The magnetic force on a moving proton in a magnetic field is calculated using the formula for the magnetic force on a charged particle:
\[ F = qvB\sin\theta \]
Where:
Given the velocity \(\vec{v} = 10^6 \hat{i} \ \text{m/s}\) (in the \( \hat{i} \) direction) and the magnetic field \(\vec{B} = 0.5 \hat{k} \ \text{T}\) (in the \( \hat{k} \) direction), the angle \(\theta\) between them is \(90^\circ\). Consequently, \(\sin\theta = \sin 90^\circ = 1\).
Substituting the values into the formula yields:
\[ F = (1.6 \times 10^{-19} \ \text{C})(10^6 \ \text{m/s})(0.5 \ \text{T})(1) \]
\[ F = 8.0 \times 10^{-14} \ \text{N} \]
Therefore, the magnitude of the magnetic force acting on the proton is \(8.0 \times 10^{-14} \ \text{N}\).

