91Ó°ÊÓ

An electromagnetic wave incident over an obstacle with a certain angle reflects that wave maintaining the same angle for a flat surface. This reflected wave is called a reflection of the incident wave.

a.

In figure 35.35, we can conclude that ray 1 travels an extra distance of $4L$more than ray 2.

Therefore to get the least possible length that will result in destructive interference, it is required to set the extra distance equated to half of the wavelength.

$$\begin{gathered} 4L=\frac{\mathrm{λ}}{2} \\ L=\frac{\mathrm{λ}}{8} \end{gathered}$$.

Here it is given that the wavelength $\mathrm{λ}$ is 420 nm.

Therefore,

$$\begin{gathered} L=\frac{420×{10}^{-9}}{8} \\ =52.50\text{nm} \end{gathered}$$.

b.

In figure 35.35, we can conclude that ray 1 travels an extra distance of $4L$more than ray 2.

Therefore to get the second least possible length that will result in destructive interference, it is required to set the extra distance equated $\frac{3}{2}$of the wavelength.

$$\begin{gathered} 4L=\frac{3}{2}\mathrm{λ} \\ L=\frac{3}{8}\mathrm{λ} \\ L=\frac{3}{8}×\left(420\text{nm}\right) \\ L=157.5\text{nm} \end{gathered}$$.