It is given that the rate of change of the de-Broglie wavelength \( \lambda \) of an electron is inversely proportional to the \( n \)th power of the distance traveled. The objective is to determine the value of \( n \). The de-Broglie wavelength \( \lambda \) of an electron is defined as: \[\lambda = \frac{h}{p}\] where \( h \) represents Planck's constant, and \( p \) denotes the momentum of the electron. The momentum of the electron within the electric field of a sheet is affected by the force exerted on it by the sheet, which is contingent upon the electric field produced by the sheet. The electric field \( E \) generated by a uniformly charged sheet is given by: \[E = \frac{\sigma}{2\epsilon_0}\] The force \( F \) acting on the electron is: \[F = eE = e \frac{\sigma}{2\epsilon_0}\] The rate of change of momentum is equivalent to the force, i.e., \[\frac{dp}{dt} = F\] From the definition of momentum, \( p = mv \), where \( m \) is the mass of the electron and \( v \) is its velocity. As velocity is proportional to momentum, the rate of change of velocity is related to the force. Consequently, the de-Broglie wavelength varies inversely with the square root of the distance traveled. Thus, the rate of change of de-Broglie wavelength is inversely proportional to the \( \frac{1}{2} \) power of the distance traveled. Therefore, \( n \) is equal to \( \frac{1}{2} \).