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Electromagnetic theory miscellaneous

Electromagnetic Theory

  1. A magnetic field →B = ( →a x + 2 →a y· 4 →a z) exists at a point is →E, a test charge moving with a velocity, →v = v0 (3 →a x – →a y + 2 →a z) experiences no force at a certain point, the electric field at that point will be—

    1. →→→→
      E = −v0(3ax − 2ay − 4az)

    2. →→→
      E = −v0(14ay + 7az)

    3. →→→
      E = −
      v0
      (14ay + 7az)
      μ

    4. →→→
      E = +
      v0
      (14ay + 7az)
      μ
Correct Option: B

B = →→→
(ax+2ay - 4az)

v = v0→→→
(3ax-ay + 2az)

Force on the charge q moving with velocity v in a magnetic field B is given by F = q.v
=V0 →→→→→→
(3ax-ay+az)×(ax+ay-4ax)

=V0 →→→→→→
(6ax-12ay+az+ 4ax+2ay-4ax)

= v0→→
(14ay + 7az)

The electric force is FE = qE
Thus, qv × B – qE=0
or
E = – v × B
∴ E = – v0→→
(14ay + 7az)



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