How Does the Shape of a 3D Trapezium Affect Electrical Resistance?

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Homework Help Overview

The problem involves determining the electrical resistance of a current moving through a 3D trapezium-shaped conductor, characterized by a base A, length L, and varying heights at the front (h) and back (Y). The original poster seeks to understand how the shape influences resistance, particularly when considering limits that lead to a rectangular solid.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the geometry of the trapezium and its implications for resistance calculations, including the area and integral setup. There are questions about the correctness of the area equation and the behavior of the integral as limits are approached, particularly when y approaches zero.

Discussion Status

Participants are actively exploring different interpretations of the geometry and its mathematical representation. Some have offered insights into the area calculations and integral evaluations, while others express uncertainty about the implications of setting limits and the resulting forms of their equations.

Contextual Notes

There is a noted complexity in the problem due to the potential for indefinite forms when limits are applied. Participants are also navigating the challenge of accurately representing the trapezium's shape in their calculations.

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Homework Statement


The shape is 3D trapezium with a base A and a length L. The front end is shorter than the back. The front is height h and the back height Y.

What is the resistance of a current moving from h to Y?


Homework Equations


R=ρL/A


The Attempt at a Solution



First to determine the area:
[itex]\frac{z-y}{x}[/itex]
[itex]z=\frac{x}{L} (y-h)+h[/itex]
That times A (the base) gives area

The integral:
[itex]\int \frac{\rho dx}{A\frac{x}{L} (y-h)+h}[/itex]

evaluated from 0 to L I get:
[itex]\frac{\rho L}{A(y-h)} ln(\frac{y}{h})[/itex]

This seems straight forward but I have a problem. The next step of the problem asks that I set the limit of y to zero so that the previous solution will give the resistance of a rectangular solid. This doesn't seem to work as the first half will be negative and the natural log becomes undefined.

I'm not sure that the integral is correct as my calculator, wolfram alpha and myself get differing answers. Though I think I made a mistake that puts me on wolframs side now. Also, the equation for the area may be incorrect though I am pretty sure that I got it correct.

Any assistance would be appreciated.
 
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From your description of the geometry, if you let y go to zero won't you end up with a wedge rather than a rectangular solid? Perhaps the height of the 'back end' is meant to be y+h?
 
I tried to draw it but it ended up looking terrible.


So it is basically a right triangle sitting on top of a rectangle when you look at it from the side. Also it is 'A' deep from this perspective and both are 'L' long. The point of the triangle is (the short side) is height 'h' and the back side is height 'y.' So when 'y' goes to zero the triangle goes away. It is not quite y+h. Rather you could say it is h+(some other variable)=y.

Trying to find a picture of one on the internet is surprisingly difficult.

Also, for some reason my area equation got cut off:

[itex]\frac{z-y}{x}=\frac{y-h}{L}[/itex]
 
bowlbase said:
I tried to draw it but it ended up looking terrible.


So it is basically a right triangle sitting on top of a rectangle when you look at it from the side. Also it is 'A' deep from this perspective and both are 'L' long. The point of the triangle is (the short side) is height 'h' and the back side is height 'y.' So when 'y' goes to zero the triangle goes away. It is not quite y+h. Rather you could say it is h+(some other variable)=y.

Trying to find a picture of one on the internet is surprisingly difficult.

Also, for some reason my area equation got cut off:

[itex]\frac{z-y}{x}=\frac{y-h}{L}[/itex]

I still don't see how if, the back end has height y, when y goes to zero the back end can be anything but zero height. That makes it the thin end of a wedge.

attachment.php?attachmentid=53088&stc=1&d=1353256880.gif
 

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Shoot, you're right. The back end is y+h. I don't know why I made that mistake. So, you'd be right if it is as I said. You're drawing is correct although except for that. The current runs right to left as pictured there.

Sorry about that mistake.
 
My area has to be wrong. I was using that Y as my total back end length in my area equation.

Can I simply modify it as so or is it totally wrong now: [itex]z=\frac{x}{L} ((y+h)-h)+(y+h)[/itex]?
 
