In a typical combustion engine,the work done by a gas molecule is given by $W = \alpha^{2} \beta e^{\frac{-\beta x^{2}}{kT}}$,where $x$ is the displacement,$k$ is the Boltzmann constant,and $T$ is the temperature. If $\alpha$ and $\beta$ are constants,the dimensions of $\alpha$ will be:

  • A
    $[MLT^{-2}]$
  • B
    $[M^{0}LT^{0}]$
  • C
    $[M^{2}LT^{-2}]$
  • D
    $[MLT^{-1}]$

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