Proving Force on Arbitrary Wire Same as Straight Wire

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Homework Help Overview

The discussion revolves around proving that the force on a wire of arbitrary shape carrying a current is the same as that on a straight wire carrying the same current in a uniform magnetic field. Participants explore the mathematical representation of the forces involved and the implications of integrating along different paths.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integral of the differential along the curvy wire and question whether this integral depends on the path taken. They also explore the nature of the force due to a magnetic field and its conservative properties.

Discussion Status

The conversation is ongoing, with participants providing insights and hints to guide each other towards understanding the integral's properties and the implications of vector notation. There is a focus on clarifying concepts without reaching a definitive conclusion.

Contextual Notes

There is an emphasis on the vector nature of points a and b, and participants are encouraged to consider the implications of their mathematical expressions and assumptions about the magnetic force.

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The figure shows a wire of arbitrary shape carrying a current i between points a and b. The wire lies in a plane at right angles to a uniform magnetic field B. Prove that the force on the wire is the same as that on a straight wire carrying a current i directly from a to b. (Hint: Replace the wire by a series of "steps" that are parllel and perpendicular to the straight line jkoining a and b.)
WEll umm
well the force on the stirahgt wire from a to b is simply
[tex]F = iL \cross B = iLB \sin( \theta)[/tex]
for the arbitrary wire
[tex]F = \int idL \cross B[/tex]
but i is constant and B is constant so
[tex]F = iB \int dL = iBL[/tex] whicvh is the same as the stariaght wire. Is this correct?
 

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See my reply to your other post. What is the integral
[tex] \int d\vec{\ell}[/tex]
along the curvy wire from [tex]\vec{a}[/tex] to [tex]\vec{b}[/tex]? Does the integral depend on path? Why?
 
The only reason i can think of an integral not depending on path is because a force is conservative. But why is the force due to a magnetic field conservative? Is it because the energy reamins constant in this system?
 
You are integrating a differential, what does that tell you about the result of the integration? If you are uncomfortable with this argument and want to be a bit more formal, then try using the fundamental theorem of line integrals on the integral
[tex] \int_C \vec{v}\cdot d\vec{\ell} = \vec{v} \cdot \int_C d\vec{\ell}[/tex]
where [tex]\vec{v}[/tex] is an arbitrary vector and C is a path from [tex]\vec{a}[/tex] to [tex]\vec{b}[/tex]. Hint: is [tex]\vec{v}[/tex] the gradient of something? What does this result tell you about [tex] \int_C d\vec{\ell} \,\, ?[/tex]
 
ok the result of this integration [tex]v \oint dl = v \int_{a}^{b} dl = v [l]_{a}^{b} = v (b - a)[/tex]

im not sure what v is the gradient of, however.
 
A couple of things and you should have your answer.

First, don't forget that [tex]\vec{a}[/tex] and [tex]\vec{b}[/tex] are vectors. I don't know if you're confused about this, or if you just don't bother to notate it, or if you can't get LaTeX to work. I just wanted to emphasize this point either way.

Second, are you sure you can't find a function that [tex]\vec{v}[/tex] is the gradient of? Hint: the partial derivative with respect to x of your unknown function is [tex]v_x[/tex], a constant.

Third, your very close to your answer, here and in the other thread. All you need to do is convince yourself (or more properly, the grader) that
[tex] \int_C d\vec{\ell} = \vec{b} - \vec{a}[/tex]
independent of the path C. Once you have this fact, the answers to both your questions are easy to get.
 

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