Confusion:collapsing 3 points with equal potential in a cubical resistor network

Click For Summary

Homework Help Overview

The discussion revolves around finding the equivalent resistance between opposite ends of a cubical resistor network, where each resistor has a resistance R. Participants are exploring the concept of collapsing points of equal potential within the circuit to simplify the analysis.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants discuss the application of Kirchhoff's laws and the implications of collapsing points of equal potential. There are attempts to visualize how certain points can be combined without altering the circuit's behavior.

Discussion Status

Some participants have provided insights into the methodology of collapsing points and the implications of symmetry in the circuit. Others are seeking further clarification on how to apply these concepts effectively, particularly in different configurations.

Contextual Notes

There is an ongoing exploration of the assumptions regarding points of equal potential and their impact on circuit analysis. Participants are also considering the effects of different voltage supply connections on the potential equivalence of points within the network.

nishantve1
Messages
74
Reaction score
1

Homework Statement



The question is to find Equivalent resistance between opposite ends of a cubical resistor network . each resistor of resistance R .

I am referring to this website here
http://mathforum.org/library/drmath/view/65234.html
I am halfway through it but I am stuck at a point . Where it says
"Now imagine shrinking these wire loops down to a single point. This
collapses together the points BDE and CFH. The circuit now looks like
this (when flattened out):"

/-R-\
--R-- /--R--\ -R-
/ \ /---R---\ / \
o---A---R--(BCD)----R--(CFH)--R--G---o
\ / \---R---/ \ /
--R-- \--R--/ -R-


Homework Equations



Only equation I believe is used will be V= IR and Kirchoff's law maybe I think it will use only the formulas for connection of resistors in parallel and series

The Attempt at a Solution



I have tried using Kirchoff's law that is enetring a current I from A then distributing it , it gives the right answer but its quiet very lengthy . Just stuck there . if some one can help it would be awesome
Thanks
 
Physics news on Phys.org
http://img69.imageshack.us/img69/2443/p1010017gh.jpg
 
Last edited by a moderator:
If points in an electric circuit are connected with wires (of zero resistance) these wires can be replaced by a single node. Points of equal potential always can be connected, it does not alter anything in the circuit.

ehild
 

Attachments

  • equivalence.JPG
    equivalence.JPG
    8.9 KB · Views: 427
vsupply=Itotal . Rtotal (1)

vsupply=I1/3 . R1/3 (2)
vsupply=I(1/3R + 1/6R + 1/3R) . (G->H ->D->A)
vsupply=I(5/6)R

Subt. in (1)
I(5/6R)=Itotal . Rtotal
Rtotal=5/6R
 
Sorry but I am still not getting how to collapse the three points together . Sorry for bring dumb but please help me out.
 
Say current I enters point G.
Then equally it is distributed to 3 branches.
Makes each branch current 1/3I(pt G)
Next points, incoming 1/3I, branchout to 2 branches which means each outlet=(1/3)/2I=1/6I.(pt H)
finally 2 branches join and equal I(1/6+1/6)=I(1/3).(pt. E)
All above from Kirchoff's Current Law(KCL)

Next Kirchoff's Voltage Law(KVL)

If you follow any route(from G to A,from higher potential to lower potential), the total voltage equal to supply voltage.
 
Last edited:
ehild said:
If points in an electric circuit are connected with wires (of zero resistance) these wires can be replaced by a single node. Points of equal potential always can be connected, it does not alter anything in the circuit.

ehild

azizlwl said:
Say current I enters point G.
Then equally it is distributed to 3 branches.
Makes each branch current 1/3I(pt G)
Next points, incoming 1/3I, branchout to 2 branches which means each outlet=(1/3)/2I=1/6I.(pt H)
finally 2 branches join and equal I(1/6+1/6)=I(1/3).(pt. E)
All above from Kirchoff's Current Law(KCL)

Next Kirchoff's Voltage Law(KVL)

If you follow any route(from G to A,from higher potential to lower potential), the total voltage equal to supply voltage.

I know how to do it by applying Kirchoff's law but I am looking forward to solve it by the method of connecting points of equal potentials . I understand that the points with equal potentials can be connected without affecting the circuit but I just wanted a more clear image of how this has been done . I mean how did they connect the three points , did they make all the point one single point ? :rolleyes:
 
See the figure in #3. They make it a single point at the end.

ehild
 
@echild Thanks but can you please show me the picture of how the three points are made one in the cubical network . Thanks
 
  • #10
Also in the same cubical network If I were to finto resistance between points B and D , why will the current bit flow through the branches CG AND AE
 
  • #11
You can distort the square, nothing happens when you do not change the connection between the nodes. Just press the dots representing the corners B,D,E together. The wires which were the edges, will bend but their resistance does not change.

ehild
 

Attachments

  • squize.JPG
    squize.JPG
    8.9 KB · Views: 474
  • #12
ehild said:
You can distort the square, nothing happens when you do not change the connection between the nodes. Just press the dots representing the corners B,D,E together. The wires which were the edges, will bend but their resistance does not change.

ehild

alright now I know how they can be connected thank you sooo much ! but how are the remaining 6 resistors in parallel ?
Also can I solve for equivalent resistance between any other two points using the same approach?
 
  • #13


1st Point - G
2nd Point all resistor with voltage drop of RI(1/3) =3 resistor in parallel
3rd Point alll resistor with voltage drop of RI(1/6+1/3) = 6 resistors in parallel
4th point all resistor with voltage drop of RI(1/6+1/3+1/3) =3 resistor in parallel
Point A

1st total resistance. =R(1/3)
2nd. total resistance. =R(1/6)
3rd. total resistance. =R(1/3)

Rt=R(5/6)
 
  • #14


azizlwl said:
1st Point - G
2nd Point all resistor with voltage drop of RI(1/3) =3 resistor in parallel
3rd Point alll resistor with voltage drop of RI(1/6+1/3) = 6 resistors in parallel
4th point all resistor with voltage drop of RI(1/6+1/3+1/3) =3 resistor in parallel
Point A

1st total resistance. =R(1/3)
2nd. total resistance. =R(1/6)
3rd. total resistance. =R(1/3)

Rt=R(5/6)

Ok alright :biggrin: Thanks . One thing that's confusing me is , as in this cube the cell was connected between A and G and then the 3 points with the same potential are easily identified . But in case we connect the cell between points A and C then why not B D and E are at the same potential ?
A------B
/| /|
D-----C |
| E---|-F
|/ |/
H-----G
 
  • #15
Check the symmetry, with the cell included. Now the configuration has got a vertical mirror planedefined by A and C. B and D are equivalent points with respect to it, but E is not. In the first configuration, it was a threefold axis between A and G.
 
  • #16
Thanks for the reply guys , I have no idea about symmetry and how to find points with equal potentials . I am cracking my head since hours , please if you will solve my dilemma I will be very very grateful to you , Please help me
Please answer this post
https://www.physicsforums.com/showthread.php?p=3938977#post3938977
Thank you so much for all the help !
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 28 ·
Replies
28
Views
9K
Replies
25
Views
4K
  • · Replies 8 ·
Replies
8
Views
7K
  • · Replies 9 ·
Replies
9
Views
7K
  • · Replies 15 ·
Replies
15
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
9
Views
2K