Solving Biot Savart Law Homework: Infinitely Long Wire

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SUMMARY

The discussion centers on applying the Biot-Savart Law to derive the magnetic field produced by an infinitely long straight wire carrying a current of i amperes. The initial expression derived is B = (i*u0*s)/(4*pi*R*(s^2+R^2)^(1/2)). Participants clarify that the limits of integration for the variable s must be set from -∞ to +∞, leading to the final result B = (u0*i)/(2*pi*R). The integral hint provided is crucial for achieving this transformation.

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  • Familiarity with vector calculus, specifically cross products
  • Knowledge of limits and integration techniques in calculus
  • Basic concepts of magnetic fields and current-carrying conductors
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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

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
 
Last edited:
Ah I get it now. Thanks very much for helping me out.
 

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