What is the Potential Difference Between c and d in This Circuit?

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gracy
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Homework Statement


If 100 volts of potential difference is applied between a and b in the circuit .Find the potential difference between c and d.
Circuit schematic with terminals a and b on the left and nodes c and d on the right, containing four 6 micro F capacitors: one top horizontal, one vertical in the middle-left, one vertical on the right, and one bottom horizontal.

2. Homework Equations

For Equivalent Capacitance in series

##\frac{1}{C}##=##\frac{1}{C_1}##+##\frac{1}{C_2}##For Equivalent Capacitance in parallel

##C##=##C_1##+##C_2##...

##Q##=##C####v##

The Attempt at a Solution

Circuit schematic with a battery labelled V between terminals a and b, a 6 micro F capacitor C2 in a vertical branch, and a rectangular loop with capacitors C1, C4 and C3, each 6 micro F, with corners labelled c and d.


Two circuit schematics: left shows battery V between a and b with a 6 micro F capacitor C2 in parallel and a 2 micro F capacitor between c and d; right shows battery V between a and b with an 8 micro F capacitor C4 between c and d.
[/B]
Equivalent capacitance between c and d (using series connection formula)
C1,C3 and C4 are in series
Ceq=2μF

this C eq and c2 are in parallel hence (using parallel connection formula)
Ceq'=8μc
This C'eq is in parallel with voltage hence it should have potential difference equal to 100 volts but it is wrong .I want to know why?
 
When you combined all the capacitors into one you "lost" the nodes c and d in the process. You simplified the circuit sown to a single capacitor that is situated between node a and b. In fact you lost c and d in your first simplification when you combined the three series capacitors into a single 2 uF capacitor. You mistakenly placed c and d node labels around it, but nodes c and d no longer exist in the simplified circuit. What you found is the potential across a and b, which you already knew since it's a given.

What you should do is first consider (as a slight but essential digression) a voltage divider that consists of capacitors in series. If you place a potential across a series-connect string of capacitors, how can you determine the potentials across the individual capacitors in the string?
 
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gneill said:
When you combined all the capacitors into one you "lost" the nodes c and d in the process.
gneill said:
You mistakenly placed c and d node labels around it
No,I deliberately place c and d .
gneill said:
but nodes c and d no longer exist in the simplified circuit.
You mean nodes c and d should not exist in the simplified circuit?
But why ?As I have clarified this earlier https://www.physicsforums.com/threads/equivalent-capacitance.845489/page-2
post #22 and #23
that we can place equivalent capacitors wherever I want and should replace other component capacitor with wire,I did that.
 
gracy said:
No,I deliberately place c and d .

You mean nodes c and d should not exist in the simplified circuit?
But why ?As I have clarified this earlier https://www.physicsforums.com/threads/equivalent-capacitance.845489/page-2
post #22 and #23
that we can place equivalent capacitors wherever I want and should replace other component capacitor with wire,I did that.
A 'series' combination of 3 capacitors is connected across 100V supply. You don't need equivalent capacitance for calculating the voltage across the middle capacitor (Vcd).
 
gracy said:

Homework Statement


If 100 volts of potential difference is applied between a and b in the circuit .Find the potential difference between c and d.
Circuit schematic of four 6 micro F capacitors: one between terminal a and point c on the top branch, one vertical between a and b on the left, one between c and d on the right, and one between b and d on the bottom, with terminals a and b at the left and points c and d at the right corners.

2. Homework Equations

For Equivalent Capacitance in series

##\frac{1}{C}##=##\frac{1}{C_1}##+##\frac{1}{C_2}##For Equivalent Capacitance in parallel

##C##=##C_1##+##C_2##...

##Q##=##C####v##

The Attempt at a Solution

Circuit schematic with a battery labelled V between nodes a and b, and four 6 micro F capacitors labelled C1, C2, C3 and C4 connected in a rectangular loop with corners a, c, d and b.


