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**1. Homework Statement**

Loop of current ##I## sitting in the xy plane. Current goes in counter clockwise direction as seen from positive z axis. Find:

a) the magnetic dipole moment

b) the approximate magnetic field at points far from the origin

c) show that, for points on the z axis, your answer is consistent with the exact field (Ex. 5.6), when z R.

**2. Homework Equations**

##\vec{m} = I \int d\vec{A}##

##\vec{A}_{dip} (\vec{r}) = \frac{\mu_0 \vec{m} \times \hat r}{4 \pi r^2}##

##\vec{B}=\nabla \times \vec{A}##

**3. The Attempt at a Solution**

a) I got that this is ##I\pi R^2 \hat z##

b) I got ##\vec{A}_{dip} (\vec{r}) = \frac{\mu_0 I R^2}{4 r^2}(\hat z \times \hat r)##, but I don't know how to interpret ##(\hat z \times \hat r)##. I tried taking the vector product by treating them as cylindrical coordinates and using the conversion to cartesian, which resulted in ##\hat \phi##. So it says that the vector potential curls around the z axis, which doesn't make sense...

Then I know I have to do ##\vec{B}=\nabla \times \vec{A}##, but that's contingent on the previous part being correct.

c) ???

Any tips?

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