In Young's double-slit experiment, the intensity ($I$) of light at a point on the screen depends on the phase difference ($\phi$) between the waves from the two slits. The intensity is given by the formula:
$I = I_{max} \cos^2\left(\frac{\phi}{2}\right)$
where $I_{max}$ is the maximum intensity.
The phase difference ($\phi$) is related to the path difference ($\Delta x$) by:
$\phi = \frac{2\pi}{\lambda} \Delta x$
Given:
Calculate the phase difference:
$\phi_1 = \frac{2\pi}{\lambda} (\lambda) = 2\pi$
Now, calculate the intensity:
$I_1 = I_{max} \cos^2\left(\frac{2\pi}{2}\right) = I_{max} \cos^2(\pi) = I_{max} (-1)^2 = I_{max}$
Therefore, $K = I_{max}$.
Given:
Calculate the phase difference:
$\phi_2 = \frac{2\pi}{\lambda} \left(\frac{\lambda}{3}\right) = \frac{2\pi}{3}$
Calculate the intensity ($I_2$):
$I_2 = I_{max} \cos^2\left(\frac{\phi_2}{2}\right) = I_{max} \cos^2\left(\frac{2\pi/3}{2}\right) = I_{max} \cos^2\left(\frac{\pi}{3}\right)$
We know that $\cos(\pi/3) = 1/2$. Substituting this value:
$I_2 = I_{max} \left(\frac{1}{2}\right)^2 = I_{max} \left(\frac{1}{4}\right) = \frac{I_{max}}{4}$
Since $K = I_{max}$, the intensity $I_2$ is:
$I_2 = \frac{K}{4}$
The intensity of light at a point where the path difference is $\lambda/3$ will be $K/4$. This corresponds to Option C.
A ray of monochromatic light is passing through an equilateral prism (ABC) as shown in the figure. The refracted ray (QR) is parallel to the base (BC) and the angle of incidence ($i$) is $50^\circ$. Then the angle of deviation ($\delta$) is :
The lens combination as shown in the figure, consists of two lenses, $L_1$ and $L_2$, of the focal lengths $+10\text{ cm}$ and $-10\text{ cm}$, respectively. The position of the image formed is :
Consider three media P, Q and R with refractive indices $1$, $1.25$, and $1.5$, respectively. The medium Q having a thickness of $5\text{ cm}$ is placed between extended media P and R as shown in the figure. An object O is placed at the center of medium Q. If viewed from medium P near the normal direction, the apparent depth of O is $h_1$. For similar observation from medium R, the apparent depth is $h_2$. The value of $|h_1 - h_2|$, in cm, is :