and C2, an open switch S.
( I couldn't draw it on the computer...)
It is given that C1 > C2 and the resistances of the connecting wires are negligible. Which of the following is/are correct after closing the switch S?
Statement 1: p.d across C1 < p.d. across C2
Statement 2: The sum of magnitudes of charges on all three capacitors = the original charge (before closing switch) on C
Statement 3: Total energy stored in three capacitors = energy stored in C before closing switch

## Homework Equations

Energy stored in capacitor= ½CΔV2 = ½QΔV = ½Q2/C
Definition of capacitance: C=Q/ΔV

## The Attempt at a Solution

(1) was proven to be true with definition of capacitance. Tried to state out heat is released for (3) but it is not true due to R(wire)=0Ω → P=0W as P=I2R.

Hello LWfromHK, welcome to PF !

From your wording, I take it you acccept that (1) is a correct answer and are in doubt about (3).

In case you want to check the answers, do you know how much energy is stored in a capacitor that is charged with a charge Q ?
If so, you should be able to calculate the energy stored after the new equalibrium is established with the energy stored before.

(2) isn't so much a calculation as a matter of understanding. Where can the inital charge on C go and what are the consequences ?

LeoWongFromHK
BvU said:
Hello LWfromHK, welcome to PF !

From your wording, I take it you acccept that (1) is a correct answer and are in doubt about (3).

In case you want to check the answers, do you know how much energy is stored in a capacitor that is charged with a charge Q ?
If so, you should be able to calculate the energy stored after the new equalibrium is established with the energy stored before.

(2) isn't so much a calculation as a matter of understanding. Where can the inital charge on C go and what are the consequences ?
Thanks for your reply! It helped a lot in both my thinking, not just only on this question.
For (2), the initial charges go into the capacitors C1 and C2, by charge sharing. The charge at C1 is equal to that at C2. For the initial charge on C transferred to C2, the same amount will be transferred on C1. Let this charge transferred to be q. Then the charge loss at C is q, charge gain at C1 is q, and that at C2 is also q. Plates that are connected by the wire from C1 to C2 will be charged by the same amount but opposite in sign, through electrostatic induction. Hence, there is a net charge gain of -q (at C) +q (at C1) +q (at C2) = +q ≠ 0 for the system
∴ (2) is incorrect

For (3), I think I would do the calculation using the result from (2),
Knowing that initial energy stored in C = Ei = ½Q2/C for initial charge Q and p.d. ΔV
Final total energy stored in all three capacitors = ½ [(Q-q)2/C + q2/C1 + q2/C2
]
= ½ {(Q2 -2Qq+q2)/C+q2/C1+q2/C2}
=Ei + q2/2Ceq - Qq/C, where Ceq is the equivalent capacitance of all three capacitors.
Take net change in energy stored in the capacitors (ΔE) = q2/2Ceq - Qq/C
Then, final total energy stored in all three capacitors = Ei + ΔE
Since q, Q, C, C1, C2 are arbitrary values, it is uncertain whether a net change in energy stored in the capacitors (ΔE) is registered. Hence, statement (3) is wrong, as a combination of any values may lead to ΔE≠ 0. We cannot consider it correct if there exists a case which ΔE≠0.
Did I get it correctly? Please notify me if I didn't. Thanks!

For (2), the initial charges go into the capacitors C1 and C2, by charge sharing. The charge at C1 is equal to that at C2. For the initial charge on C transferred to C2, the same amount will be transferred on C1. Let this charge transferred to be q. Then the charge loss at C is q, charge gain at C1 is q, and that at C2 is also q. Plates that are connected by the wire from C1 to C2 will be charged by the same amount but opposite in sign, through electrostatic induction. Hence, there is a net charge gain of -q (at C) +q (at C1) +q (at C2) = +q ≠ 0 for the system
∴ (2) is incorrect
Almost. The last line is correct, but not for the reason you state in the preceding line .

Once the switch is closed, you have three capacitors in series. Whatever charge there is, it can't get out of the circuit!
If a charge q is transferred from C to C1, then a charge -q is transferred from the bottom plate of C to the bottom plate of C2. So the net charge gain is zero. That reason (2) is incorrect nevertheless is because the sentence "sum of magnitudes of charges on all three capacitors" nastily wants you to add |Q-q| on C, |q| on C1 and |q| on C2.

