Concept:
- The magnetic force on a moving charge is a vector quantity given by the Lorentz force law $\vec{F} = q(\vec{v} \times \vec{B})$; the familiar scalar formula $qvB\sin\theta$ is just the magnitude of this cross product.
- Placing the velocity and magnetic field along two perpendicular coordinate axes makes the perpendicular condition automatic and lets the force be computed directly using vector identities instead of remembering to substitute $\sin 90^\circ$.
Step 1: Set up the velocity and field as perpendicular vectors along the axes.
Since the proton enters perpendicular to the field, take:
$\vec{v} = v\,\hat{x} = (3\times10^6)\,\hat{x}\ \text{m/s}$
$\vec{B} = B\,\hat{y} = (2)\,\hat{y}\ \text{T}$
Step 2: Compute the cross product $\vec{v} \times \vec{B}$.
$\vec{v} \times \vec{B} = (v\,\hat{x}) \times (B\,\hat{y}) = vB\,(\hat{x} \times \hat{y}) = vB\,\hat{z}$
using the standard identity $\hat{x} \times \hat{y} = \hat{z}$.
Step 3: Substitute the numeric values to get the magnitude of $\vec{v} \times \vec{B}$.
$|\vec{v} \times \vec{B}| = vB = (3\times10^6)(2) = 6\times10^6$
Step 4: Multiply by the charge to get the force.
$F = q\,|\vec{v} \times \vec{B}| = (1.6\times10^{-19})(6\times10^6)$
$F = 9.6\times10^{-13}\ N$
Final Answer: $F = 9.6\times10^{-13}\ N$, directed along $\hat{z}$, perpendicular to both $\vec{v}$ and $\vec{B}$