91影视

The penetration depth is the reciprocal of a factor $\left(伪\right)$, which represents how far the wave function, representing the particle inside the well, extends in the classically forbidden region outside the well. It is given as-

$$\begin{gathered} \mathit{未}\mathbf{=}\frac{\mathbf{1}}{\mathbf{伪}} \\ \mathbf{}\mathbf{}\mathbf{}\mathbf{=}\frac{\mathbf{鈩�}}{\sqrt{\mathbf{2}\mathbf{m}\left(U_o-E\right)}}\mathbf{}\mathbf{}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\mathbf{路}\left(1\right) \end{gathered}$$

Here, m and E are the mass and energy of the particle inside the well,role="math" localid="1660113324667" ${\mathbf{U}}_{\mathbf{o}}$is the height of the well, and$\mathit{鈩�}$is the modified Planck鈥檚 constant.

For a particle in the ground state, equation (1) states that the penetration depth is inversely proportional to the square root of the difference in the height of the well and the energy of the particle. As the ground state energy of the particle remains constant, on increasing the walls of the well, wave function in the ground state will penetrate less and less into the classically forbidden region outside of the walls and when the well is infinitely high, the penetration depth is zero.

On increasing the height of the well, the penetration depth decreases. This results in a decrease in the wavelength of the wave inside the well. Hence, the energy increases.

Thus, the penetration of wave function in the forbidden region decreases, and the energy of the wave increases, increasing the height of the well.