In a typical combustion engine the work done by a gas molecule is given \(W=\alpha^2\beta e^{\frac{-\beta x^2}{kT}}\),
where x is the displacement, k is the Boltzmann constant and T is the temperature. If a and b are constants, dimensions of a will be :
(1) [MLT–2]
(2) [M0LT0]
(3) [M2LT–2]
(4) [MLT–1]