A telephone cable at a place has four long straight horizontal wires carrying a current of 1.0 A in the same direction east to west. The earth’s magnetic field at the place is 0.39 G, and the angle of dip is 35°. The magnetic declination is nearly zero. What are the resultant magnetic fields at points 4.0 cm below the cable?
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Interpreting the problem statement;
Dip angle δ= 35°
r= 4 cm= 0.04 m
Earth's Magnetic field R= 0.39*10^−4
Horizontal component of the magnetic field H= R cosδ
H =0.39*10^−4 *(cos 35°)
H= 3.19*10^−5 T
B₁= (4*μ₀*2*I)/ (4π *r) =[(4*10^−7)*(2)*(1)] /0.04 =2*10^−5 T
The direction of B₁ at Q is vertically inwards to the plane of paper, and the horizontal component of Earth's magnetic field is given by;
H₁= H + B₁
H₁= (3.19*10^−5) +(2*10^−5 )
H₁= 5.19*10^−5 T
The resultant magnetic field at dip angle;
R= √(H₁²+V²)
R= √{(5.19*10^−5)²+(2.2*10^−5)²} T
R = 5.54*10^−5 T
Hence the resultant magnetic field at point 4 cm above the cable is 5.54*10^−3 T
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