$A$ uniform electric field vector $E$ exists along the horizontal direction as shown. The electric potential at $A$ is $V_A$. $A$ small point charge $q$ is slowly moved from $A$ to $B$ along the curved path as shown. The potential energy of the charge when it is at point $B$ is

  • A
    $q(V_A - Ex)$
  • B
    $q(V_A + Ex)$
  • C
    $q(Ex - V_A)$
  • D
    $qEx$

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