Magnetic field due to a straight current carrying conductor of finite length
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Straight current carrying conductor of finite length –
Suppose a straight current carrying wire AB, carrying current i, lies in the plane of the paper as shown in the figure, P is a point at a perpendicular distance R from conductor, where magnetic field is to be determined.
Conductor
According to Biot-Savart’s Law, the field at point P due to current element idl = qVB→ is
dB =
μ0
4π
idlsinθ
r2
=
μ0I
4π
(
dlsinθ
r
)
i
r
Now from the figure dlsinθ = rdφ and cosφ = R/r
∴ dB =
μ0I
4π
.
cosφ
R
dφ
Hence magnetic field due to the whole conductor
B = θ1∫−θ2 = dB = θ1∫−θ2
μ0I
4πR
cosφ.dφ =
μ0I
4πR
[sinθ1 + sinθ2]
∴ dB =
μ0I
4πR
[sinθ1 + sinθ2]
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