$A$ charged particle of specific charge $\alpha$ is released from the origin at time $t = 0$ with velocity $\vec{V} = V_o \hat{i} + V_o \hat{j}$ in a magnetic field $\vec{B} = B_o \hat{i}$. The coordinates of the particle at time $t = \frac{\pi}{B_o \alpha}$ are (specific charge $\alpha = q/m$):

  • A
    $\left( \frac{V_o}{2 B_o \alpha}, \frac{\sqrt{2} V_o}{\alpha B_o}, \frac{-V_o}{B_o \alpha} \right)$
  • B
    $\left( \frac{-V_o}{2 B_o \alpha}, 0, 0 \right)$
  • C
    $\left( 0, \frac{2 V_o}{B_o \alpha}, \frac{V_o \pi}{2 B_o \alpha} \right)$
  • D
    $\left( \frac{V_o \pi}{B_o \alpha}, 0, - \frac{2 V_o}{B_o \alpha} \right)$

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