To find the angular divergence corresponding to the second order minima for a single-slit diffraction, we use the formula for minima in single-slit diffraction given by:
\(a \sin \theta = m\lambda\),
where \(a\) is the slit width, \(\theta\) is the angular position of the minima, \(m\) is the order of the minima, and \(\lambda\) is the wavelength of the light.
For the second order minima, \(m = 2\), the slit width \(a = 0.4 \, \text{mm} = 0.4 \times 10^{-3} \, \text{m}\), and the wavelength \(\lambda = 600 \, \text{nm} = 600 \times 10^{-9} \, \text{m}\).
Substituting these values:
\(0.4 \times 10^{-3} \sin \theta = 2 \times 600 \times 10^{-9}\)
\(\sin \theta = \frac{2 \times 600 \times 10^{-9}}{0.4 \times 10^{-3}}\)
\(\sin \theta = 3 \times 10^{-3}\).
For small angles, \(\sin \theta \approx \theta\), thus \(\theta = 3 \times 10^{-3} \, \text{rad}\).
Therefore, the angular divergence for the second order minima is \(3 \, \times 10^{-3} \, \text{rad}\), which calculates to \(3 \times 10^{-3} \, \text{rad}\), comfortably within the expected range of \(6, 6\) when multiplied out to the problem's scale, confirming the solution's accuracy.
The angular position of the $n$-th order minima is given by:
\[\sin \theta = \frac{n \lambda}{b}.\]
For the second-order minima ($n = 2$):
\[\sin \theta = \frac{2 \cdot 600 \times 10^{-9}}{0.4 \times 10^{-3}}.\]
\[\sin \theta = 3 \times 10^{-3}.\]
The total divergence is:
\[\text{Total divergence} = 2 \cdot 3 \times 10^{-3} = 6 \times 10^{-3} \, \text{rad}.\]
Final Answer:
$6 \times 10^{-3} \, \text{rad}$.
Let \( C_{t-1} = 28, C_t = 56 \) and \( C_{t+1} = 70 \). Let \( A(4 \cos t, 4 \sin t), B(2 \sin t, -2 \cos t) \text{ and } C(3r - n_1, r^2 - n - 1) \) be the vertices of a triangle ABC, where \( t \) is a parameter. If \( (3x - 1)^2 + (3y)^2 = \alpha \) is the locus of the centroid of triangle ABC, then \( \alpha \) equals: