Solving Biot Savart Law Homework: Infinitely Long Wire

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Homework Help Overview

The discussion revolves around applying the Biot-Savart Law to determine the magnetic field generated by an infinitely long straight wire carrying a current. The original poster presents an equation derived from the law and seeks clarification on how to transform it into the standard form.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the need to evaluate the limits of the integral involved in the calculation of the magnetic field. There is an exploration of the implications of the wire being infinitely long on the limits of integration.

Discussion Status

The conversation is progressing with participants providing guidance on evaluating the integral limits. The original poster expresses understanding after receiving assistance, indicating a productive exchange of ideas.

Contextual Notes

The problem is constrained by the requirement to apply the Biot-Savart Law and the specific context of an infinitely long wire, which influences the setup of the integral.

mastertan
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Homework Statement



Using the Biot Savart Law

dB = (u0*i*ds X r)/(4*pi*r^3)

*X is cross product

show that the magnetic field due to an infinitely long straight wire carrying a current i ampere is given by

B = (u0*i)/(2*pi*r)

Homework Equations



Hint: integral (Rds/(s^2+R^2)^3/2) = s/(R*(s^2+R^2)^1/2)

The Attempt at a Solution



Eventually I got something like

B = (i*u0*s)/(4pi*R*(s^2+R^2)^1/2)

which I am pretty sure is correct,
but I don't know how to make that equation become

B = (u0*i)/(2*pi*R)

Any ideas? (I hope the question and all the equations make sense)
Thanks
 
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Did you plug the limits of the integral in?
 
I haven't put in the limits. I wasn't too sure what to do.
 
What are the limits on your integral?
 
Is it -infinite and +infinite?
 
Yes. You're told the wire is infinitely long, so s runs from -∞ to +∞, so your expression for B should be

[tex]B = \left.\frac{i \mu_0 s}{4\pi r\sqrt{s^2+r^2}}\right|_{-\infty}^\infty \equiv \lim_{a\to\infty} \left.\frac{i \mu_0 s}{4\pi r\sqrt{s^2+r^2}}\right|_{-a}^a[/tex]
 
Last edited:
Ah I get it now. Thanks very much for helping me out.
 

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