The induced voltage is equal in magnitude to the rate of change in flux, Φ, times the number of loops of wire.The flux is equal to BA.
ξ = -Nd(BA)/dt = NBdA/dt =NBvL where L is the length across and v is the velocity of the loop into the field or out of the field and N is the number of loops. There is not induced current when the loop is out of the B field or completely in the B field. Answers to a and c are 0.
ξ = 45* .6 Tesla* 0.1 m* 0.02 m/s = ,054 V. With the field into the plane and the loop is leaving to the right. Lenz's Law states that the induced current will run so as to support the B field that is reducing because the area of the loop in the field is going down. As a result, the current will run clockwise.
I = V/R which I leave to you to calculate.
d) To solve for total charge we need to multiply the current times the time for the loop to leave the field.
The time will be 10 cm/ 2 cm/s = 5 seconds.
Good luck!