Integration using substitution

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Homework Help Overview

The problem involves calculating the resistance of a wire shaped like a truncated cone, with given radii, resistivity, and length. The original poster attempts to use the formula R = ρL/A, where A is the cross-sectional area, and is facing challenges with integration by substitution.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the setup of the integral for resistance and the difficulties encountered with the integration process. Questions arise about the dimensionality of the wire and the definition of its cross-section.

Discussion Status

Some participants have provided clarifications regarding the geometry of the wire and its implications for the resistance calculation. There is an ongoing exploration of the integration process, with no explicit consensus reached on the method to resolve the original poster's difficulties.

Contextual Notes

Participants note the need for clarity on the dimensional aspects of the wire and the assumptions regarding its shape and cross-section. The original poster's setup may lack certain details necessary for a complete understanding of the problem.

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Homework Statement



I have a wire in the shape of a truncated cone. One side has radius a and the other has radius b. The wire has resistivity ρ and length L. I am supposed to find the resistance of the wire using R = ρL/A

Homework Equations



R= ρL/A

The Attempt at a Solution



So far I have set up my integeral. I know the answer, but I am having trouble with the actual integration by substitution.

ρ∫ dx / (π * (a + (b - a)(x / L))^2)

u = a + (b - a)(x / L)

du = ( b - a ) / L

This just gets me into a huge mess. The answer is ρL/ab. Thanks for any help.
 
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This just gets me into a huge mess
How does this huge mess look like? It should be quite simple.

du= is missing a dx.
 
How can you have a wire (one-dimensional) "in shape of a truncated cone" (three dimensional).
 
A wire is not a line, it has a finite cross-section.
 
Oh, I see. Thanks. So we are just talking about the truncated cone.

Since the sides are lines, the diameter at each point is a linear function of ditance along the axis. Taking x= 0 where the diameter is "b" and x= L where it is a, we have d= (a- b)(x/L)+ b so that the radius is d/2= (a- b)(x/2L)+ b/2 and the cross section area is [itex]A= \pi (a- b)^2(x^2/4L^2)+ \pi(a- b)(x/2L)b+ \pi b^2/4[/itex].

Since [itex]R= \rho L/A[/itex], with a small section of length "dx", [itex]R=\rho dx/A= \rho dx/(\pi (a- b)^2(x^2/4L^2)+ \pi(a- b)(x/2L)b+ \pi b^2/4)[/itex] and the total resistance is the integral of that, with respect to x, from 0 to L.

Drawing a thin "lamina" perpendicular to the
 

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