The force on a current-carrying conductor in a magnetic field is given by the formula:
\[
F = BIL \sin \theta
\]
Where:
- \( F \) is the force on the conductor,
- \( B \) is the magnetic field strength,
- \( I \) is the current in the conductor,
- \( L \) is the length of the conductor in the magnetic field,
- \( \theta \) is the angle between the magnetic field and the direction of current.
We are given that:
- \( F = 10 \, \text{N} \),
- \( B = 4 \, \text{T} \),
- \( I = 2 \, \text{A} \),
- The angle \( \theta \) is unknown.
Rearranging the formula to solve for \( \sin \theta \):
\[
\sin \theta = \frac{F}{BIL} = \frac{10}{4 \times 2 \times L}
\]
Assuming that the length \( L \) of the conductor is such that the force is maximized, i.e., \( \sin \theta = 1 \), which implies \( \theta = 90^\circ \). Thus, the angle between the current and the magnetic field is \( 90^\circ \).