Wave Optics
ЁЯУР Formula & Cheat Sheet (English)
Quick Revision Notes: Class 12 Physics
Chapter: Wave Optics (рдкреНрд░рдХрд╛рд╢рд┐рдХреА)
### 1. Wavefront and Huygens' Principle (рддрд░рдВрдЧрд╛рдЧреНрд░ рддрдерд╛ рд╣рд╛рдЗрдЧреЗрдиреНрд╕ рдХрд╛ рд╕рд┐рджреНрдзрд╛рдиреНрдд)
- Wavefront (рддрд░рдВрдЧрд╛рдЧреНрд░): The locus of all adjacent points vibrating in the same phase is called a wavefront.
- Types: Spherical (рдЧреЛрд▓реАрдп), Cylindrical (рдмреЗрд▓рдирд╛рдХрд╛рд░), and Plane (рд╕рдорддрд▓).
- Huygens' Principle (рд╣рд╛рдЗрдЧреЗрдиреНрд╕ рдХрд╛ рд╕рд┐рджреНрдзрд╛рдиреНрдд):
- Every point on a given wavefront acts as a source of secondary wavelets (рджреНрд╡рд┐рддреАрдпрдХ рддрд░рдВрдЧрд┐рдХрд╛рдПрдБ) travelling in all directions with the speed of light.
- The envelope of these secondary wavelets at any later time gives the new position of the wavefront.
- Laws of Reflection and Refraction: Huygens' principle successfully explains the laws of reflection ($\angle i = \angle r$) and refraction ($\frac{\sin i}{\sin r} = \frac{v_1}{v_2} = \mu$).
### 2. Interference of Light Waves (рдкреНрд░рдХрд╛рд╢ рдХрд╛ рд╡реНрдпрддрд┐рдХрд░рдг)
The modification in the intensity of light due to the superposition of two or more light waves is called interference.
- Superposition Principle: Resultant displacement $y = y_1 + y_2$.
- Condition for Sustained Interference: The sources must be coherent (рдХрд▓рд╛-рд╕рдВрдмрджреНрдз) i.e., they must maintain a constant phase difference.
Mathematical Analysis:
Let two waves be:
-
$y_1 = a_1 \sin(\omega t)$
-
$y_2 = a_2 \sin(\omega t + \phi)$
-
Resultant Amplitude ($R$):
R = sqrt(a_1^2 + a_2^2 + 2a_1a_2 \cos\phi) -
Resultant Intensity ($I$): Since $I \propto R^2$,
I = I_1 + I_2 + 2\sqrt{I_1I_2} \cos\phi
Conditions for Interference:
-
Constructive Interference (рд╕рдВрдкреЛрд╖реА рд╡реНрдпрддрд┐рдХрд░рдг - Maximum Intensity):
- Path difference ($\Delta x$):
\Delta x = n\lambda(where $n = 0, 1, 2, 3, \dots$) - Phase difference ($\phi$):
\phi = 2n\pi - Maximum Intensity:
I_max = (\sqrt{I_1} + \sqrt{I_2})^2 \propto (a_1 + a_2)^2
- Path difference ($\Delta x$):
-
Destructive Interference (рд╡рд┐рдирд╛рд╢реА рд╡реНрдпрддрд┐рдХрд░рдг - Minimum Intensity):
- Path difference ($\Delta x$):
\Delta x = (2n - 1)\frac{\lambda}{2}(where $n = 1, 2, 3, \dots$) - Phase difference ($\phi$):
\phi = (2n - 1)\pi - Minimum Intensity:
I_min = (\sqrt{I_1} - \sqrt{I_2})^2 \propto (a_1 - a_2)^2
- Path difference ($\Delta x$):
### 3. Young's Double Slit Experiment (YDSE) (рдпрдВрдЧ рдХрд╛ рджреНрд╡рд┐-рд╕реНрд▓рд┐рдЯ рдкреНрд░рдпреЛрдЧ)
-
Fringe Width ($\beta$): The distance between two consecutive bright or dark fringes.
\beta = \frac{\lambda D}{d}- $\lambda$ = Wavelength of light (рдкреНрд░рдХрд╛рд╢ рдХреА рддрд░рдВрдЧрджреИрд░реНрдзреНрдп)
- $D$ = Distance between slits and screen (рд╕реНрд▓рд┐рдЯ рдФрд░ рдкрд░реНрджреЗ рдХреЗ рдмреАрдЪ рдХреА рджреВрд░реА)
- $d$ = Distance between the two slits (рджреЛрдиреЛрдВ рд╕реНрд▓рд┐рдЯреЛрдВ рдХреЗ рдмреАрдЪ рдХреА рджреВрд░реА)
-
Angular Fringe Width ($\theta$):
\theta = \frac{\beta}{D} = \frac{\lambda}{d} -
Position of $n$-th Bright Fringe:
x_n = \frac{n\lambda D}{d} -
Position of $n$-th Dark Fringe:
x_n' = (2n - 1)\frac{\lambda D}{2d} -
Effect of Medium: When the entire setup is immersed in a medium of refractive index $\mu$:
- New wavelength:
\lambda' = \frac{\lambda}{\mu} - New fringe width:
\beta' = \frac{\beta}{\mu}
- New wavelength:
### 4. Diffraction of Light (рдкреНрд░рдХрд╛рд╢ рдХрд╛ рд╡рд┐рд╡рд░реНрддрди)
The bending of light around the corners of an obstacle or aperture into the region of geometrical shadow is called diffraction.
-
Condition for Minima (Single Slit):
a \sin\theta = n\lambda(where $n = 1, 2, 3, \dots$)- $a$ = Width of the slit
-
Condition for Maxima:
a \sin\theta = (2n + 1)\frac{\lambda}{2}(where $n = 1, 2, 3, \dots$) -
Central Maximum Width:
- Linear Width:
\frac{2\lambda D}{a} - Angular Width:
\frac{2\lambda}{a}
- Linear Width:
### 5. Polarization of Light (рдкреНрд░рдХрд╛рд╢ рдХрд╛ рдзреНрд░реБрд╡рдг)
The phenomenon of restricting the vibrations of light waves into a single plane is called polarization. (Proves the transverse nature of light waves).
-
Malus's Law (рдорд╛рд▓рд╕ рдХрд╛ рдирд┐рдпрдо): When completely plane-polarized light is incident on an analyzer, the transmitted intensity $I$ is directly proportional to the square of the cosine of the angle ($\theta$) between the transmission axes of the polarizer and the analyzer.
I = I_0 \cos^2\theta(where $I_0$ is the initial intensity) -
Brewster's Law (рдмреНрд░реВрд╕реНрдЯрд░ рдХрд╛ рдирд┐рдпрдо): When unpolarized light is incident at a specific polarizing angle ($i_p$ or $i_B$) on a transparent surface, the reflected light is completely plane-polarized, and the reflected and refracted rays are perpendicular to each other.
\mu = \tan(i_p)- $\mu$ = Refractive index of the medium
- $i_p$ = Brewster's angle (рдзреНрд░реБрд╡рдг рдХреЛрдг)
### Important Constants & Relations for Quick Numericals
- Speed of light in vacuum:
c = 3 \times 10^8 \text{ m/s} - Relationship:
c = \nu\lambda(where $\nu$ is frequency) - Visible light wavelength range:
4000 \text{ \AA} \text{ to } 7000 \text{ \AA}($1 \text{ \AA} = 10^{-10} \text{ m}$)