
In a double slit experiment, the condition for a dark fringe can be stated as:
d sin θ = (m + 0.5)λ.
Given that the dark fringe is observed at point P, we can approximate sin θ ≈ θ ≈ x/D, where x is the distance of the fringe from the center, and D is the distance to the screen.
Using the given data:
Wavelength λ = 400 nm = 400 × 10-9 m,
Distance D = 0.2 m.
The first dark fringe corresponds to m = 0, so:
d(0) + 0.5(400 × 10-9) = d.
Since x is approximately D:
d = λ/2.
Calculating:
d = (400 × 10-9)/2 = 200 × 10-9 m = 0.2 mm.
The minimum distance between the slits is 0.2 mm, which falls within the range [0.2, 0.2] mm.
Step1. Path Difference Condition for Minima: - For a dark fringe (minima) at P, the path difference should be:
\[ 2\sqrt{D^2 + d^2} - 2D = \frac{\lambda}{2} \]
- Rearrange:
\[ \sqrt{D^2 + d^2} - D = \frac{\lambda}{4} \]
- Therefore:
\[ \sqrt{D^2 + d^2} = D + \frac{\lambda}{4} \]
Step 2. Square Both Sides:
\[ D^2 + d^2 = D^2 + D\lambda + \frac{\lambda^2}{16} \]
- Simplify to solve for d:
\[ d^2 = D\lambda + \frac{\lambda^2}{16} \]
Step 3. Substitute Given Values: - \(\lambda = 400 \, \text{nm} = 400 \times 10^{-9} \, \text{m}\), \(D = 0.2 \, \text{m}\)
\[ d^2 = 0.2 \times 400 \times 10^{-9} + \frac{(400 \times 10^{-9})^2}{16} \]
- Calculate:
\[ d^2 \approx 4 \times 10^{-8} \, \text{m}^2 \]
\[ d \approx 2 \times 10^{-4} \, \text{m} = 0.20 \, \text{mm} \]
So, the correct answer is: \(d = 0.20 \, \text{mm}\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)