91Ó°ÊÓ

The wavelength of source,${\mathrm{λ}}_{source}=532\text{ n³¾}$

The wavelength of observer,${\mathrm{λ}}_{obs}=412\text{ n³¾}$

The expression to calculate the observer frequency in terms of source frequency, speed and speed of light is given as follows.

${\mathit{f}}_{\mathbf{o}\mathbf{b}\mathbf{s}}\mathbf{=}{\mathit{f}}_{\mathbf{s}\mathbf{o}\mathbf{u}\mathbf{r}\mathbf{c}\mathbf{e}}\frac{\sqrt{\mathbf{1}\mathbf{-}{\mathbf{\left(}\frac{\mathbf{v}}{\mathbf{c}}\mathbf{\right)}}^{\mathbf{2}}}}{\mathbf{1}\mathbf{+}\frac{\mathbf{v}}{\mathbf{c}}\mathbf{c}\mathbf{o}\mathbf{s}\mathbf{θ}}$

Here,$\mathrm{θ}$is the angle between the source of light and observer.

The expression between the frequency, wavelength and speed of light is given as follows.

$\mathit{λ}\mathbf{=}\frac{\mathbf{c}}{\mathbf{f}}$

Here,$\mathit{λ}$is the wavelength, $\mathit{c}$is the speed of light and role="math" localid="1658810978725" $\mathit{f}$is the frequency.

Determine the wavelength equation for the observer.

${\mathrm{λ}}_{obs}=\frac{c}{f_{obs}}$

Substitute$f_{source}\frac{\sqrt{1−{\left(\frac{v}{c}\right)}^2}}{1+\frac{v}{c}\cos \mathrm{θ}}$for$f_{obs}$into above equation.

$\begin{array}{l}{\mathrm{λ}}_{obs}=\frac{c}{f_{source}\frac{\sqrt{1−{\left(\frac{v}{c}\right)}^2}}{1+\frac{v}{c}\cos \mathrm{θ}}}\\ {\mathrm{λ}}_{obs}=\frac{c}{f_{source}}\frac{1+\frac{v}{c}\cos \mathrm{θ}}{\sqrt{1−{\left(\frac{v}{c}\right)}^2}}\end{array}$

Substitute${\mathrm{λ}}_{source}$for $\frac{c}{f_{source}}$into above equation.

${\mathrm{λ}}_{obs}={\mathrm{λ}}_{source}\frac{1+\frac{v}{c}\cos \mathrm{θ}}{\sqrt{1−{\left(\frac{v}{c}\right)}^2}}$ …(¾±)

The observed wavelength is shorter than the wavelength in the rest frame. Therefore, light is approaching.The angle between the source and observer when the source moving towards the observe is equal to $180°$.

Substitute $180°$for$\mathrm{θ}$into equation (i).

$\begin{array}{c}{\mathrm{λ}}_{obs}={\mathrm{λ}}_{source}\frac{1+\frac{v}{c}\cos 180°}{\sqrt{1−{\left(\frac{v}{c}\right)}^2}}\\ {\mathrm{λ}}_{obs}={\mathrm{λ}}_{source}\frac{1−\frac{v}{c}}{\sqrt{1−{\left(\frac{v}{c}\right)}^2}}\\ {\mathrm{λ}}_{obs}\sqrt{1−{\left(\frac{v}{c}\right)}^2}={\mathrm{λ}}_{source}(1−\frac{v}{c})\end{array}$

Take a square of both the sides of the above equation.

$\begin{array}{c}{\mathrm{λ}}_{0bs}^2[1−{\left(\frac{v}{c}\right)}^2]={\mathrm{λ}}_{source}^2{(1−\frac{v}{c})}^2\\ {\mathrm{λ}}_{0bs}^2\left[(1−\frac{v}{c})(1+\frac{v}{c})\right]={\mathrm{λ}}_{source}^2{(1−\frac{v}{c})}^2\\ {\mathrm{λ}}_{0bs}^2(1+\frac{v}{c})={\mathrm{λ}}_{source}^2(1−\frac{v}{c})\\ {\mathrm{λ}}_{0bs}^2+\frac{v}{c}{\mathrm{λ}}_{0bs}^2={\mathrm{λ}}_{source}^2−{\mathrm{λ}}_{source}^2\frac{v}{c}\end{array}$

Solve further as,

$\begin{array}{c}\frac{v}{c}{\mathrm{λ}}_{0bs}^2+{\mathrm{λ}}_{source}^2\frac{v}{c}={\mathrm{λ}}_{source}^2−{\mathrm{λ}}_{0bs}^2\\ \frac{v}{c}({\mathrm{λ}}_{0bs}^2+{\mathrm{λ}}_{source}^2)={\mathrm{λ}}_{source}^2−{\mathrm{λ}}_{0bs}^2\\ \frac{v}{c}=\frac{{\mathrm{λ}}_{source}^2−{\mathrm{λ}}_{0bs}^2}{{\mathrm{λ}}_{0bs}^2+{\mathrm{λ}}_{source}^2}\end{array}$

Substitute$532\text{ n³¾}$ for ${\mathrm{λ}}_{source}$and$412\text{ n³¾}$ for${\mathrm{λ}}_{obs}$ into above equation.

$\begin{array}{c}\frac{v}{c}=\frac{{532}^2−{412}^2}{{532}^2+{412}^2}\\ \frac{v}{c}=\frac{113280}{452768}\\ \frac{v}{c}=0.25\\ v=0.25c\end{array}$

Hence the velocity of the source is $0.25c$and it is approaching towards the source.

The speed of the light would be the same in the opposite direction but the angle between the observer and source is$0°$.

Calculate the wavelength of the light,

Substitute $532\text{ n³¾}$for${\mathrm{λ}}_{source}$, $0°$for $\mathrm{θ}$and$0.25c$for $v$into equation (i).

$\begin{array}{l}{\mathrm{λ}}_{source}=532×{10}^{−9}\frac{1+\frac{0.25c}{c}\cos 0}{\sqrt{1−{\left(\frac{0.25c}{c}\right)}^2}}\\ {\mathrm{λ}}_{source}=532×{10}^{−9}\frac{1+0.25}{\sqrt{1−0.0625}}\\ {\mathrm{λ}}_{source}=532×{10}^{−9}×1.29\\ {\mathrm{λ}}_{source}=687\text{ n³¾}\end{array}$

Hence the wavelength of the light when the light is receding is$687\text{ n³¾}$ .

The speed of the light would be the same but for circling the Earth the angle between the observer and source is $90°$.

Calculate the wavelength of the light,

Substitute $532\text{ n³¾}$for${\mathrm{λ}}_{source}$ ,$90°$for$\mathrm{θ}$ and$0.25c$ for$v$ into equation (i).

$\begin{array}{l}{\mathrm{λ}}_{source}=532×{10}^{−9}\frac{1+\frac{0.25c}{c}\cos 90°}{\sqrt{1−{\left(\frac{0.25c}{c}\right)}^2}}\\ {\mathrm{λ}}_{source}=532×{10}^{−9}\frac{1}{\sqrt{1−0.0625}}\\ {\mathrm{λ}}_{source}=532×{10}^{−9}×1.032\\ {\mathrm{λ}}_{source}=549\text{ n³¾}\end{array}$

Hence the wavelength of the light for circling the Earth $549\text{ n³¾}$.