To solve this problem it is necessary to apply the concepts related to Faraday's law and the induced emf.
By definition the induced electromotive force is defined as
[tex]\int E dl = -\frac{d\phi}{dt}[/tex]
[tex]\int E dl = -(\frac{dB}{dt})A[/tex]
Where,
[tex]\phi =[/tex] Electric field
B = Magnetic Field
A = Area
At the theory the magnetic field is defined as,
[tex]B = \mu_0 NI[/tex]
Where,
N = Number of loops
I = current
[tex]\mu_0 =[/tex] Permeability constant
We know also that the cross sectional area, is the area from a circle, and the length is equal to the perimeter then
A = \pi r^2
l = 2\pi r
Replacing at the previous equation we have that
[tex]E (2\pi r) = \mu_0 n (\frac{di}{dt})(\pi R^2)[/tex]
Where,
R = Radius of the solenoid
r = The distance from the axis
Re-arrange to find the current in function of time,
[tex]\frac{di}{dt} = \frac{Er}{\mu_0 NR^2}[/tex]
Replacing our values we have
[tex]\frac{di}{dt} = \frac{(8.00*10^{-6})(0.0348)}{(4\pi*10^{-7})(390)(1.2*10^-2)^2}[/tex]
[tex]\frac{di}{dt} = 3.94487A/s[/tex]