Transcript Slide 1
RDCH 702: Nucleosynthesis • Readings: Modern Nuclear Chemistry: Chapter 12 Nuclear Astrophysics, Chapter 2 Nuclear Properties • Formation processes Role of nuclear reactions • Relationship between nuclear properties and chemical abundance • Electron orbitals 3-1 Natural Element Production • • • • • • Nuclear Astrophysics fundamental information on the properties of nuclei and their reactions to the perceived properties of astrological objects processes that occur in space Universe is composed of a large variety of massive objects distributed in an enormous volume Most of the volume is very empty (< 1x10-18 kg/m3) and cold (~ 3 K) Massive objects very dense (sun's core ~ 2x105 kg/m3) and very hot (sun's core~16x106 K) At temperatures and densities light elements are ionized and have high enough thermal velocities to induce a nuclear reaction heavier elements were created by a variety of nuclear processes in massive stellar systems systems must explode to disperse the heavy elements distribution of isotopes here on earth underlying information on the elemental abundances nuclear processes to produce the primordial elements 3-2 Timeline • Big bang 15E9 years ago • Temperature 1E9 K • Upon cooling influence of forces felt 2 hours H (89 %) and He (11 %) Strong force for nucleus Electromagnetic force for electrons 3-3 Subatomic particles • A number of subatomic particles have relevance to radiochemistry Electron Proton Z, atomic number Neutron isotopes Photon Neutrino Positron a particle Is actually a nucleus b particle 3-4 •Chart of the nuclide trends •Actinides some distance from stable elements 3-5 Stable Nuclei N Z Number even even 160 odd even 53 even odd 49 odd odd 4 • As Z increases the line of stability moves from N=Z to N/Z ~ 1.5 Influence of the Coulomb force For odd A nuclei only one stable isobar is found for even A nuclei multiple stable nuclei are possible no stable heavier odd-odd nuclei Find the stable odd-odd nuclei 3-6 Origin of element • Initial H and He • Others formed from nuclear reactions H and He still most abundant • Noted difference in trends with Z 3-7 Abundances • General logarithmic decline in the elemental abundance with atomic number a large dip at beryllium (Z=4) peaks at carbon and oxygen (Z=6-8), iron (Z ~ 26) and the platinum (Z=78) to lead (Z=82) region a strong odd-even staggering • All the even Z elements with Z>6 are more abundant than their odd atomic number neighbors nuclear stability nearly all radioactive decay will have taken place since production the stable remains and extremely long lived isotopic abundances strong staggering and gaps lightest nuclei mass numbers multiple of 4 have highest abundances 3-8 Elemental Trends • Trends are based on isotopes rather than elements Isotope described the nucleus composition Number of protons and neutrons Stability driven by combination of nucleons 3-9 Abundances • Earth predominantly oxygen, silicon, aluminum, iron and calcium more than 90% of the earth’s crust • Solar system is mostly hydrogen some helium Based on mass of sun • Geophysical and geochemical material processing 3-10 Origin of Elements • • • • Gravitational coalescence of H and He into clouds Increase in temperature to fusion Proton reaction 1H + n → 2H + g 2H + 1H → 3He 2H + n → 3H 3H + 1H → 4He + g 3He + n → 4He + g 3H + 2H → 4He + n 2H + 2H → 4He + g 4He + 3H → 7Li + g 3He+4He → 7Be + g 7Be short lived Initial nucleosynthesis lasted 30 minutes * Consider neutron reaction and free neutron half life Further nucleosynthesis in stars No EC process in stars 3-11 Stellar Nucleosynthesis • He burning 4He + 4He ↔ 8Be + γ - 91.78 keV Too short lived 3 4He → 12C + γ + 7.367 MeV 12C + 4He →16O 16O + 4He →20Ne • CNO cycle 12C + 1H →13N + g 13N →13C + e++ νe 13C + 1H →14N + γ 14N + 1H →15O + γ 15O →15N + e+ + νe 15N + 1H →12C + 4He Net result is conversion of 4 protons to alpha