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Page Title: Cross Sections
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Atom Density
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Nuclear Physics and Reactor Theory Volume 1 of 2
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Cross Sections

N NA M 2.699 g cm3 6.022  x  1023atoms mole 26.9815 g mole 6.024  x  1022atoms cm3 DOE-HDBK-1019/1-93 Reactor Theory (Neutron Characteristics) NUCLEAR CROSS SECTIONS AND NEUTRON FLUX Rev. 0 Page 7 NP-02 Example: A  block  of  aluminum  has  a  density  of  2.699  g/cm  .    If  the  gram  atomic  weight  of 3 aluminum is 26.9815 g, calculate the atom density of the aluminum. Solution: Cross Sections The probability of a neutron interacting with a nucleus for a particular reaction is dependent upon not only  the kind of nucleus involved, but also the energy of the neutron.  Accordingly, the absorption of a thermal neutron in most materials is much more probable than the absorption of  a  fast neutron.  Also, the probability of interaction will vary depending upon the type of reaction involved. The probability of a particular reaction occurring between a neutron and a nucleus is called the microscopic cross section (   ) of the nucleus for the particular reaction.  This cross section will vary with the energy of the neutron.  The microscopic cross section may also be regarded as the effective area the nucleus presents to the neutron for the particular reaction.  The larger the effective area, the greater the probability for reaction. Because  the microscopic cross section is an area, it is expressed in units of area, or square centimeters.  A square centimeter is tremendously large in comparison to the effective area of a nucleus, and it has been suggested that a physicist once referred to the measure of a square centimeter  as  being  "as  big  as  a  barn"  when  applied  to  nuclear  processes.    The  name  has persisted and microscopic cross sections are expressed in terms of barns.   The relationship between barns and cm   is shown below. 2 1 barn = 10 cm -24 2

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