An x-ray beam of wavelength 0.97A0 is obtained in the third-order afte...
To solve this problem, we need to use the Bragg's law, which relates the angle of incidence, the angle of reflection, and the wavelength of the x-ray beam. The equation is given by:
nλ = 2d sinθ
where n is the order of reflection, λ is the wavelength of the x-ray beam, d is the spacing between the crystal planes, and θ is the angle of incidence/reflection.
Let's calculate the wavelength of the x-ray beam in the first order after reflection at 300 from the crystal:
n = 1
θ = 300
We need to find the spacing between the crystal planes (d) to calculate the wavelength. Rearranging the equation, we have:
λ = 2d sinθ / n
Substituting the values, we get:
λ = 2d sin(300) / 1
Now, let's calculate the wavelength of the x-ray beam in the third order after reflection at 600 from the crystal:
n = 3
θ = 600
Using the same equation, we have:
λ = 2d sin(600) / 3
Now, we have two equations with two unknowns (d and λ) and we can solve them simultaneously.
Now, let's solve the two equations simultaneously:
2d sin(300) = λ
2d sin(600) = 3λ
Dividing the two equations, we have:
sin(300) / sin(600) = λ / (3λ)
sin(300) / sin(600) = 1/3
Using the values of sin(300) = 0.5 and sin(600) = 0.866, we can solve for λ:
0.5 / 0.866 = 1/3
λ = 1.732A0
Therefore, the wavelength of the second x-ray beam is 1.732A0, which is approximately equal to 1.68A0.
An x-ray beam of wavelength 0.97A0 is obtained in the third-order afte...