Find the current density as a function of distance r from the axis of a radially symmetrical parallel stream of electrons if the magnetic induction inside the stream varies as , where b, are positive constants.
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By ampere's law we have :
B ( r ) ( 2 π r ) = μ 0 ∫ 0 r J ( x ) d S = μ 0 ∫ 0 r ( J ( x ) 2 π x ) d x
⇒ r B ( r ) = μ 0 ∫ 0 r x J ( x ) d x
Applying newton's leibnit'z rule we have :
B ( r ) + r d r d B ( r ) = μ 0 r J ( r ) .
Putting the values we have :
b r α + r ( α b r α − 1 ) = μ 0 r J ( r )
⇒ μ 0 b r α − 1 ( α + 1 ) = J ( r )