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Visible light of wavelenght 8000 xx 1...

Visible light of wavelenght `8000 xx 10^(-8)` cm falls normally on a single slit and produces a diffraction pattern. It is found that the Third diffraction minimum is at `45^(@)` from the central maximum. If the first minimum is produced at `theta_(1)` then `theta_(1) ` is close to :

A

`40^(@)`

B

`35^(@)`

C

`30^(@)`

D

`15^(@)`

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The correct Answer is:
To solve the problem, we need to find the angle \( \theta_1 \) at which the first diffraction minimum occurs, given that the third diffraction minimum is at \( 45^\circ \). ### Step-by-Step Solution: 1. **Understanding the Diffraction Condition**: The condition for the minima in a single-slit diffraction pattern is given by the formula: \[ n \lambda = d \sin \theta \] where \( n \) is the order of the minimum, \( \lambda \) is the wavelength of the light, \( d \) is the width of the slit, and \( \theta \) is the angle at which the minimum occurs. 2. **Given Values**: - Wavelength \( \lambda = 8000 \times 10^{-8} \) cm. - The angle for the third minimum \( \theta_3 = 45^\circ \). - For the third minimum, \( n = 3 \). 3. **Finding the Slit Width \( d \)**: Using the formula for the third minimum: \[ 3 \lambda = d \sin(45^\circ) \] Since \( \sin(45^\circ) = \frac{\sqrt{2}}{2} \), we can rewrite the equation as: \[ d = \frac{3 \lambda}{\sin(45^\circ)} = \frac{3 \lambda}{\frac{\sqrt{2}}{2}} = 3 \sqrt{2} \lambda \] 4. **Substituting the Wavelength**: Now substituting the value of \( \lambda \): \[ d = 3 \sqrt{2} \times 8000 \times 10^{-8} \text{ cm} \] 5. **Finding the First Minimum**: For the first minimum (\( n = 1 \)), we use the same formula: \[ \lambda = d \sin(\theta_1) \] Substituting the value of \( d \): \[ \lambda = (3 \sqrt{2} \lambda) \sin(\theta_1) \] Dividing both sides by \( \lambda \) (assuming \( \lambda \neq 0 \)): \[ 1 = 3 \sqrt{2} \sin(\theta_1) \] Rearranging gives: \[ \sin(\theta_1) = \frac{1}{3 \sqrt{2}} \] 6. **Calculating \( \theta_1 \)**: Now we find \( \theta_1 \): \[ \theta_1 = \sin^{-1}\left(\frac{1}{3 \sqrt{2}}\right) \] 7. **Approximating \( \theta_1 \)**: Using a calculator or trigonometric tables, we can find: \[ \theta_1 \approx 15^\circ \] ### Final Answer: Thus, \( \theta_1 \) is approximately \( 15^\circ \).

To solve the problem, we need to find the angle \( \theta_1 \) at which the first diffraction minimum occurs, given that the third diffraction minimum is at \( 45^\circ \). ### Step-by-Step Solution: 1. **Understanding the Diffraction Condition**: The condition for the minima in a single-slit diffraction pattern is given by the formula: \[ n \lambda = d \sin \theta ...
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