The magnetic force on a current-carrying conductor is given by: \[ F = BIL \sin\theta \] Where: \( B = 2 \, \text{T} \), \( I = 3 \, \text{A} \), \( L = 0.5 \, \text{m} \), and \( \theta = 90^\circ \) (perpendicular) \[ F = 2 \times 3 \times 0.5 \times \sin 90^\circ = 3 \, \text{N} \]