In a Thomson set-up for the determination of $e/m$,electrons accelerated by $2.5 \ kV$ enter the region of crossed electric and magnetic fields of strengths $3.6 \times 10^4 \ Vm^{-1}$ and $1.2 \times 10^{-3} \ T$ respectively and go through undeflected. The measured value of $e/m$ of the electron is equal to

  • A
    $1.0 \times 10^{11} \ C \ kg^{-1}$
  • B
    $1.76 \times 10^{11} \ C \ kg^{-1}$
  • C
    $1.80 \times 10^{11} \ C \ kg^{-1}$
  • D
    $1.85 \times 10^{11} \ C \ kg^{-1}$

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