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The second order Bragg diffraction of X ...

The second order Bragg diffraction of `X` rays with `lambda=Å` form a set of parallel planes in a metal occurs at an angle `60^(@)`. the distance between the scattering planes in the crystal is

A

`0.575Å`

B

`1.00Å`

C

`2.00Å`

D

`1.15Å`

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The correct Answer is:
To find the distance between the scattering planes in the crystal using Bragg's law, we can follow these steps: ### Step 1: Write down Bragg's Law Bragg's law is given by the equation: \[ n\lambda = 2d \sin \theta \] where: - \( n \) is the order of diffraction, - \( \lambda \) is the wavelength of the X-rays, - \( d \) is the distance between the scattering planes, - \( \theta \) is the angle of diffraction. ### Step 2: Identify the values From the problem statement, we have: - \( \lambda = 1 \) Å (1 Angstrom = \( 1 \times 10^{-10} \) m), - \( \theta = 60^\circ \), - \( n = 2 \) (since it is second order diffraction). ### Step 3: Substitute the values into Bragg's Law Substituting the known values into the equation: \[ 2 \times 1 \text{ Å} = 2d \sin(60^\circ) \] ### Step 4: Calculate \( \sin(60^\circ) \) We know that: \[ \sin(60^\circ) = \frac{\sqrt{3}}{2} \] ### Step 5: Substitute \( \sin(60^\circ) \) into the equation Now substituting \( \sin(60^\circ) \) into the equation: \[ 2 \text{ Å} = 2d \left(\frac{\sqrt{3}}{2}\right) \] ### Step 6: Simplify the equation We can simplify the equation: \[ 2 \text{ Å} = d \sqrt{3} \] ### Step 7: Solve for \( d \) Now, solve for \( d \): \[ d = \frac{2 \text{ Å}}{\sqrt{3}} \] ### Step 8: Calculate the numerical value of \( d \) Calculating \( d \): \[ d \approx \frac{2}{1.732} \approx 1.1547 \text{ Å} \] ### Step 9: Round off the result Rounding off the result, we get: \[ d \approx 1.15 \text{ Å} \] ### Final Answer The distance between the scattering planes in the crystal is approximately \( 1.15 \) Å. ---

To find the distance between the scattering planes in the crystal using Bragg's law, we can follow these steps: ### Step 1: Write down Bragg's Law Bragg's law is given by the equation: \[ n\lambda = 2d \sin \theta \] where: - \( n \) is the order of diffraction, - \( \lambda \) is the wavelength of the X-rays, ...
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