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    Nuclear Reactionsand Radiation

    3.4 Getting ready to calculate a

    reaction rate but you gotta get

    the flux

    L. R. Foulke

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    SUMMARY - MICROSCOPIC

    CROSS SECTIONS MICROSCOPIC ()

    Measure of Equivalent Nucleus "TargetSize

    Multiplied with Atom Density (N) to YieldMacroscopic Cross Section ()

    =N

    Note: for this lecture, we will try to reserve capital N for numberdensity of a nuclide, and lower case n for neutron density.

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    Microscopic Cross Section So far we have only considered the probability that

    any type of reaction will occur:

    This is referred to as the Total Microscopic CrossSection, t

    We can also consider the probability that a specifictype of reaction will occur:

    Microscopic Scattering Cross Section,s

    Microscopic Absorption Cross Section, a Microscopic Capture (n,) Cross Section, c Microscopic Fission Cross Section, f

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    Cross Section Hierarchy

    t=

    a+

    s

    a=c+f

    s=

    e+

    i

    Micros on eachlevel are the sum

    of all constituent

    micros on lower

    levels.

    Image Source: See Note 1

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    Macroscopic Cross Sections Microscopic cross sections give us information about

    the probability of interaction on a per nucleus basis

    What if we want to know the probability of an interaction in amaterial with a known density.

    In this case we need to multiply the probability of interactingwith a single nucleus by the number (density) of nuclei in the

    material.

    The quantity is called the macroscopic crosssection, it has units of 1/cm.

    t= N

    tUnits: [nuclei/cm3] x [cm2/nucleus]

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    Macroscopic Cross Sections The macroscopic cross section gives the probability

    that a neutron will undergo a reaction per distance

    travelled (1/cm).

    Since microscopic cross sections are energy dependentit follows that macroscopic cross sections are as well.

    Macroscopic cross sections for individual reaction typescan be calculated from the corresponding microscopiccross sections.

    a= N

    a

    s= N

    s f = N f

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    Calculating Number Density Calculating macroscopic cross sections requirescalculation of the number density of nuclei in a

    material.

    This information can be calculated using Avogadro'snumber.Avogadros NumberNA= 6.02210

    23 atoms/mole

    Atomic mass of atom in amu = Mass [g] per mole of atoms

    Units: [atoms/cm3] = [g/cm3] [atoms/mole] [mole/g]

    N = NA/A N= Atomic number density = Material densityNA = Avogadros Number

    A = Atomic mass

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    SUMMARY - MACROSCOPIC

    CROSS SECTIONS MACROSCOPIC ()

    Product of Microscopic Cross Section andAtom Density

    Multiplied with Neutron Flux () to Yield aReaction Rate (R)

    R =

    R = (cm1)(neutrons / cm2 sec) = reactions / cm3 sec

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    Reaction Rates Neutron radiation levels are usually measured in termsofneutron flux, denoted

    Neutron flux is the rate at which neutrons pass through a spatialposition, per unit time.

    Units: [neutrons / cm2 / sec] The rate of neutron interactions (per unit volume) in a

    material is given by:

    The rate of individual reactions can be calculated by substitutingthe reaction cross section for the total cross section.

    R = t

    Units: [neutrons/cm2/sec][reactions/cm]

    = [reactions/cm3/sec]

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    Neutrons at t = 0Neutrons at t = t

    Total distance traveled by all neutrons during t= Total path length generated by all neutrons during t

    What is Neutron Flux?

    Image Source: See Note 2

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    Neutrons at t = 0Neutrons at t = t

    Total distance traveled by all neutrons during t= Total path length generated by all neutrons during t

    What is Neutron Flux?

    Image Source: See Note 2

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    Neutron Fluxes

    Image Source: See Note 1

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    Reaction Rate:

    Reaction Rate Density (Energy Integrated)Rate at which neutrons at position , all

    energies, undergo a reaction of typex.

    This reaction rate density is what must becalculated to design a reactor; it governs where thefission energy is deposited.

    Rx

    r,t( ) = x

    r,t( )

    r,t( )

    r

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    Neutron Attenuation

    Image Source: See Note 1

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    NEUTRON BEAM ATTENUATION

    NEUTRON BEAM INTERACTION (x) = (x) x

    d(x) = (x) dxd(x)

    dx= (x)

    (x) = (0) e x

    (x)

    0

    = e x

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    1) Adapted with permission from the AmericanNuclear Society. Nuclear Engineering

    Theory and Technology of CommercialNuclear Powerby Ronald Allen Knief, 2ndEdition. Copyright 2008 by the AmericanNuclear Society, La Grange Park, Illinois.

    Figure 2-10 (slide 4), 4-1 (slide 12), and 2-14(slide 14).

    2) Reprinted with permission from DavidGriesheimer, University of Pittsburgh.

    Image Source Notes