Magnetic Field of a Long Straight Wire: Difference between revisions

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Imagine orienting a wire on the y-axis and having a current run through the wire in the +y direction. We are interested in finding the magnetic field at some point along the z axis, say (0,0,z).
Imagine orienting a wire on the y-axis and having a current run through the wire in the +y direction. We are interested in finding the magnetic field at some point along the z axis, say (0,0,z).


From here, it is an integral problem where you take an arbitrary piece of the rod and plug it into the generic formula for change in magnetic field: <math> \vec{B}  =\frac{\mu_0}{4\pi} \frac{(I\vec{l} \times \hat{r})}{x^2+y^2}  </math>
From here, it is an integral problem where you take an arbitrary piece of the rod and plug it into the generic formula for change in magnetic field: <math> \vec{B}  =\frac{\mu_0}{4\pi} \frac{I(\vec{l} \times \hat{r})}{x^2+y^2}  </math>

Revision as of 00:49, 3 December 2015

In many cases, we are interested in calculating the electric field of a long, straight wire. -Claimed by Arjun Patra


Calculation of Magnetic Field

Imagine orienting a wire on the y-axis and having a current run through the wire in the +y direction. We are interested in finding the magnetic field at some point along the z axis, say (0,0,z).

From here, it is an integral problem where you take an arbitrary piece of the rod and plug it into the generic formula for change in magnetic field: [math]\displaystyle{ \vec{B} =\frac{\mu_0}{4\pi} \frac{I(\vec{l} \times \hat{r})}{x^2+y^2} }[/math]