Figure of rare earth elemental abundances removed due to copyright restrictions. See figure 3.1 on page 26 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 1 Given that the r-process nucleosynthetic production ratio for 235U/238U is roughly 1.35 ± 0.3, use the present-day terrestrial isotope ratio to estimate the “age of the elements” assuming a one-time production event for these isotopes. 2 Figures of recession velocity vs. distance removed due to copyright restrictions. See figure 4.4 on page 50 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 3 No. of 238U atoms/100 235U atoms 400 Ratio when earth formed 300 Evolution of galaxy ratio 200 100 0 Ratio after first supernova 0 5 10 15 20 25 Time after our galaxy formed (Billions of years) No. of 232Th atoms/100 235U atoms 2000 Evolution of galaxy ratio 1500 1000 Ratio when earth formed 500 0 Ratio after first supernova 0 5 10 15 20 25 Time after our galaxy formed (Billions of years) Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 4 Figure of uranium and thorium ratios vs. time and age removed due to copyright restrictions. See figure 7.1 on page 81 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 5 Li+ O-2 Be2+ 0.92 1.38 1.18 K+ 1.31 0.45 Cl-1 S-2 Na+ F-1 Al3+ Mg2+ 0.39 Si4+ 0.26 1.84 1.81 0.72 Ca2+ 1.51 1.00 Rb+ 1.61 Sr2+ 1.18 Mn2+ Ti4+ 0.42 0.66 Fe2+ Fe3+ 0.63 0.49 Zr4+ 0.59 Ce3+ 1.14 Eu2+ 1.25 Th4+ U4+ 1.05 1.00 Lu3+ Eu3+ 1.05 1.06 Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 6 Anion Triangular coordination Tetrahedral coordination 0.15 < Rc / Ra < 0.22 0.22 < Rc / Ra < 0.41 A B C D Octahedral coordination Cubic coordination 0.41 < Rc / Ra < 0.73 Rc / Ra > 0.73 Cation Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 7 Figure of 87Sr/86Sr vs. 87Rb/86Sr (atomic) removed due to copyright restrictions. See figure 12.7 on page 179 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 8 © AAAS. All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/fairuse. Source: Amelin, Yuri, Alexander N. Krot, et al. "Lead Isotopic Ages of Chondrules and Calcium-Aluminum-Rich Inclusions." Science 297, no. 5587 (2002): 1678-83. 9 Figure of 207Pb/204Pb vs. 206Pb/204Pb with 4567 million year reference evolution line removed due to copyright restrictions. See figure 10.3 on page 121 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 10 Figure of (26Al/27Al)INI x10-5 and time relative to CAI formation (x106 years) vs. various meteorites removed due to copyright restrictions. See figure 11.7 on page 153 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 11 Figure of ages of various meteorites with respect to solar system formation removed due to copyright restrictions. See figure 13.1 on page 193 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 12 Figure of 107Ag/109Ag vs. 108Pd/109Ag, x105 of Gibeon Metal and Normal Silver removed due to copyright restrictions. See figure 12.9 on page 182 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 13 High Hf/W silicate earth increased growth of 182W c pi tion u l o ev Undifferentiated solar system objects 1.85170 0 10 20 30 Time of core formation W -I so to Core ratio Ch on dr iti c 182 W/183W Growth 1.85205 lk u B th Ear e at lic i S Chondrite Low Hf/W core no increase in 182W Silicate Earth high Hf/W Core low Hf/W 40 50 Years after t0 (Ma) Image by MIT OpenCourseWare. 14 Figure of ε182 of Early Archaean samples and 3.8 billion year igneous mix with inset of ε182 vs. Cr/Ti for Early Archaean samples, Enstatite chondrites, Allende (C1), and Iron meteorites removed due to copyright restrictions. See figure 19.1 on page 247 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 15 Figure of ε182 of carbonaceous chondrites, ordinary chondrites, and iron meteorites removed due to copyright restrictions. See figure 11.8 on page 154 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 16 Rock and metal condense in the hot inner solar system. Solar nebula contracts and flattens into a single spinning disk. The Sun will form in the center of the disk containing all the elements, but mostly h and He. (A) H, He and other noble gases remain gas. Other elements condense according to their volatility. (B) Rock, metal and ices condense in the outer solar system. Accretion of planetesi-mals which will combine in giant impacts to form the planets. (C) T-Tauri phases of the Sun creates large solar wind that ejects gas from between the planets. (D) Solid particles stick togeather. Once larger objects have accreted, they are called planetesimals. (E) Large outer planets have sufficient mass to accumulate vast atmosphere including H2 and He. Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 17 Andromeda Galaxy Triangulum Galaxy The Local Group Milky Way Galaxy Milky Way Galaxy Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 18 Pluto’s Orbit Kuiper Belt and outer Solar System planetary orbits Orbit of Binary Kulper Belt Object 1998 WW31 The Oort Cloud (Comprising many billions of comets) Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 19 Earth 0.8 os m H ic ” ab un 0.4 da nc e Loss/gain of metal Gain/loss of silicon “C 0.6 da xi O n/ io ct du Re Fe(metal)/Si E n tio L 0.2 CO/CV LL CM 0 0 0.2 0.4 0.6 C1 0.8 1.0 Fe(oxide)/Si Image by MIT OpenCourseWare. After figure 11.1 in Tolstikhin, Igor and Jan Kramers. "The Evolution of Matter: From the Big Bang to the Present Day." 20 Figure of ε182(Earth) - ε182(initial) vs. time (millions of years) and Concentration/concentration in C1 vs. time (millions of years) removed due to copyright restrictions. See figure 18.3 on page 241 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 21 1.2 Ti Mo Zr Pr 1.0 0.8 Volitility coefficient Nd Ba Ce Th La Yb Cu Nb Gd U Er Lu Ca Al Sr Lu Ta Rh Sm Sc Tm Dy W V Tb Y Re Hf Os Ru Ir Mg Si Co Cr 0.6 Fe Pd Pt Ni Au P As 0.4 O Cu Mn Na Li Ga 0.2 0 0 10 20 30 40 Cd Sb Pb Rb K 50 Sn Ge Cs Ag Bi 60 Se ln F Zn Te Br Cl l S Tl B C 70 H N 80 Volitility order Highly refractories Medium refractories Semi-volatiles Highly volatiles Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 22 Figure of Depletion relative to C1 and refractory element vs. Increasing siderophile behavior of refractory and transitional elements and volatile elements and low-pressure metal-silicate partition coefficients removed due to copyright restrictions. See figure 18.1 on page 232 of Tolstikhin, Igor and Jan Kramers. “The Evolution of Matter: From the Big Bang to the Present Day.” Cambridge University Press, 2008. 23 Cumulation% 0 Rb Ba K B Be Pr Sr Hf Nb Sm Eu Tb In Er Lu Tm Ti Ca O Mg Si V Cs Cd Cu TI I Fe W Ag P N As Se Re Ru Ir 0.1 0.2 0.3 0.4 0.5 0.6 Xu Fraction in the core 0.7 0.8 0.9 Xu Fraction in the crust Crust K Hf Na Lithophile Mantle Ti Ca Mg Si Xcs Fraction in the core Xcs mantle Fe Core W Siderophile and Calcophile Au Xcs crust 1 Th U F La Ce Ta Nd Zr Li Na Gd Dy Ho Y Yb Ga AI Sc Zn Co Mn Pb Cr Sn Hg Bi CI Br Ge Sb Ni S Mo Au Pd Pt Os Image by MIT OpenCourseWare. After How to Build a Habitable Planet. 24 TN Nucleosynthesis Presolar grains Solar Nebula ∆tNF Condensation Accretion Solar wind Regolith Melting Differentiation Core formation Meteorite Parent Body Cosmic rays TF Impacts Meteoroids on heliocentric orbits TC tC Orbital perturbations Collision with Earth tF TT tT Meteorite in laboratory TL Image by MIT OpenCourseWare. After figure 98 in Heide & Wlotzka, Meteorites. 25 Time After Solar System Formation (Myr) ε182W +10.0 Juvinas eucrite +8.0 Eucrite parent body mantle +6.0 +4.0 +2.0 Mars 0 Earth -2.0 Two-stage model Solar system E1 Iron meteorites encrite parent body core Core -4.0 0 10 E2 MC 20 30 40 50 60 Image by MIT OpenCourseWare. 26 Partition model Partition coefficient Do Ro E Cation radius Image by MIT OpenCourseWare. 27 © AAAS. All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/fairuse. Source: Blundy, Jon, and Bernard Wood. "Partitioning of Trace Elements between Crystals and Melts." Earth and Planetary Science Letters 210, no. 3 (2003): 383-97. 28 Courtesy of Mineralogical Society of America. Used with permission. 29 MIT OpenCourseWare http://ocw.mit.edu 12.744 Marine Isotope Chemistry Fall 2012 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.