Nuclear Macroscopic cross-section

In summary, the nuclear macroscopic cross-section is a measure of the probability of a nuclear interaction occurring within a given material. It combines the microscopic cross-section, which describes the likelihood of interactions at the atomic level, with the number density of target nuclei. The macroscopic cross-section is essential for understanding and calculating interactions such as absorption, scattering, and fission in nuclear physics and engineering applications. It is typically expressed in units of area per unit volume and plays a critical role in reactor design, radiation shielding, and nuclear safety analysis.
  • #1
badvot
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Homework Statement
Calculate the macroscopic cross section using volume fractions
Relevant Equations
Macroscopic nuclear cross section
This question is in the book " Introduction to nuclear engineering by Lamarsh" Chapter3:
Screenshot 2024-05-03 210913.png

I think it's pretty basic but I couldn't find the proper way to prove it, and now I even suspect that it's not a correct question.
My attempt solution:


Screenshot 2024-05-03 211748.png


I would very much appreciate your help. Thanks in advance.
 
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  • #2
You need to distinguish between the number density ##N_i^{(mix)}## of constituent ##i## in the mixture and the number density ##N_i^{(norm)}## of constituent ##i## at its normal density.

How is ##N_i^{(mix)}## related to ##N_i^{(norm)}## and ##f_i##?

You are asked to show, $$\Sigma_a^{(mix)} = f_1 \Sigma_{a1}^{(norm)} + f_2 \Sigma_{a2}^{(norm)} + ...$$
 
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  • #3
Thank you so much. I think I get it now, and here is my understanding:
If we assume two species (x,y)
$$\Sigma_{mix}= \frac{No\ of\ X\ atoms}{Volume\ of\ X} \times \frac{Volume\ of\ X}{Volume\ of\ X+Y} + \frac{No\ of\ Y\ atoms}{Volume\ of\ Y} \times \frac{Volume\ of\ Y}{Volume\ of\ X+Y}$$
 
  • #4
badvot said:
Thank you so much. I think I get it now, and here is my understanding:
If we assume two species (x,y)
$$\Sigma_{mix}= \frac{No\ of\ X\ atoms}{Volume\ of\ X} \times \frac{Volume\ of\ X}{Volume\ of\ X+Y} + \frac{No\ of\ Y\ atoms}{Volume\ of\ Y} \times \frac{Volume\ of\ Y}{Volume\ of\ X+Y}$$
The left side of your equation, ##\Sigma_{mix}##, is the macroscopic absorption cross-section of the mixture. This has the dimension of inverse length. However, the right side of your equation has the dimension of inverse volume.

Also, you would expect ##\Sigma_{mix}## to depend on the microscopic absorption cross-sections ##\sigma_{a1}## and ##\sigma_{a2}## of the two species. However, these do not appear on the right side.
 
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  • #5
Oh, I guess I was so enthusiastic to write the answer that I forgot to include the microscopic cross-section for each species :oldbiggrin:
$$\Sigma_{mix}= \frac{No\ of\ X\ atoms}{Volume\ of\ X} \times
\frac{Volume\ of\ X}{Volume\ of\ X+Y} \times \sigma_{X} + \frac{No\ of\ Y\ atoms}{Volume\ of\ Y} \times \frac{Volume\ of\ Y}{Volume\ of\ X+Y} \times \sigma_{Y}$$
The volume fractions are those below, while the rest of the terms ##\sigma \times \frac{No\ of\ atoms}{Volume}## equal the ##\Sigma_{a}^{(norm)}## for each species
$$\frac{Volume\ of\ X}{Volume\ of\ X+Y} =F_{X}$$
$$\frac{Volume\ of\ Y}{Volume\ of\ X+Y} =F_{Y}$$
The units check out
$$cm^{-1}= \frac{\#}{cm^{3}} \times \frac{cm^{3}}{cm^{3}} \times cm^{2} + \frac{\#}{cm^{3}} \times \frac{cm^{3}}{cm^{3}} \times cm^{2} $$
 
  • #6
OK. That looks good.
 
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FAQ: Nuclear Macroscopic cross-section

What is a nuclear macroscopic cross-section?

The nuclear macroscopic cross-section is a measure of the probability of a nuclear interaction occurring within a material, expressed in terms of area. It is defined as the product of the microscopic cross-section of a specific nuclear reaction and the number density of target nuclei in the material. The macroscopic cross-section is crucial for understanding how materials interact with radiation.

How is the macroscopic cross-section calculated?

The macroscopic cross-section (Σ) can be calculated using the formula Σ = Nσ, where N is the number density of target nuclei (number of nuclei per unit volume) and σ is the microscopic cross-section (the effective area for a specific interaction). The units of the macroscopic cross-section are typically given in cm-1.

What are the different types of macroscopic cross-sections?

There are several types of macroscopic cross-sections, including total cross-section (ΣT), absorption cross-section (ΣA), scattering cross-section (ΣS), and fission cross-section (ΣF). Each type corresponds to different nuclear interactions and helps describe how a material interacts with neutrons or other particles.

Why is the macroscopic cross-section important in nuclear engineering?

The macroscopic cross-section is essential in nuclear engineering as it helps predict how radiation interacts with materials, which is critical for reactor design, radiation shielding, and safety analysis. It allows engineers to calculate neutron flux, absorption rates, and overall material behavior in nuclear systems.

How does temperature affect the macroscopic cross-section?

Temperature can affect the macroscopic cross-section by influencing the number density of nuclei and the microscopic cross-section through changes in material properties, such as density and atomic vibrations. Higher temperatures may lead to increased atomic motion, which can alter the likelihood of nuclear interactions, thus changing the effective macroscopic cross-section.

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