A conducting metal circular-wire-loop of radius r is placed perpendicular to a magnetic field which varies with time as B=B₀e⁻ᵗ⁄τ, where B₀ and τ are constants, at time t = 0. If the resistance of the loop is R then the heat generated in the loop after a long time (t→∞) is
π²r⁴B₀⁴/τR
π²r⁴B₀²R/τ
π²r⁴B₀²/τR
π²r⁴B₀/τR
Solution:
Flux through the loop, Φ=→B.→S Φ=B₀πr²e⁻ᵗ⁄τ ε=-dΦ/dt=B₀πr²/τe⁻ᵗ⁄τ Heat Q=∫∞₀ ε²/R dt Q=∫∞₀B₀²π²r⁴e⁻²ᵗ⁄τ/Rτ² dt =[B₀²π²r⁴e⁻²ᵗ⁄τ/2Rτ]∞₀=π²r⁴B₀²/2τR