If this is established, we can move on to (3) comfortably, using your equation. You are well underway, but there is more to be said here. If you want a simple case: take C as in this problem and replace C1 and C2 by one uncharged capacitor with capacity C as well. What can you say about the energies before and after in that case ?

Again (3) is indeed wrong, but I suspect it is always wrong.

(Afterwards, there will be the complicating question: where did the energy go ?! intriguing, but fortunately not within the scope of this exercise. More later...)

--

LeoWongFromHK
BvU said:
Almost. The last line is correct, but not for the reason you state in the preceding line .

Once the switch is closed, you have three capacitors in series. Whatever charge there is, it can't get out of the circuit!
If a charge q is transferred from C to C1, then a charge -q is transferred from the bottom plate of C to the bottom plate of C2. So the net charge gain is zero. That reason (2) is incorrect nevertheless is because the sentence "sum of magnitudes of charges on all three capacitors" nastily wants you to add |Q-q| on C, |q| on C1 and |q| on C2.

If this is established, we can move on to (3) comfortably, using your equation. You are well underway, but there is more to be said here. If you want a simple case: take C as in this problem and replace C1 and C2 by one uncharged capacitor with capacity C as well. What can you say about the energies before and after in that case ?

Again (3) is indeed wrong, but I suspect it is always wrong.

(Afterwards, there will be the complicating question: where did the energy go ?! intriguing, but fortunately not within the scope of this exercise. More later...)

--
I see, the magnitudes of charges cannot be added through summation.

The charge on both capacitors will be equal, that is, half of the original of the charge carried by C. and thus the energy stored in each capacitor will be (½)2=¼ times the original C. Hence, the total energy will be 2×¼=½ times the original.

I suggest the energy difference is the work done to push the charges from one capacitor to another. Otherwise, no charges can be accumulated at the other uncharged capacitor.

LeoWongFromHK said:
I see, the magnitudes of charges cannot be added through summation.

The charge on both capacitors will be equal, that is, half of the original of the charge carried by C. and thus the energy stored in each capacitor will be (½)2=¼ times the original C. Hence, the total energy will be 2×¼=½ times the original.

I suggest the energy difference is the work done to push the charges from one capacitor to another. Otherwise, no charges can be accumulated at the other uncharged capacitor.
Good work. So (2) is done with, right ?

For (3), you have shown that for two equal capacities the energy is reduced to one half the original energy. You could work it out further with unequal capacities (good exercise in dealing with inequalities!)

To explain it is probably beyond the scope of the exercise: in the case of ideal capacitors, ideal zero resistance connections etc., the current when the switch closes would jump to infinity, which is rather impossible. And once this big current is flowing, it wants to keep going (by self-inductance): the discharge goes on beyond equilibrium and the current reverses. An oscillating circuit that radiates off electromagnetic waves that carry away energy. All very far fetched: a really small resistance already limits the current and dissipates electric energy into heat (or a flash of light, for example).

--​

LeoWongFromHK

## What is the purpose of charging capacitors in series with another capacitor?

The purpose of charging capacitors in series with another capacitor is to increase the overall capacitance of the circuit. By connecting capacitors in series, the total capacitance is equal to the reciprocal of the sum of the reciprocals of each individual capacitor's capacitance.

## How does charging capacitors in series affect the voltage across each capacitor?

When capacitors are connected in series, the total voltage across the circuit is divided among the individual capacitors. This means that the voltage across each capacitor will be less than the total voltage applied to the circuit.

## What is the formula for calculating the total capacitance of capacitors in series?

The formula for calculating the total capacitance of capacitors in series is: 1/Ctotal = 1/C1 + 1/C2 + 1/C3 + ... + 1/Cn, where Ctotal is the total capacitance and C1, C2, C3, etc. are the individual capacitances of each capacitor in the series.

## What happens to the energy stored in capacitors when they are connected in series?

When capacitors are connected in series, the total energy stored in the circuit remains the same. However, the energy is divided among the individual capacitors, with each one storing a smaller amount of energy compared to when they are used individually.

## What are some practical applications of charging capacitors in series with another capacitor?

Charging capacitors in series with another capacitor is commonly used in electronic circuits to increase the overall capacitance and store more energy. This can be useful in applications such as power supplies, filters, and timing circuits.

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