Consider a circular loop of wire carrying current \(I\) in a homogeneous (constant) magnetic field.
The loop is in the \(xy\)-plane and the current goes in the counter-clockwise direction (if you're looking down onto the \(xy\)-plane). The magnetic field is \(\vec{B}=B_0 \left(\sin\alpha\, \hat{x}+\cos\alpha\, \hat{z}\right)\).
(2pts) The Lorentz Force Law \[\vec{F}=q_{\hbox{test}} \left(\vec{E}+\vec{v}\times\vec{B}\right)\] says that the moving charges in the loop will experience a force due to the magnetic field.
Rewrite the Lorentz Force Law as an integral over the current in the loop. Describe in words how you did the conversion, don't just look up a formula in a book.