The magnetic field perpendicular to a single 17.2-cm-diameter circular loop of copper wire decreases uniformly from 0.590 T to zero.
If the wire is 2.75 mm in diameter, how much charge moves past a point in the coil during this operation? The resistivity of copper is 1.68×10−8Ω⋅m.
Given
Diameter of the circular loop DL = 17.2 cm = 0.172 m
Diameter of the wire Dw = 2.75 mm = 2.75 x 10-3 m
Resistivity of copper ρ= 1.68 x 10-8 ohm.m
Change in magnetic field ΔB = 0 - 0.590 = -0.590 T
(let’s say the time taken for the filed to go through this change is Δt )
The angle between the surface vector and the field θ = 0o
(the surface vector is perpendicular to surface but parallel to magnetic field)
Solution
Area of the loop
AL = πrL2 = π(DL/2)2 = 3.14 x (0.172/2)2 = 0.02322344 m2
Emf induced in the loop
e = -Acosθ (ΔB/Δt)
e = - 0.02322344 x 1 x (-0.590/Δt)
e = 0.0137018296/Δt
e = IR
0.0137018296/Δt = IR
0.0137018296/Δt = (Δq/Δt)R
0.0137018296= (Δq)R
0.0137018296= (Δq)ρL/Aw
The length of the wire L = 2πrL
Area od cross section of the wire Aw = πrw2
0.0137018296= (Δq)ρ2πrL/πrw2
0.0137018296= (Δq)ρ2rL/rw2
0.0137018296= (Δq)ρDL/rw2
0.0137018296= (Δq) x 1.68 x 10-8 x 0.172 / (2.75 x 10-3/2)2
Δq = 8.96 C
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