Discharging a charged capacitor to another neutral capacitor

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SUMMARY

The discussion revolves around the discharge of a charged capacitor (C1 = 5μF, V0 = 6.50V) into another neutral capacitor (C2 = 5.3μF) when connected in series. The key equations used are q = CV and the relationship between the voltages across the capacitors, V1 = V2, leading to the conclusion that charge is conserved while voltage is not. The correct approach involves recognizing that the total charge initially on C1 is distributed between C1 and C2, resulting in the equations q1/C1 = q2/C2 and q1 + q2 = q0, where q0 is the initial charge on C1. Misunderstandings about voltage conservation in capacitor circuits are clarified through the discussion.

PREREQUISITES
  • Understanding of capacitor charging and discharging principles
  • Familiarity with series and parallel capacitor configurations
  • Knowledge of the relationship between charge, voltage, and capacitance (q = CV)
  • Basic circuit analysis skills, including Kirchhoff's voltage law
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  • Study the principles of capacitor networks and their configurations
  • Learn about energy conservation in capacitor circuits
  • Explore the effects of resistance on capacitor discharge rates
  • Investigate the implications of connecting capacitors in series versus parallel
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Hijaz Aslam
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Homework Statement


After a capacitor of capacitance ##C_1## is charged up to a voltage ##V_o##, the Battery is removed from the circuit. Another capacitor of capacitance ##C_2## is connected in series with the capaciotr ##C_1##. Find the charge on each capacitor after equilibrium is attained. (##C_1=5microF##, ##C_2=5.3microF##, ##V_o=6.50V##).

Homework Equations


##q=CV##

The Attempt at a Solution


I tried cracking the problem as follows:

Initially ##C_1## has a voltage of ##V_o##. After connecting ##C_2## voltages of both the capacitors will become equal. So we have ##V_1=V_2## . Now as the initial potential was ##V_o##, and as the capacitors are connected in series ##V_1+V_2=V_o##. Therefore ##V_1=V_2=V_o/2##. Hence ##q_1=C_1V/2## and ##q_2=C_2V/2##. But after substituting the values, the final figure seems wrong!

My textbook attempts this question by taking: ##V_1=V_2## and assuming that ##C_1## initially had charge ##q_o##. Therefore as ##V_1=V_2## we have ##q_1/C_1=q_2/C_2## and taking ##q_1+q_2=q_o## and simplifying they arrive at the answer.
Textbook method seems fine. But what is wrong with my method? Am I missing any concepts? (I think I am likely to be wrong at ##V_1+V_2=V_o##).
 
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Why do you think the sum of voltages stays the same?
The charge stays the same, the voltage does not have to.
 
Well my text mentions that in case of a Battery the voltage is maintained, whereas in case of Capacitors as it lacks the electro-chemical reaction (as in case of a cell) the voltage is not conserved. Why is the charge conserved but not the voltage. Can I have an explanation?
 
Why would voltage be conserved?
 
Dear Hijaz,
If you make a little drawing you will see that, as you already expected, ##V_1+V_2=V_o## can not be correct.
Fortunately, you have enough equations left over to determine q1 and q1
 
I thought about it and arrived at the following explanation : The moment ##C_2## is connected to the circuit, nature urges the voltage of both the capacitors to be the same. At the same time ##C_1## pushes charges into ##C_2## to attain the state represented by ##q_1/C_1=q_2/C_2##. And at some point when the required charge ##q_2## is consumed by ##C_2##, ##C_1## in the hurry to attain equilibrium sheds any left over voltage somehow (or any similar method).
Am I right? Or is my explanation coincidental and a blunder?

But still we can argue: why can't ##q_1/C_1=q_2/C_2## be still attained at the same time following the condition ##V_1+V_2=q_1/C_1+q_2/C_2=V_o##.
And I think I've found a possible explanation for that too. Isn't it because the charge supplied by ##C_1## is limited to ##q_o## (which ##C_1## attained during it's initial charging by the cell)?
 
Thinking is good. Making a little drawing is better. If you follow V1 plus V2, then you are back at the same point (*). But you traversed C2 in the opposite direction, meaning you have V1 - V2 = 0, in other words V1 = V2 -- which you already had (and correctly so).

"The moment C2 is connected to the circuit, nature urges the voltage of both the capacitors to be the same" yes ( but again: *)
"C1 pushes charge into C 2 to attain the state represented by q1 /C1 =q2 /C2" yes ( but again: *)

There is no "hurry", but it goes fast, yes. Lightning speed, so to say (there is no mention of resistance to limit the rate of discharge).
"Shedding of voltage" is the same thing as unloading charge: q = CV. Driving force is voltage difference. Unloading stops when voltage difference is zero, well before q0 is supplied.

- - - - - - -
(*)
I suddenly realize there may be a misunderstanding: how exactly do you interpret
Another capacitor of capacitance C2 is connected in series with the capacitor C1
-- again a good reason for a drawing!
 

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