the EMF induced across the end of a conductor due to its motion in magnetic field is called

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Solution

$D e a r S t u d e n t, T h e e m f i n d u c e d a c r o s s t h e e n d s o f a c o n d u c t o r d u e t o i t s m o t i o n i n m a g n e t i c f i e l d i s c a l l e d m o t i o n a l e m f . M o t i o n a l e m f i s, ε = B l v M o t i o n a l e m f d e p e n d s o n, 1 . M a g n e t i c f i e l d B . 2 . T h e l e n g t h o f t h e r o d l . 3 . V e l o c i t y a t w h i c h t h e r o d m o v e s v . R e g a r d s .$

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