A very high magnetic field is applied to a stationary charge. Then the charge experiences
A
A force in the direction of magnetic field
B
A force perpendicular to the magnetic field
C
A force in an arbitrary direction
D
No force
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D
No force
d (d) ${F_m} = qvB\sin \theta $, if $v = 0\; \Rightarrow {F_m} = 0$
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