The angular separation for the minima in a single-slit diffraction is given by: \[ \theta_1 = \sin^{-1}\left( \frac{2\lambda}{a} \right), \quad \theta_2 = \sin^{-1}\left( \frac{3\lambda}{a} \right) \] where \( \lambda = 628 \, \text{nm} \) is the wavelength and \( a \) is the slit width. Also, we know: \[ \theta_1 + \theta_2 = 30^\circ \] \[ \Rightarrow \sin^{-1}\left( \frac{2\lambda}{a} \right) + \sin^{-1}\left( \frac{3\lambda}{a} \right) = \frac{\pi}{6} \] Solving this, we find: \[ a = 6.07 \, \mu m \] Thus, the width of the slit is \( a = 6 \, \mu m \).
We are asked to find the width of the slit in a single-slit diffraction experiment. We are given the wavelength of light used and the angular separation between the second minimum on the left and the third minimum on the right of the central maximum.
In a single-slit diffraction pattern, the condition for the \( n^{th} \) intensity minimum is given by the formula:
\[ a \sin(\theta_n) = n\lambda \]
where \( a \) is the width of the slit, \( \theta_n \) is the angular position of the \( n^{th} \) minimum from the central maximum, \( \lambda \) is the wavelength of the light, and \( n \) is a non-zero integer (\( n = \pm 1, \pm 2, \pm 3, \ldots \)).
For small angles, we can use the approximation \( \sin(\theta) \approx \theta \), where \( \theta \) is in radians. So the formula becomes:
\[ a \theta_n \approx n\lambda \quad \implies \quad \theta_n \approx \frac{n\lambda}{a} \]
Step 1: List the given values and convert them to appropriate SI units.
We need to convert the angular separation to radians for use in the small-angle approximation formula:
\[ \Delta\theta = 30^\circ = 30 \times \frac{\pi}{180} \, \text{radians} = \frac{\pi}{6} \, \text{radians} \]
Step 2: Determine the angular positions of the specified minima.
Let \( \theta_2 \) be the angular position of the second minimum to the left of the central maximum (\( n=2 \)). Using the small angle approximation:
\[ \theta_2 \approx \frac{2\lambda}{a} \]
Let \( \theta_3 \) be the angular position of the third minimum to the right of the central maximum (\( n=3 \)). Using the small angle approximation:
\[ \theta_3 \approx \frac{3\lambda}{a} \]
Step 3: Relate the individual angular positions to the total angular separation.
The total angular separation \( \Delta\theta \) between the second minimum on the left and the third minimum on the right is the sum of their individual angular positions from the center.
\[ \Delta\theta = \theta_2 + \theta_3 \]
Step 4: Substitute the expressions for \( \theta_2 \) and \( \theta_3 \) and solve for the slit width \( a \).
\[ \Delta\theta \approx \frac{2\lambda}{a} + \frac{3\lambda}{a} = \frac{5\lambda}{a} \]
Rearranging the formula to solve for \( a \):
\[ a \approx \frac{5\lambda}{\Delta\theta} \]
Step 5: Substitute the numerical values and calculate the slit width.
We have \( \lambda = 628 \times 10^{-9} \, \text{m} \) and \( \Delta\theta = \frac{\pi}{6} \, \text{rad} \). Note that \( 628 \approx 200 \times \pi \).
\[ a = \frac{5 \times (628 \times 10^{-9} \, \text{m})}{\frac{\pi}{6}} \] \[ a = \frac{30 \times (628 \times 10^{-9} \, \text{m})}{\pi} \]
Using the approximation \( 628 \approx 200\pi \):
\[ a \approx \frac{30 \times (200\pi \times 10^{-9} \, \text{m})}{\pi} = 6000 \times 10^{-9} \, \text{m} \] \[ a = 6 \times 10^{-6} \, \text{m} \]
Step 6: Express the final answer in micrometers.
Since \( 1 \, \mu\text{m} = 10^{-6} \, \text{m} \), the slit width is:
\[ a = 6 \, \mu\text{m} \]
The width of the slit is 6 \( \mu \)m.
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Two blocks of masses \( m \) and \( M \), \( (M > m) \), are placed on a frictionless table as shown in figure. A massless spring with spring constant \( k \) is attached with the lower block. If the system is slightly displaced and released then \( \mu = \) coefficient of friction between the two blocks.
(A) The time period of small oscillation of the two blocks is \( T = 2\pi \sqrt{\dfrac{(m + M)}{k}} \)
(B) The acceleration of the blocks is \( a = \dfrac{kx}{M + m} \)
(\( x = \) displacement of the blocks from the mean position)
(C) The magnitude of the frictional force on the upper block is \( \dfrac{m\mu |x|}{M + m} \)
(D) The maximum amplitude of the upper block, if it does not slip, is \( \dfrac{\mu (M + m) g}{k} \)
(E) Maximum frictional force can be \( \mu (M + m) g \)
Choose the correct answer from the options given below:
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: