Physics > Wave Optics > 1.0 Introduction
Wave Optics
1.0 Introduction
1.1 Wavefronts
1.2 Huygens Principle
1.3 Interference of light
1.4 Intensity distribution
1.5 Phase difference
2.0 Young's double slit experiment
3.0 Diffraction of light
4.0 Polarisation
1.4 Intensity distribution
1.2 Huygens Principle
1.3 Interference of light
1.4 Intensity distribution
1.5 Phase difference
If $A_1$ and $A_2$ are the amplitudes of interfering waves due to two coherent sources $S_1$ & $S_2$ and $\phi $ is constant phase difference between the two waves at any point $P$, then the resultant amplitude at point $P$ will be,
$$R = \sqrt {A_1^2 + A_2^2 + 2{A_1}{A_2}\cos \phi } \quad ...(i)$$
where $R$ is the resultant of the two interfering waves.
As we know, the relation between amplitudes and intensity we can write, \[\left. \begin{gathered} {I_1} = A_1^2 \hspace{1em} \\ {I_2} = A_2^2 \hspace{1em} \\ I = {R^2} \hspace{1em} \\ \end{gathered} \right\}\quad ...(ii)\]
From equation $(i)$ and $(ii)$ we get,
$$\begin{equation} \begin{aligned} {R^2} = A_1^2 + A_2^2 + 2{A_1}{A_2}\cos \phi \\ I = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \cos \phi \\\end{aligned} \end{equation} $$
If $I_1=I_2=I_0$, $$\begin{equation} \begin{aligned} I = {I_0} + {I_0} + 2\sqrt {{I_0}{I_0}} \cos \phi \\ I = 2{I_0}\left( {1 + \cos \phi } \right) \\ I = 4{I_0}{\cos ^2}\left( {\frac{\phi }{2}} \right) \\\end{aligned} \end{equation} $$
For constructive interference
$$I = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \cos \phi $$ For constructive interference or maximum intensity,
$$\begin{equation} \begin{aligned} \cos \phi = 1 \\ \phi = 2n\pi \quad {\text{where }}n \in I \\\end{aligned} \end{equation} $$ So, $$\begin{equation} \begin{aligned} I = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \\ I = {\left( {\sqrt {{I_1}} + \sqrt {{I_2}} } \right)^2} \\\end{aligned} \end{equation} $$
If $I_1=I_2=I_0$, then, $${I_{\max }} = 4{I_0}$$
For destructive interference
$$I = {I_1} + {I_2} + 2\sqrt {{I_1}{I_2}} \cos \phi $$ For destructive interference or minimum intensity,
$$\begin{equation} \begin{aligned} \cos \phi = - 1 \\ \phi = (2n + 1)\pi \quad {\text{where }}n \in I \\\end{aligned} \end{equation} $$ So, $$\begin{equation} \begin{aligned} I = {I_1} + {I_2} - 2\sqrt {{I_1}{I_2}} \\ I = {\left( {\sqrt {{I_1}} - \sqrt {{I_2}} } \right)^2} \\\end{aligned} \end{equation} $$
If $I_1=I_2=I_0$, then, $${I_{\min }} = 0$$
For incoherent sources
When the sources are incoherent, resultant intensity is given by,
$$I = {I_1} + {I_2}$$