particle 4 1H → 4He +2 e++ 2 νe +3 γ 3-12 Origin of elements Neutron Capture and proton emission 14N + n →14C +1H; 14N(n,1H)14C • Alpha Cluster Based on behavior of particles composed of alphas • Stability nuclear stability related to abundance Even-even, even A 3-13 Formation of elements A>60 Neutron Capture; S-process A>60 68Zn(n, γ) 69Zn, 69Zn → 69Ga + b- + n mean times of neutron capture reactions longer than beta decay half-life Isotope can beta decay before another capture Up to Bi 3-14 Nucleosynthesis: R process • Neutron capture time scale very much less than b- decay lifetimes • Neutron density 1028/m3 Extremely high flux capture times of the order of fractions of a second Unstable neutron rich nuclei • rapidly decay to form stable neutron rich nuclei • all A<209 and peaks at N=50,82, 126 (magic numbers) 3-15 • • • • • • P process Formation of proton rich nuclei Proton capture process 70<A<200 Photonuclear process, at higher Z (around 40) (g, p), (g,a), (g, n) 190Pt and 168Yb from p process Also associated with proton capture process (p,g) Variation on description in the literature 3-16 • Proton-rich nuclei with Z = 7-26 • (p,g) and b+ decays that populate the prich nuclei Also associated with rapid proton capture process • Initiates as a side chain of the CNO cycle 21Na and 19Ne • Forms a small number of nuclei with A< 100 rp process (rapid proton capture) 3-17 Origin of elements • Binding energy Difference between energy of nucleus and nucleons Related to mass excess Dm=mnucleonsmnucleus Ebind=Dmc2 * Related to nuclear models 3-18 Periodic property of element • Common properties of elements • Modern period table develop Actinides added in 1940s by Seaborg s, p, d, f blocks 3-19 Bohr Atom • Models of atoms Plum pudding Bohr atom Inclusion of quantum states Based on Rutherford atom • Bohr atom for 1 electron system Etotal =1/2mev2+q1q2/4peor q2=-e * Include proton and electron 1/2mev2-Ze2/4peor 2 d 1 Electron position described by wavefunction x, y, z, and time Probability of finding electron in a space proportional to 2 3-20 Bohr Atom • Net force on the electron is zero 0=Fdynamic+Fcoulombic 1/2mev2/r+q1q2/4peor2 Force is 1/r2 E Fdr Energy 1/r 1/2mev2/r-Ze2/4peor2 Z is charge on nucleus • Quantize energy through angular momentum mvr=nh/2p, n=1,2,3…. Can solve for r, E, v • R=(eoh2/pmee2)(n2/Z) Radius is quantized and goes at n2 R=0.529 Å for Z=1, n=1 Ao (Bohr radius) 3-21 Orbitals • Wavefunctions specified by quantum numbers n=1,2,3,4 Principal quantum number l=0 to n-1 Orbital angular momentum Electron orbitals * s,p,d,f ml= +l Spin=+-1/2 Energy related to Z and n * DEtrans=kZ2D(1/n2) 3-22 Orbitals 3-23 Many Electron Atoms • Electron configuration Based on quantum numbers Pauli exclusion principle Aufbau principle and Hund’s rule Degenerate orbitals have same spin Maximize unfilled orbitals * 1s 2s 2p 3s 3p 4s 3d 4p 5s 4d 5p 6s 4f 5d 6p 7s 5f 3-24 Many electron orbitals • Electron configuration of Zr and Zr4+ [Kr]4d25s2 and [Kr] • For Fe, Fe2+, and Fe3+ [Ar]4s23d6, [Ar]4s23d4, [Ar]4s23d3 • Effective nuclear charge Zeff=Z-s Related to electron penetration towards nucleus 3-25 Atomic Radii • Increase down a group • Decrease across a period Lanthanide and actinide contraction for ionic radius 3-26 3-27 Topic review • Routes and reactions in nucleosynthesis • Influence of reaction rate and particles on nucleosynthesis • Relationships between nuclear and chemical properties • Electron orbitals and interactions 3-28 Study Questions • • • • How are actinides made in nucleosynthesis? What is the s-process? What elements were produced in the big bang? Which isotopes are produced by photonuclear reactions? • What do binding energetic predict about abundance and energy release? • What are the stable odd-odd isotopes? 3-29 Pop Quiz • Discuss the reaction necessary for the formation of 12C in stellar processes. Why is this unusual? 3-30