The induced emf in the coil is given by Faraday's law:
E=NAdtdB
The resistance of the coil is R=ρal, where l is the total length of the wire and a is its cross-sectional area.
The length of the wire is l=N(2πRc), where Rc is the radius of the coil. Since the area of the coil is A=πRc2, we have Rc=πA.
Thus, l=2NπA.
The cross-sectional area of the wire is a=πr2.
Therefore, the resistance is:
R=ρπr22NπA∝r2NA
The power dissipated in the coil is:
P=RE2∝r2NA(NA)2=NA3/2r2
For the second coil, the parameters are N′=2N, A′=2A, and r′=3r. The new power dissipated is:
P′=P(N2N)(A2A)3/2(r3r)2
P′=P(2)(22)(9)=362P
Given that P′=2αP, we can compare the expressions to find:
2α=362⇒α=36
Answer: 36