Magnetic field from an infinite sheet of charge

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SUMMARY

The magnetic field generated by an infinite sheet of charge with surface charge density \(\sigma\) moving with velocity \(\vec{v} = v\hat{i}\) is defined as \(\vec{B} = -\frac{1}{2}\mu_0 \sigma v \hat{j}\). This conclusion is derived by integrating along the y-axis, taking into account the symmetry of the problem which results in cancellation of components, leaving only the \(\hat{j}\) direction. The relevant equation for the magnetic field from an infinite wire, \(B = \frac{\mu_0 I}{2\pi R}\), serves as a foundational reference for understanding this scenario.

PREREQUISITES
  • Understanding of electromagnetic theory, specifically the behavior of magnetic fields.
  • Familiarity with the concept of surface charge density (\(\sigma\)).
  • Knowledge of vector calculus, particularly integration along axes.
  • Basic principles of symmetry in physics problems.
NEXT STEPS
  • Study the derivation of the magnetic field from an infinite sheet of charge.
  • Learn about the effects of charge motion on magnetic fields, specifically in the context of special relativity.
  • Explore the relationship between current density and magnetic fields using Ampère's Law.
  • Investigate the implications of magnetic fields in different geometrical configurations, such as infinite wires and sheets.
USEFUL FOR

Students and professionals in physics, particularly those focusing on electromagnetism, as well as educators looking to enhance their understanding of magnetic fields generated by charged surfaces.

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Homework Statement



you have an infinite sheet of charge in the xy plane, with surfance charge density \sigma, that is moving with a velocity \vec{}v = v\hat{}i. Show that the magnetic fiel at some location above the plane (x,y,z,) = (x,y,h,) is given by

\vec{}B = -(1/2)\mu<sub>o</sub>\sigmav\vec{}

Homework Equations



B = \muoi/2piR

The magnetic field from an infinite wire a distance r away from it.

The Attempt at a Solution



I know I have to integrate along the y axis. I also know that there is some cancelation due to symetry and only the j hat componets are left. I'm having trouble relating v, i, and \sigma

Thank you in advance for any help.
 
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sorry about the formating of the answer. It's my first attempt at using the tools.

if it helps

B = (-1/2) mu_o sigma v
in the j hat direction.
 

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