A stronger external magnetic field leads to a higher induced current in the loop.

Faster movement of the loop relative to the magnetic field results in a greater induced current and a stronger magnetic force.

Maximum induced current and magnetic force occur.

The induced current and magnetic force are zero.

Increasing the number of turns or coils in a loop results in a higher induced current.

Translational Acceleration: Results in linear motion, changes the object's position in a straight line. | Rotational Acceleration: Results in rotational motion, changes the object's angular velocity around an axis.

1. Determine the induced current (I) in the conductor. 2. Identify the magnetic field vector ($\vec{B}$). 3. Define the displacement vector ($\vec{d}$). 4. Integrate $I(\vec{d} \times \vec{B})$ over the length of the conductor to find the magnetic force $\vec{F}_{B}$.

1. Identify all forces acting on the loop (including magnetic force). 2. Calculate the net force ($\vec{F}_{net}$). 3. Use $\vec{F}_{net} = m\vec{a}$ to find the acceleration ($\vec{a}$). 4. Use kinematic equations to predict the loop's motion.