Motion of a Charged Particle in a Magnetic Field
- The Lorentz Force on a charged particle moving in a magnetic field is:
\[
\mathbf{F} = q (\mathbf{v} \times \mathbf{B})
\]
- Given \( \mathbf{B} = B_0 \hat{i} \) and \( \mathbf{v} = v_x \hat{i} + v_y \hat{j} \), we calculate the cross-product:
\[
\mathbf{F} = q [(v_x \hat{i} + v_y \hat{j}) \times (B_0 \hat{i})]
\]
- Since \( \hat{i} \times \hat{i} = 0 \) and \( \hat{j} \times \hat{i} = -\hat{k} \), we get:
\[
\mathbf{F} = -q v_y B_0 \hat{k}
\]
- The force acts perpendicular to the velocity component in the \( yz \)-plane, causing circular motion in that plane.
- The velocity component along \( x \)-direction remains unchanged, leading to a helical path.
Thus, the correct answer is (C) helical path.