In a double-slit experiment, when light of wavelength $\text{600 nm}$ is used, the central maximum and the second bright fringe are separated by $\text{3 mm}$ on a screen placed $\text{1.5 m}$ away. If the entire apparatus is then immersed in a liquid with a refractive index of $\text{1.5}$, what will be the angular separation between the first and fourth dark fringes?
$\text{0.1146}^\circ$
This problem involves analyzing a double-slit experiment. We are given information about the light's wavelength ($\lambda$), the positions of fringes like the central maximum and the second bright fringe, the distance to the screen (D), and the refractive index (n) of a liquid the setup is immersed in. The goal is to find the angular separation between the first and fourth dark fringes in the liquid.
In a double-slit experiment, the positions of the fringes are determined by the wavelength of light ($\lambda$), the distance between the slits (d), and the distance to the screen (D).
We will use these relationships to calculate the slit separation (d) from the initial conditions in air and then determine the required angular separation in the liquid.
First, we need to determine the distance between the two slits (d) using the experiment's initial setup in air.
Using the formula for the position of a bright fringe ($y_n = \frac{n \lambda_{air} D}{d}$), we can write for the second bright fringe (n=2):
$y_2 = \frac{2 \lambda_{air} D}{d}$
Rearranging the formula to solve for the slit separation (d):
$d = \frac{2 \lambda_{air} D}{y_2}$
Substituting the given values:
$d = \frac{2 \times (600 \times 10^{-9} \text{ m}) \times (1.5 \text{ m})}{3 \times 10^{-3} \text{ m}}$
$d = \frac{1800 \times 10^{-9}}{3 \times 10^{-3}} \text{ m}$
$d = 600 \times 10^{-6} \text{ m}$
Thus, the slit separation d is $600 \times 10^{-6}$ meters (or $0.6$ mm).
Next, we calculate the wavelength of the light when it travels through the liquid. The wavelength changes based on the medium's refractive index (n).
The relationship between the wavelength in air and the wavelength in the liquid ($\lambda_{liquid}$) is:
$\lambda_{liquid} = \frac{\lambda_{air}}{n}$
Substituting the values:
$\lambda_{liquid} = \frac{600 \text{ nm}}{1.5}$
$\lambda_{liquid} = \text{400 nm} = 400 \times 10^{-9}$ m
So, the effective wavelength of light inside the liquid is $\text{400 nm}$.
Now, we calculate the angular separation between the first and fourth dark fringes in the liquid. The angular position of the m-th dark fringe is given by $\theta'_m = \frac{(m + 1/2) \lambda_{liquid}}{d}$.
The angular position of the first dark fringe ($m=0$) is:
$\theta'_{0} = \frac{(0 + 1/2) \lambda_{liquid}}{d} = \frac{0.5 \lambda_{liquid}}{d}$
The angular position of the fourth dark fringe ($m=3$) is:
$\theta'_{3} = \frac{(3 + 1/2) \lambda_{liquid}}{d} = \frac{3.5 \lambda_{liquid}}{d}$
The required angular separation ($\Delta \theta$) is the difference between these two angular positions:
$\Delta \theta = \theta'_{3} - \theta'_{0} = \frac{3.5 \lambda_{liquid}}{d} - \frac{0.5 \lambda_{liquid}}{d}$
$\Delta \theta = \frac{(3.5 - 0.5) \lambda_{liquid}}{d} = \frac{3.0 \lambda_{liquid}}{d}$
Substitute the calculated values of $\lambda_{liquid}$ and d:
$\Delta \theta = \frac{3.0 \times (400 \times 10^{-9} \text{ m})}{600 \times 10^{-6} \text{ m}}$
$\Delta \theta = \frac{1200 \times 10^{-9}}{600 \times 10^{-6}}$
$\Delta \theta = 2 \times 10^{-3}$ radians
The calculated angular separation is in radians. We need to convert this to degrees to match the options provided.
The conversion formula is:
Angle in degrees = Angle in radians $\times \frac{180}{\pi}$
Performing the conversion:
$\Delta \theta (\text{degrees}) = (2 \times 10^{-3}) \times \frac{180}{\pi}$
$\Delta \theta (\text{degrees}) = \frac{0.36}{\pi}$
Using the approximate value of $\pi \approx 3.14159$:
$\Delta \theta (\text{degrees}) \approx \frac{0.36}{3.14159} \approx 0.11459^\circ$
Rounding to four decimal places, the angular separation between the first and fourth dark fringes in the liquid is approximately $\text{0.1146}^\circ$.
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