Physics, asked by paingomaima, 11 hours ago

Problem 4 a) An incident 71 pm X-ray is incident on a calcite target. i. Find the wavelength of the X-ray scattered at a 30° angle, ii. What is the largest shift that can be expected in this experiment? b) X-rays of wavelength 10.0 pm are scattered from a target. i. Find the wavelength of x-rays scattered through 45° ii. Find the maximum wavelength present in the scattered x-rays. iii. Find the maximum kinetic energy of the recoil electrons, c) At what scattering angle will incident 100 keV x-rays leave a target with an energy of 90 keV.​

Answers

Answered by tangledfrozen195
8

Answer:

Hi paingomaima. I hope this answer would help you

Compton shift is given as Δλ=

mc

h

(1−cosϕ)=

9.1×10

−31

Kg×3×10

8

m/s

6.62×10

−34

Js

(1−cos85

0

)

where m is the mass of electron and h is Planck's constant with c as speed of light in air.

On calculation we get the shift as Δλ=2.2×10

−12

meter=2.2picometer

Answered by ishwaryam062001
0

Answer:

Explanation:

From the above question,

They have given :

a) i. The wavelength of the X-ray scattered at a 30° attitude can be observed the use of the Bragg equation:

                        2d sin θ = nλ

For calcite, d = 2.71 Å. Converting the incident wavelength to Å,

we have:

            λ = 0.071 nm

               = 0.71 Å

Substituting these values into the Bragg equation, we get:

                        2(2.71 Å) sin 30° = 1λ

                        λ = 1.24 Å

Therefore, the wavelength of the X-ray scattered at a 30° attitude is 1.24 Å.

ii. The greatest shift that can be anticipated in this scan is given through the Compton shift:

                        Δλ = λ(1 - cosθ)

where λ is the incident wavelength and θ is the scattering angle.

Substituting the values we have:

                        Δλ = 0.71 Å (1 - cos 30°)

                        Δλ = 0.118 Å

Therefore, the greatest shift that can be anticipated in this test is 0.118 Å.

b) i. The wavelength of x-rays scattered via 45° can additionally be determined the use of the Bragg equation, assuming that the goal cloth has atomic planes separated with the aid of d = λ/2:

                        2d sin θ = nλ

Substituting the given values:

                        2(λ/2) sin 45° = 1λ'

                        λ' = λ/√2

                        λ' = 7.07 pm

Therefore, the wavelength of x-rays scattered thru 45° is 7.07 pm.

ii. The most wavelength current in the scattered x-rays is given via the Compton shift:

                        Δλ = λ(1 - cosθ)

Substituting the given values:

                        Δλ = 10.0 pm (1 - cos 180°)

                        Δλ = 20.0 pm

Therefore, the most wavelength existing in the scattered x-rays is 20.0 pm.

iii. The most kinetic strength of the shy away electrons is given via the Compton formula:

                        E = h(c/λ - c/λ')

where h is Planck's constant, c is the pace of light, λ is the incident wavelength, and λ' is the scattered wavelength.

Substituting the given values:

                        E = h(c/10.0 pm - c/20.0 pm)

                        E = 1.24 keV

Therefore, the most kinetic power of the pull away electrons is 1.24 keV.

c) The electricity of the scattered X-rays is given by:

                        E' = E/(1 + E/mc^2*(1-cosθ))

where E is the incident energy, m is the relaxation mass of the electron, and c is the velocity of light.

Substituting the given values:

                        E = one hundred keV

                        E' = ninety keV

                        θ = ?

Solving for θ, we get:

                        cos θ = 1 - (mc^2(E - E'))/(E'E + mc^2*E')

                        cos θ = 0.954

                        θ = 18.26°

Therefore, the scattering attitude is about 18.26°.

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