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The longest wavelength that can be analy...

The longest wavelength that can be analysed by a sodium chloride crystal of spacing `d = 2.82 Å` in the second order is -

A

`2.82overset(@)A`

B

`5.64overset(@)A`

C

`8.46overset(@)A`

D

`11.28overset(@)A`

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The correct Answer is:
To find the longest wavelength that can be analyzed by a sodium chloride crystal with a spacing of \( d = 2.82 \, \text{Å} \) in the second order, we can use Bragg's Law, which is given by: \[ 2d \sin \theta = n \lambda \] Where: - \( d \) is the crystal spacing, - \( \theta \) is the angle of incidence, - \( n \) is the order of diffraction, - \( \lambda \) is the wavelength. ### Step 1: Rearranging Bragg's Law We need to find the wavelength \( \lambda \). Rearranging the equation gives: \[ \lambda = \frac{2d \sin \theta}{n} \] ### Step 2: Maximizing Wavelength To find the longest wavelength, we need to maximize \( \lambda \). The maximum value of \( \sin \theta \) is 1 (which occurs at \( \theta = 90^\circ \)). Therefore, we can write: \[ \lambda_{\text{max}} = \frac{2d}{n} \] ### Step 3: Substituting Values We know: - \( d = 2.82 \, \text{Å} = 2.82 \times 10^{-10} \, \text{m} \) (since \( 1 \, \text{Å} = 10^{-10} \, \text{m} \)) - \( n = 2 \) (since we are looking for the second order) Substituting these values into the equation gives: \[ \lambda_{\text{max}} = \frac{2 \times (2.82 \times 10^{-10} \, \text{m})}{2} \] ### Step 4: Simplifying the Expression The 2's in the numerator and denominator cancel out: \[ \lambda_{\text{max}} = 2.82 \times 10^{-10} \, \text{m} \] ### Step 5: Converting to Angstroms Since \( 1 \, \text{Å} = 10^{-10} \, \text{m} \), we can express the wavelength in angstroms: \[ \lambda_{\text{max}} = 2.82 \, \text{Å} \] ### Final Answer Thus, the longest wavelength that can be analyzed by the sodium chloride crystal in the second order is: \[ \lambda_{\text{max}} = 2.82 \, \text{Å} \]

To find the longest wavelength that can be analyzed by a sodium chloride crystal with a spacing of \( d = 2.82 \, \text{Å} \) in the second order, we can use Bragg's Law, which is given by: \[ 2d \sin \theta = n \lambda \] Where: - \( d \) is the crystal spacing, ...
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