ESS C109/C209: Isotope Geochemistry

Lecture 2 Notes

Introduction to Isotope Geochemistry

April 4, 2007

 

Introduction

               The parts of an atom. Nomenclature for nuclear chemistry

p+ (= H+) = 11H+

n = 10n

eÐ = bÐ

Other things that interact with nuclei (created or destroyed in nuclear reactions)

a = 42He has mass, charge (typically), and energy

e+ = b+ has energy and charge but little mass

Photon = g has energy but no mass or charge

Neutrino = ne etc. has energy but no mass or charge

Exotic particles (muons, etc.)

 

               Hand out Nuclides & Isotopes booklets

 

Nuclear Chemistry

  1. Neutrons and protons interact to create nuclear chemistry.
    1. Analogous to the electron-nucleus (electronic) interactions in chemistry
    2. Some nuclear structures are stable (e.g., 42He)
      Stability determined by nuclear binding energy
      E=mc2 Ð Low energy (stable) nuclei are less massive. 1 amu=931.5 MeV

      Binding energy of 42He:

      Mass of 42He = 4.00260325 amu

      Mass of 2 11H = 2 x 1.007825032
      Mass of 2 10n = 2 x 1.008664923
      Total        = 4.03297991

      Binding energy = 0.030377 amu = 28.3 MeV


    3. Is a neutron more stable than 11H?

                                                                  i.      Less stable nuclei decay to more stable nuclei

                                                                    ii.      Most common mechanisms are a or b emission, or fission.

    1. Table 15 (p. 27) Ð Binding energies vs. mass.

  1. Why are some nuclei more stable than others? (Table 14 (p. 27) )
    1. Protons are like-charge, tend to repel

                                                                  i.      Too many protons ˆ unstable

    1. Neutrons dilute charge, bind protons together

                                                                  i.      More protons ˆ more neutrons

                                                                    ii.      Nonlinear Ð more neutrons per proton in heavy nuclei.

    1. Neutrons & protons like to Òpair upÓ

                                                                  i.      Even # of protons = more stable

                                                                    ii.      Even # of neutrons = more stable

                                                                      iii.      For light elements, same # protons & neutrons = more stable

1.      Even-Even nuclei most stable

2.      Can you find any stable odd-odd nuclei?
Odd-Odd nuclei only stable for light elements
(when # protons = # neutrons)

    1. Shell structure: ÒNoble nucleiÓ

                                                                  i.      In chemistry, some elements are particularly stable in atomic form Ð which ones?  (He, Ne, Ar, Kr, Xe)

1.      Stable because they have full electronic shells, i.e. 2 s-electrons, 6 p-electrons, etc. in each orbital.

                                                                    ii.      There are nuclear-chemical shells also, nuclei with full shells of either protons or neutrons are particularly stable, or ÒmagicÓ.

1.      Magic numbers are 2, 8, 20, 28, 50, 82, 126, 184

2.      Look at calcium in booklet. See the magic number?

3.      A nucleus with a magic number of neutrons and a magic number of protons is Òdoubly magicÓ.

    1. Return to Table 15 (p. 27). Why is 42He so stable?

  1. Modes of decay on unstable nuclei
    1. b-decay (4019K, p. 46) Students write equations.

                                                                  i.      Too many protons? b+ -decay (whereÕs it go?)

                                                                    ii.      Too many neutrons? b- -decay (whereÕs it go?)

    1. Electron capture (e) Ð similar to b+ -decay
    2. a-decay (84Be, p. 40)

                                                                  i.      emission of 42He

                                                                    ii.      most common for nuclei beyond mass 140

    1. Spontaneous fission (24494Pu, p. 71)

                                                                  i.      Splitting yields two daughters of similar mass (~1/2 parent mass).

                                                                    ii.      Daughters are typically heterogenous (many different products).

                                                                      iii.      Most common for very heavy nuclei (m > 200)

                                                                     iv.      Usually accompanied by many short-lived b- decays to regain line of stability.