Calculating resistance of wired cubes

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In summary, a student is seeking help with a difficult physics problem posted in their country's math-physics magazine. The problem involves calculating resistance in a circuit and the student has attempted to solve it but has not been successful. Another student provides a solution by simplifying the circuit and solving for the resistance between two points. The student is grateful for the help and continues to practice with tricky problems for the International Physics Olympiad.
  • #1
Tusike
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Homework Statement


This problem was posted in february in my country's math-physics magazine for high school students, as part of the competition. I couldn't do it then, and every now and again I try it, but still I can't do it, so any help on where to start would be very much appreciated.

http://www.komal.hu/verseny/feladat.cgi?a=honap&h=201002&t=fiz&l=en"

Scroll down and see problem P. 4231. Unfortunately for me, this site has excellent math, physics, and informatics problems, but they usually only provide the solution for the math and informatics ones.

Homework Equations


Not much. R = U/I may help and Kirchoff's equations.


The Attempt at a Solution



As I said, I didn't really get anywhere. I tried to draw down the whole thing as a circuit in 2D, but what I got wasn't pretty, with overlapping wires and all. Normally in problems like these, the idea I saw was that you write down the resistance after n number of cubes have been attached to either side, then the same for n+1, and you say as n nears infinity, they are equal. Normally that equation gives a value for the whole resistance. But I just couldn't write down those equations.

Thanks for any help!
-Tusike
 
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  • #2
A very tricky one :uhh:
You can easily see that each couple of symmetric points (e.g. C and D, E and F, G and H) have the same electric potential (see figure (1)). That means you can join the points in each couple together and get a 2-D circuit like in figure (2). Again, because of symmetry, potential at C-D = potential at E-F, there is no current running through the wire joining them, so you can omit it. Therefore, the problem becomes solving for the resistance of AP (the 2r resistor is excluded). As the circuit is periodic and infinite, we can consider RAP as in figure (3). From here, you can solve for RAP and then RAB.
 

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  • #3
Okay, I see how you got figure (2), I even did that back then, but I didn't know how to continue. First of all: after getting figure (2), the red wires on your image would have the resistance of R (where R is the one in the original problem), and the black ones would have a resistance of R/2, right? Since we got them by combining two parallel R's.
I'm not sure I understand how you got figure (3) from (2). because if you fold figure (2) on that AP line, which you can because of the symmetry in potentials, AP would be connected with that red wire, still a resistance of R, and the mentioned R(AP). So I would understand figure (3) if there was a red line connecting A and P:) In figure (3), this line would have a resistance of R, the red lines R/2, and the black ones R/4 right?
And after getting R(AP), how does R(AB) come from that?

Sorry for not understanding this right away, and thanks for the help so far!

-Tusike
 
  • #4
Sorry for the confusion. I forgot to say r=R/2, it's just to make it look a bit better :biggrin: When I mentioned R(AP), I excluded the red wire (the 2r one) in order to make it cleaner, so we got something like in figure (3). You can include the red wire, but it doesn't matter. In figure (3), the red lines are R (or 2r), the black lines are R/2 (or r).
And after solving for R(AP), you just have to redraw the circuit in some convenient way. It is no longer a complicated circuit, but just a simple one which contains series and parallel resistors, as we have removed the line joining C-D and E-F.
 
  • #5
wires.JPG


I'm not sure you understood what I meant. Here is what I get from figure (2). B' and Q' are equipotential to B and Q, as shown by the purple curves. And the whole (3) is the infinite wire you get after connecting these equipotential points.

EDIT: OK, I see what you meant:) It's things like these that make me wonder why I'm trying for the IPhO. By R(AP) I thought you meant the whole resistance between those two points. Of course, if you just look at the whole part to the left of points A and P, you get what you're figure (3) had, and the same on the other side's B and Q. Everything's perfectly clear now, thank you very much!

-Tusike
 
  • #6
Oh sorry for the confusion again :uhh:
I'll make it a bit clearer. You'll see that I have split (AP) into 2 parallel parts: one is the red wire, the other is (A'P') which corresponds to figure (3). The blue wires are just connecting wires, zero resistance.

EDIT: I see you got it. Btw, I think if it's crucial to practice with these kinds of tricky problems to get into the IPhO team, then go for it. But if you don't have to, then you shouldn't dig into these things too much. Sometimes there is not much physics in these problems.
 

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  • #7
Well every now and again tricky problems like these are fun:) plus it really did bug me a lot.
Thanks again for the help!
 

1. How do I calculate the resistance of a wired cube?

To calculate the resistance of a wired cube, you will need to use the formula R = ρ * (L/A), where R is resistance, ρ is the resistivity of the material, L is the length of the wire, and A is the cross-sectional area of the wire. For a cube, the length and cross-sectional area will be the same for each side of the cube. Therefore, you can find the total resistance by multiplying the resistance of one side by 6.

2. What is the resistivity of the material used in a wired cube?

The resistivity of a material is a measure of how strongly it resists the flow of electric current. It is typically denoted by the symbol ρ and is measured in ohm-meters (Ω*m). The resistivity of the material used in a wired cube will depend on the specific material used. Common materials used for wires include copper, aluminum, and silver, which have resistivities of 1.68 x 10^-8 Ω*m, 2.82 x 10^-8 Ω*m, and 1.59 x 10^-8 Ω*m, respectively.

3. What is the cross-sectional area of a wired cube?

The cross-sectional area of a wired cube is the area of a square that makes up one of its sides. It is typically measured in square meters (m^2). To find the cross-sectional area of a cube, you can square the length of one side. For example, if the cube has sides that are each 0.1 meters long, the cross-sectional area would be 0.01 m^2.

4. How does the length of the wire affect the resistance of a wired cube?

According to the formula R = ρ * (L/A), the length of the wire does affect the resistance of a wired cube. The longer the wire, the higher the resistance will be. This is because a longer wire will have more resistance due to the increased distance the electrons must travel through the wire. This is why longer wires tend to have more resistance than shorter wires.

5. Can the resistance of a wired cube be reduced?

Yes, the resistance of a wired cube can be reduced. One way to do this is by using a material with a lower resistivity, such as silver or copper. Another way is to decrease the length of the wire or increase the cross-sectional area. Additionally, using thicker wires or multiple wires in parallel can also reduce the resistance of a wired cube.

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