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In Young's double-slit experiment lambda...

In Young's double-slit experiment `lambda = 500 nm, d = 1 mm`, and `D = 4 m`. The minimum distance from the central maximum for which the intensity is half of the maximum intensity is `'**' xx 10^(-4) m`. What is the value of `'**'`?

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To solve the problem, we will follow these steps: ### Step 1: Understand the problem We are given: - Wavelength, \( \lambda = 500 \, \text{nm} = 500 \times 10^{-9} \, \text{m} \) - Distance between the slits, \( d = 1 \, \text{mm} = 1 \times 10^{-3} \, \text{m} \) - Distance from the slits to the screen, \( D = 4 \, \text{m} \) We need to find the minimum distance \( x \) from the central maximum where the intensity is half of the maximum intensity. ### Step 2: Use the intensity formula In Young's double-slit experiment, the intensity \( I \) at a point on the screen is given by: \[ I = I_{\text{max}} \cos^2 \left( \frac{\phi}{2} \right) \] where \( \phi \) is the phase difference between the two waves arriving at that point. ### Step 3: Set up the condition for half intensity For the intensity to be half of the maximum intensity: \[ I = \frac{I_{\text{max}}}{2} \] This gives us: \[ \frac{I_{\text{max}}}{2} = I_{\text{max}} \cos^2 \left( \frac{\phi}{2} \right) \] Dividing both sides by \( I_{\text{max}} \): \[ \frac{1}{2} = \cos^2 \left( \frac{\phi}{2} \right) \] Taking the square root: \[ \cos \left( \frac{\phi}{2} \right) = \frac{1}{\sqrt{2}} \implies \frac{\phi}{2} = \frac{\pi}{4} \implies \phi = \frac{\pi}{2} \] ### Step 4: Relate phase difference to path difference The phase difference \( \phi \) is related to the path difference \( \Delta x \) by: \[ \phi = \frac{2\pi}{\lambda} \Delta x \] Setting \( \phi = \frac{\pi}{2} \): \[ \frac{\pi}{2} = \frac{2\pi}{\lambda} \Delta x \] Solving for \( \Delta x \): \[ \Delta x = \frac{\lambda}{4} \] ### Step 5: Express path difference in terms of \( x \) The path difference \( \Delta x \) for a point at distance \( x \) from the central maximum is given by: \[ \Delta x = \frac{xD}{d} \] Setting this equal to \( \frac{\lambda}{4} \): \[ \frac{xD}{d} = \frac{\lambda}{4} \] ### Step 6: Solve for \( x \) Rearranging gives: \[ x = \frac{\lambda d}{4D} \] Substituting the known values: \[ x = \frac{(500 \times 10^{-9} \, \text{m})(1 \times 10^{-3} \, \text{m})}{4(4 \, \text{m})} \] Calculating: \[ x = \frac{500 \times 10^{-12}}{16} = 31.25 \times 10^{-6} \, \text{m} = 3.125 \times 10^{-5} \, \text{m} \] ### Step 7: Convert to required format To express \( x \) in the form \( ** \times 10^{-4} \, \text{m} \): \[ 3.125 \times 10^{-5} \, \text{m} = 0.3125 \times 10^{-4} \, \text{m} \] Thus, the value of \( ** \) is approximately \( 3.125 \). ### Final Answer The value of \( ** \) is \( 3 \) (if rounded to the nearest whole number).

To solve the problem, we will follow these steps: ### Step 1: Understand the problem We are given: - Wavelength, \( \lambda = 500 \, \text{nm} = 500 \times 10^{-9} \, \text{m} \) - Distance between the slits, \( d = 1 \, \text{mm} = 1 \times 10^{-3} \, \text{m} \) - Distance from the slits to the screen, \( D = 4 \, \text{m} \) ...
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