View attachment 92911 [/B]
Equivalent capacitance between c and d (using series connection formula)
C1,C3 and C4 are in series
Ceq=2μF

this C eq and c2 are in parallel hence (using parallel connection formula)
Ceq'=8μc
This C'eq is in parallel with voltage hence it should have potential difference equal to 100 volts but it is wrong .I want to know why?
C1 and C3 are not in between c and d. Also, if you want to calculate equivalent capacitance between C and D, your source should be between c and d. What you've calculated is the equivalent capacitance between a and b.
 
cnh1995 said:
your source should be between c and d.
you mean voltage source?
 
gracy said:
No,I deliberately place c and d .
You created new labels c and d where they were not previously located. In the original circuit c and d surrounded the middle capacitor in the string of three. You collapsed the string and moved the labels c and d to the outside ends of the string where it connects to the rest of the circuit. In fact your new labels c and d are identical to the nodes identified by a and b.
You mean nodes c and d should not exist in the simplified circuit?
Right. They were abolished when you reduced the three capacitors. Effectively you cut off the branch containing the three capacitors and nodes c and d and replaced it with a single new capacitor. You lost c and d when you did that.

Left: a circuit with a battery V between nodes a and b, a capacitor C2 in parallel, and a blue-outlined new capacitor Cnew across the same nodes. Right: a rectangular loop with capacitors C1, C3 and C4, each 6 micro F, with nodes c and d marked and a red arrow labeled Thrown away.

But why ?As I have clarified this earlier https://www.physicsforums.com/threads/equivalent-capacitance.845489/page-2
post #22 and #23
that we can place equivalent capacitors wherever I want and should replace other component capacitor with wire,I did that.
When you simplify component networks you lose analytical access to nodes that get absorbed into the replacement components. Sometimes you just have to leave some components unsimplified to retain access to nodes you need.
 
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gneill said:
Sometimes you just have to leave some components unsimplified to retain access to nodes you need.
Here we need c and d so should I not simplify the series connection between C1,C3 and C4 ?
 
gracy said:
Here we need c and d so should I not simplify the series connection between C1,C3 and C4 ?
Yes. You needn't consider C2 too..
 
gracy said:
Here we need c and d so should I not simplify the series connection between C1,C3 and C4 ?
Correct.
 
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gneill said:
Effectively you cut off the branch containing the three capacitors and nodes c and d and replaced it with a single new capacitor.
Circuit schematic: a battery V between nodes a and b with capacitor C2 in parallel, plus a blue-outlined new capacitor Cnew connected to the same nodes. Right: hand-drawn loop with C1 6 micro F, C3 6 micro F, C4 6 micro F and nodes c and d, with a red arrow labelled Thrown away.
\
is blue node new node?It wasn't there previously?
 
The item in blue is new, yes, but there's no new node. The new capacitor connects to where the old string of three capacitors connected, and those two nodes existed before. In fact they are nodes a and b: just follow the wires to the labels near the battery.
 
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https://www.physicsforums.com/threads/equivalent-capacitance.845489/
in post #9
gneill said:
Remember, when you collapse a series of components down to one then you will be eliminating any nodes that were along the path, leaving just the two nodes at the ends where the "new" component attach.
Circuit schematic with a battery labelled V between nodes a and b, a 6 micro F capacitor C2 in the middle branch, and C1, C3 and C4 each 6 micro F; red wire highlights the path from C1 through c and d to C4, with labels for remaining nodes at each end.


Left: circuit with battery V between nodes a and b, capacitor C2 across the terminals, and a blue-highlighted equivalent capacitor Cnew drawn beside it. Right: a loop of capacitors labelled C1, C3 and C4, each 6 micro F, with nodes c and d and a red curved arrow labelled Thrown away.


