Problem 2:
A certain wire carries a current I and is long and straight except for a semicircular loop of radius R. Consider the magnetic field at the center of the semicircle (center being defined as where the center would be if the circle were whole).
(here r is a unit vector). Define the x-direction as to the right, y-direction as up, and z-direction as out of the page. For any location on the long straight sections, the vector Idl is in the x-direction, and the unit vector r which points from the source of the field (a piece of the straight section) to the field point (the center of the semicircle) is either in the x-direction or the -x direction. Thus the cross product I dl x r is zero (cross product of two parallel or anti-parallel vectors is zero), and so B from these sections is zero (at the center).
Or, use the Biot-Savart law. Consider a piece of the semicircle. Now I dl is tangent to the circle, pointing clockwise, and r is pointing radially inward. Thus their cross product points into the page.
dB =
(µ0/4) I
dl x r/r2
Integrate dB around the semicircle. We note that I, µ0,
4 and r2=R2
are all
constants (a circle is at a constant radius!). We also note that
r and dl are perpendicular so their cross-product is
easy. Thus the integral becomes
B =
(µ0/4) I/R2
dl
The integral is thus the path length around the semicircle, i.e.
R, and we have
B =
(µ0/4)( I
R)/R2 =
(µ0 I) /( 4 R)
plugging in R = 5 cm and I = 2 A we get
B = 1.26 x10-5 T
Problem 3
Test 3
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