Magnetic field strength, B=1.5 T
Radius of the cylindrical region, r=10 cm=0.1 m
Current in the wire passing through the cylindrical region, I=7A
(a) If the wire intersects the axis, then the length of the wire is the diameter of the cylindrical region. Thus, l=2r=0.2 m
Angle between magnetic field and current, θ=90°
Magnetic force acting on the wire is given by the relation,
F=BIl sin θ=1.5×7×0.2×sin 90°=2.1 N
Hence, a force of 2.1 N acts on the wire in a vertically downward direction.
(b) New length of the wire after turning it to the Northeast-Northwest direction can be given as:
l1=lsinθ
Angle between magnetic field and current, θ=45°
Force on the wire,
F=BIl1sin θ
=BIl
=1.5×7×0.2
=2.1 N
Hence, a force of 2.1 N acts vertically downward on the wire. This is independent of angle θ because lsinθ is fixed.
(c) The wire is lowered from the axis by distance, d=6.0 cm
Let l2 be the new length of the wire.
∴(l22)2=4(d+r)
=4(10+6)=4(16)
∴l2=8×2=16 cm=0.16 m
Magnetic force exerted on the wire,
F2=BIl2
=1.5×7×0.16
=1.68 N
Hence, a force of 1.68 N acts in a vertically downward direction on the wire.