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

  • Thread starter Thread starter bowlbase
  • Start date Start date
  • Tags Tags
    Resistance
Click For Summary
SUMMARY

The discussion focuses on calculating the electrical resistance of a 3D trapezium-shaped conductor with a base A and length L, where the front height is h and the back height is y. The resistance is derived using the formula R=ρL/A, leading to an integral that evaluates to R=ρL/(A(y-h)) ln(y/h). Participants identified issues with the limit as y approaches zero, which complicates the transition to a rectangular solid's resistance. The consensus is that applying the limit before integration simplifies the problem and avoids undefined forms.

PREREQUISITES
  • Understanding of electrical resistance and the formula R=ρL/A
  • Familiarity with calculus, specifically integration techniques
  • Knowledge of limits and their application in calculus
  • Basic geometry of 3D shapes, particularly trapeziums
NEXT STEPS
  • Study the application of limits in calculus, particularly L'Hôpital's rule
  • Explore advanced integration techniques for complex shapes
  • Learn about the physical implications of resistance in non-uniform materials
  • Investigate the geometric properties of trapezoidal shapes in electrical applications
USEFUL FOR

Students in physics or engineering, electrical engineers, and anyone involved in material science or electrical resistance calculations.

bowlbase
Messages
145
Reaction score
2

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:
\frac{z-y}{x}
z=\frac{x}{L} (y-h)+h
That times A (the base) gives area

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

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

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.
 
Physics news on Phys.org
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:

\frac{z-y}{x}=\frac{y-h}{L}
 
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:

\frac{z-y}{x}=\frac{y-h}{L}

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
 

Attachments

  • Fig1.gif
    Fig1.gif
    3.2 KB · Views: 653
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: z=\frac{x}{L} ((y+h)-h)+(y+h)?
 
Okay, here is where I'm at:

Area:


\frac{z-h}{x}=\frac{y+h-h}{L}

\frac{z-h}{x}=\frac{y}{L}

z=\frac{x y}{L}+h

\int \frac{\rho dx}{A\frac{x y}{L}+h}

\frac{\rho}{A}\int \frac{dx}{\frac{x y}{L}+h}

from 0 to L I get

\frac{P}{A}\frac{L}{y}ln(\frac{y+h}{h})

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

\frac{P}{A}\frac{L}{h}

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:


\frac{z-h}{x}=\frac{y+h-h}{L}

\frac{z-h}{x}=\frac{y}{L}

z=\frac{x y}{L}+h

\int \frac{\rho dx}{A\frac{x y}{L}+h}

\frac{\rho}{A}\int \frac{dx}{\frac{x y}{L}+h}

from 0 to L I get

\frac{P}{A}\frac{L}{y}ln(\frac{y+h}{h})

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

\frac{P}{A}\frac{L}{h}

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.

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

-\frac{\rho}{A}\frac{L}{y}ln(\frac{h}{h+y})

With my area:
\frac{\rho}{A}\frac{L}{y}ln(\frac{y+h}{h})
 
  • #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.
 

Similar threads

  • · Replies 10 ·
Replies
10
Views
1K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 36 ·
2
Replies
36
Views
2K
Replies
5
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
Replies
20
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 9 ·
Replies
9
Views
3K