Red nodes-eliminated nodes
Blue nodes-new introduced wires with equivalent capacitor
Black nodes-nodes which are left at the points of attachment of the new (equivalent )capacitor at both ends
 
Attachments
  • Circuit schematic with a battery between nodes a and b, a 6 micro F capacitor C2 in parallel with the battery, and a path from a through C1 (6 micro F) to node c, C4 (6 micro F) from c to d, and C3 (6 micro F) from d back to b; the c-to-d branch is highlighted in red.
    eliminated.png
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I understood where I was wrong.All thanks to you guys.How shall I proceed from here?
 
gracy said:
How shall I proceed from here.

gneill said:
What you should do is first consider (as a slight but essential digression) a voltage divider that consists of capacitors in series. If you place a potential across a series-connect string of capacitors, how can you determine the potentials across the individual capacitors in the string?
:smile:
 
gracy said:
I understood where I was wrong.All thanks to you guys.How shall I proceed from here.
Just use voltage divider for the series combination in the original diagram.
 
cnh1995 said:
Also, if you want to calculate equivalent capacitance between C and D, your source should be between c and d.
I did not understand this.Can not we calculate equivalent capacitance between two points if there is no battery between them?
Then how we did it here?There was no battery/voltage source in between A and B but we calculated equivalent capacitance between A and B.https://www.physicsforums.com/threads/equivalent-capacitance-circular-arrangement.845579/

Circular ring of capacitors with labelled points A and B, values 3 µF, 4 µF, 5 µF and 2 µF, beside an equivalent circuit with 2 µF in parallel with 3 µF, 4 µF and 5 µF in series between A and B.
 
gracy said:
I did not understand this.Can not we calculate equivalent capacitance between two points if there is no battery between them?
Then how we did it here?There was no battery/voltage source in between A and B but we calculated equivalent capacitance between A and B.https://www.physicsforums.com/threads/equivalent-capacitance-circular-arrangement.845579/

Left: a circle of wire with capacitors labelled 3 micro F, 2 micro F, 4 micro F and 5 micro F, with terminals A and B on the right. Double arrow to right: A connects to a 2 µF capacitor in parallel with a series branch of 3 µF, 4 µF and 5 µF capacitors, ending at B.
The equivalent capacitance between two points will be "seen" by a source placed between those points. That's the fundamental meaning of 'equivalent capacitance'. Here, if you place a source between A and B, it will "see" the capacitance of the network to be equal to the calculated equivalent capacitance between A and B, only for which the diagram has been modified. What you had calculated earlier was the capacitance "seen" by the voltage source between A and B which wouldn't be same as seen by a voltage source between C and D.
 
The presence of batteries or voltage sources does not change the effective capacitance of the circuit between nodes A and B. It depends only on the capacitors in the circuit and how they are interconnected.
 
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gracy said:
But according to this applying voltage source matters
But in that problem, it was mentioned that there is a p.d. of 100V connected between a and b. Voltage between c and d was to be found out. So, there's no point in 'putting' a source between c and d.
 
gracy said:
But according to this applying voltage source matters
https://www.physicsforums.com/threads/equivalent-capacitance-circular-arrangement.845579/page-3
#post 51
It matters in that it would change the problem to a different problem. You can't determine the potential between c and d due to the 100 V at a and b if you place yet another source somewhere in the circuit. In fact, placing a source across c and d would force that potential to be whatever that new source supplies, and would be completely independent of the a-b source.
 
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gneill said:
it implies that you need a voltage source in order to determine the equivalent capacitance.
But I have seen some problems in which I was asked to determine equivalent capacitance between two points and there was no voltage source.
 
Last edited:
A source won't change the capacitance between nodes?
Then what voltage source does?
 
gracy said:
But I have seen some problems in which I was asked to determine equivalent potential between two points and there was no voltage source.
Then the potential difference must have been zero. Unless the voltage source was already charged capacitors and there were no paths for discharging them. Capacitors retain their charge if there are no closed paths for them to discharge through.

Perhaps you should post one of these problems as a new thread.
 
gracy said:
A source won't change the capacitance between nodes?
Then what voltage source does?
It provides a potential difference. In circuits where current can flow it provides the potential that drives current.
 
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