Okay, here is where I'm at:

Area:


[itex]\frac{z-h}{x}=\frac{y+h-h}{L}[/itex]

[itex]\frac{z-h}{x}=\frac{y}{L}[/itex]

[itex]z=\frac{x y}{L}+h[/itex]

[itex]\int \frac{\rho dx}{A\frac{x y}{L}+h}[/itex]

[itex]\frac{\rho}{A}\int \frac{dx}{\frac{x y}{L}+h}[/itex]

from 0 to L I get

[itex]\frac{P}{A}\frac{L}{y}ln(\frac{y+h}{h})[/itex]

So, in my final answer if y goes to zero I have a problem. But if y=0 in my integral it works out quite nicely to

[itex]\frac{P}{A}\frac{L}{h}[/itex]

Which is what I believe a rectangular solid to be. I'm just worried now that perhaps my original answer was intended to have the limit set to zero which would make it answer incorrect.

Does this look ship shape to you?
 
If h is the height of the rectangular slab, and y is the "back end" thickness of the triangular wedge sitting on it, then you can describe the height w.r.t. x (x being the distance from the "back end") as:

z = (h+y) - x*(y/L)

The cross sectional area is then z*A
 
bowlbase said:
Okay, here is where I'm at:

Area:


[itex]\frac{z-h}{x}=\frac{y+h-h}{L}[/itex]

[itex]\frac{z-h}{x}=\frac{y}{L}[/itex]

[itex]z=\frac{x y}{L}+h[/itex]

[itex]\int \frac{\rho dx}{A\frac{x y}{L}+h}[/itex]

[itex]\frac{\rho}{A}\int \frac{dx}{\frac{x y}{L}+h}[/itex]

from 0 to L I get

[itex]\frac{P}{A}\frac{L}{y}ln(\frac{y+h}{h})[/itex]

So, in my final answer if y goes to zero I have a problem. But if y=0 in my integral it works out quite nicely to

[itex]\frac{P}{A}\frac{L}{h}[/itex]

Which is what I believe a rectangular solid to be. I'm just worried now that perhaps my original answer was intended to have the limit set to zero which would make it answer incorrect.

Does this look ship shape to you?

The problem is tricky because the straightforward approach leads to an indefinite form when y is allowed to go to zero after integration. It would be better to apply the limit before integrating.

Note that the expression for the area can be rearranged:
$$Area = z A = \left((h + y) - \frac{x}{L}y\right)A = \left( \left(1 - \frac{x}{L}\right)y + h\right)A$$
If y is allowed to go to zero then the term on the left disappears without a struggle.
 
Last edited:
  • #10
I get a slightly different answer from your area equation.

[itex]\int \frac{\rho dx}{A(h+y)-x\frac{y}{L}}[/itex]

[itex]-\frac{\rho}{A}\frac{L}{y}ln(\frac{h}{h+y})[/itex]

With my area:
[itex]\frac{\rho}{A}\frac{L}{y}ln(\frac{y+h}{h})[/itex]
 
  • #11
Yeah, sorry, I missed carrying the base width "A" though the area rearrangement; I edited my previous post accordingly.

Note that if you apply the limit y → 0 in your result you end up with the indefinite form 0/0.

Either apply the limit before integration (simple) or deal with the indefinite form afterward (L'Hopital).
 
  • #12
I went ahead and inserted the A into the integral before. We're very similar but for the log and the negative sign.

Actually, I think we're exactly the same except for your negative sign which actually cancels from the log since h/(h+y) is less than 1.

That's sort of an interesting result. Are we both correct then or is that just a wildly unlikely coincidence?
 
  • #13
bowlbase said:
I went ahead and inserted the A into the integral before. We're very similar but for the log and the negative sign.

Actually, I think we're exactly the same except for your negative sign which actually cancels from the log since h/(h+y) is less than 1.

That's sort of an interesting result. Are we both correct then or is that just a wildly unlikely coincidence?

It's no coincidence that the results are the same since it was only an algebraic rearrangement of the integrand.
 

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