The force on a proton moving in a magnetic field is given by the formula:
\[
F = qvB \sin \theta
\]
Where:
- \( q \) is the charge of the proton \( = 1.6 \times 10^{-19} \, \text{C} \)
- \( v \) is the velocity \( = 4 \times 10^5 \, \text{m/s} \)
- \( B \) is the magnetic field intensity \( = 2500 \, \text{N/Amp-m} \)
- \( \theta = 0^\circ \) (since the proton is moving parallel to the magnetic field)
Since \( \sin 0^\circ = 0 \), the force on the proton is:
\[
F = 1.6 \times 10^{-19} \times 4 \times 10^5 \times 2500 \times 0 = 0 \, \text{N}
\]
Thus, the force exerted on the proton is 0 N.