Therefore, the radius r should increase at a rate of approximately 0.0109 meters per second to maintain zero induced emf in the loop.
The key to solving this problem lies in Faraday's Law of Electromagnetic Induction, which states:
ε = -N dΦ/dt
where:
ε is the induced emf in the loop
N is the number of turns (1 in this case)
Φ is the magnetic flux through the loop
dΦ/dt is the rate of change of magnetic flux
For a circular loop in a uniform magnetic field, the magnetic flux is given by:
Φ = BA
where:
B is the magnetic field strength
A is the area of the loop
In this case, A = πr^2.
We are given that the magnetic field magnitude is decreasing at a constant rate of -1.7 × 10^-2 T/s. Therefore, the rate of change of magnetic flux is:
dΦ/dt = -Bπr^2 d(B)/dt = -1.7 × 10^-2 πr^2 (0.520 T/s)
We want the induced emf ε to be zero. From Faraday's Law, this means:
0 = -1.7 × 10^-2 πr^2 (0.520 T/s) - N r dr/dt
Since N = 1, we can solve for dr/dt:
dr/dt = (1.7 × 10^-2 πr^2 (0.520 T/s)) / r
Substituting r = 0.2 m (20 cm) and the given values:
dr/dt = (1.7 × 10^-2 π (0.2 m)^2 (0.520 T/s)) / 0.2 m
≈ 0.0109 m/s