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Let S1 and S2 be the two slits in Young'...

Let `S_1 and S_2` be the two slits in Young's double slit experiment. If central maxima is observed at P and angle `S_1 P S_2 = theta`, (`theta` is small) find the y-coordinates of the 3rd minima assuming the origin at the central maxima. (`lambda` = wavelength of monochromatic light used).`

A

`+-(2lambda)/theta`

B

`+-(5lambda)/(2 theta)`

C

`+- 5/2 lambda theta`

D

`+-2 lambda theta `

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To find the y-coordinate of the third minima in Young's double slit experiment, we can follow these steps: ### Step 1: Understand the condition for minima In Young's double slit experiment, minima occur when the path difference between the light coming from the two slits is an odd multiple of half the wavelength, i.e., \[ \Delta d = \left(m + \frac{1}{2}\right) \lambda \] where \( m \) is an integer (0, 1, 2, ...). For the third minima, \( m = 2 \): \[ \Delta d = \left(2 + \frac{1}{2}\right) \lambda = \frac{5}{2} \lambda \] ### Step 2: Relate path difference to geometry The path difference \( \Delta d \) can also be expressed in terms of the angle \( \theta \) and the distance between the slits \( d \): \[ \Delta d = d \sin(\theta) \] For small angles, we can use the approximation \( \sin(\theta) \approx \theta \) (in radians). Thus, we have: \[ \Delta d \approx d \theta \] ### Step 3: Set up the equation for the third minima From the previous steps, we can equate the two expressions for the path difference: \[ d \theta = \frac{5}{2} \lambda \] ### Step 4: Solve for \( \theta \) Rearranging the equation gives: \[ \theta = \frac{5 \lambda}{2d} \] ### Step 5: Find the y-coordinate In the geometry of the setup, the y-coordinate of the minima can be expressed as: \[ y = D \tan(\theta) \] For small angles, \( \tan(\theta) \approx \theta \). Thus, \[ y \approx D \theta \] Substituting the expression for \( \theta \): \[ y \approx D \left(\frac{5 \lambda}{2d}\right) \] This gives: \[ y = \frac{5D \lambda}{2d} \] ### Step 6: Consider both directions for minima Since minima can occur above and below the central maxima, the y-coordinates for the third minima are: \[ y = \pm \frac{5D \lambda}{2d} \] ### Final Result The y-coordinates of the third minima are: \[ y = \frac{5D \lambda}{2d} \quad \text{and} \quad y = -\frac{5D \lambda}{2d} \]

To find the y-coordinate of the third minima in Young's double slit experiment, we can follow these steps: ### Step 1: Understand the condition for minima In Young's double slit experiment, minima occur when the path difference between the light coming from the two slits is an odd multiple of half the wavelength, i.e., \[ \Delta d = \left(m + \frac{1}{2}\right) \lambda \] where \( m \) is an integer (0, 1, 2, ...). For the third minima, \( m = 2 \): ...
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