A cylindrical conductor AB of non-uniform area of cross-section carries a current of 5 A. The radius of the conductor at one end A is 0.5 cm. The current density at the other end of the conductor is half of the value at A The radius of the conductor at the end B is nearly
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Magnetic field at a distance r inside a conductor of radius R is given by ampere’s circuital law
B×2πr=μ
0
Jπr
2
B=
2
μ
0
Jr
B=
2πR
2
μ
0
rI
Thus magnetic field inside a conductor is given by
B=
2πR
2
μ
0
rI
Magnetic field strength
H=
μ
0
B
H=
2πR
2
Ir
Explanation:
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