An electron accelerated through a potential difference $V$ enters a uniform transverse magnetic field and experiences a force $F$. If the accelerating potential is increased to $2V$, the electron in the same magnetic field will experience a force

  • A

    $F$

  • B

    $\frac{F}{2}$

  • C

    $\sqrt 2 F$

  • D

    $2F$

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