Evaluate the magnetic field

The magnetic field lines are shown at right. There is not enough symmetry in this situation to invoke Ampere’s law easily for the calculation of the field.

- What is the formula for the Biot-Savart law?

- What is the direction of the contribution to the field
*d***B**contributed by the infinitesimal current segment*d***s**_{1}shown at the top of the loop? Show it on the sketch. - Consider the conjugate element
*d***s**_{2}at the bottom of the loop. Present a sketch or brief discussion that demonstrates that the total field**B**at point*P*is horizontal.Since the final effect of each

*d***B is that only its horizontal component contributes to the total****b**, our final integral need involve only that component from the Biot-Savart law. Any infinitesimal segment*d***s**contributes the same horizontal component regardless of its position on the loop. **Express the horizontal component of***d***B**in terms of*x*and*a*.Since

*d***s**is perperdicular to**r**for all differential current elements, regardless of their position on the loop:Thus the magnitude of the contribution to the magnetic field from the current segment of arc length

*d*s is:**What is the total field strength****B**at point*P*?Integrating over all current segments reduces to evaluation of the circumference of the loop since all contributions

*d*B have the same magnitude:**Check the limit of the above expression for***x*= 0, the point at the center of the loop.The denominator involving

*x*and*a*above reduces to*a*^{3}in this limit. Thus magnetic field at the center of the loop isas expected.

**Check the limit far away;***i.e.*,*x*>>*a*.The denominator involving

*x*and*a*above reduces to*x*^{3}in this limit. Thus the magnetic field behaves as a dipolar field, as expected!

"http://www.physics.udel.edu/~watson/phys208/quiz7soln.html"

Last updated April 17, 1998.

Copyright George Watson, Univ. of Delaware, 1998.