Isotopes Reading: Winter, Chapter 9, pp. 167-180.

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Presentation transcript:

Isotopes Reading: Winter, Chapter 9, pp

Isotopes Same Z, different A (variable # of neutrons) General notation for a nuclide: 614C

Isotopes Same Z, different A (variable # of neutrons) General notation for a nuclide: 614C As n varies  different isotopes of an element 12 C 13 C 14 C

Stable Isotopes Stable: last ~ forever Chemical fractionation is impossible Mass fractionation is the only discrimination possible

Oxygen Isotopes Concentrations expressed by reference to a standard International standard for O isotopes = standard mean ocean water (SMOW) 16 O99.756% of natural oxygen 17 O 0.039%“ 18 O 0.205% “

18 O and 16 O are the commonly used isotopes and their ratio is expressed as  :  18 O/ 16 O) = eq  result expressed in per mille (‰) result expressed in per mille (‰) (O/O)(O/O) (O/O) x sample 1816 SMOW 1816 SMOW What is  of SMOW?? What is  for meteoric water?

Evaporation seawater  water vapor (clouds) –Light isotope enriched in vapor > liquid –Efficient, since  mass = 1/8 total mass  = therefore < thus  clouds is (-) (O/O)(O/O) (O/O) x vapor 1816 SMOW 1816 SMOW (O/O)1816Vapor (O/O)1816SMOW

Relationship between d( 18 O/ 16 O) and mean annual temperature for meteoric precipitation, after Dansgaard (1964). Tellus, 16,

 O and H isotopes Juvenile vs. meteoric vs. brine water   18 O for mantle rocks  surface-reworked sediments Evaluate contamination of mantle-derived magmas by crustal sediments Stable isotopes are useful in assessing relative contribution of various reservoirs, each with a distinctive isotopic signature

Radioactive Isotopes Unstable isotopes decay to other nuclides The rate of decay is constant, and not affected by P, T, X… Parent nuclide = radioactive nuclide that decays Daughter nuclide(s) are the radiogenic atomic products

Isotopic variations between rocks, etc. due to: 1. Mass fractionation (as for stable isotopes) Only effective for light isotopes: H He C O S

Isotopic variations between rocks, etc. due to: 1. Mass fractionation (as for stable isotopes) 2. Daughters produced in varying proportions resulting from previous event of chemical fractionation

Isotopic variations between rocks, etc. due to: 1. Mass fractionation (as for stable isotopes) 2. Daughters produced in varying proportions resulting from previous event of chemical fractionation 40 K  40 Ar by radioactive decay Basalt  rhyolite by FX (a chemical fractionation process) Rhyolite has more K than basalt 40 K  more 40 Ar over time in rhyolite than in basalt 40 Ar/ 39 Ar ratio will be different in each

Isotopic variations between rocks, etc. due to: 1. Mass fractionation (as for stable isotopes) 2. Daughters produced in varying proportions resulting from previous event of chemical fractionation 3. Time The longer 40 K  40 Ar decay takes place, the greater the difference between the basalt and rhyolite will be

Radioactive Decay The Law of Radioactive Decay eq  dN dt N or dN dt =N # parent atoms time  1½¼

D = Ne t - N = N(e t -1) eq 9-14  age of a sample (t) if we know: D the amount of the daughter nuclide produced N the amount of the original parent nuclide remaining the decay constant for the system in question

The K-Ar System 40 K  either 40 Ca or 40 Ar – 40 Ca is common. Cannot distinguish radiogenic 40 Ca from non-radiogenic 40 Ca – 40 Ar is an inert gas which can be trapped in many solid phases as it forms in them

The appropriate decay equation is: eq Ar = 40 Ar o + 40 K(e - t -1) Where e = x a -1 (proton capture) and = x a -1 (whole process) and = x a -1 (whole process) e      

Blocking temperatures for various minerals differ 40 Ar- 39 Ar technique grew from this discovery

Sr-Rb System  87 Rb  87 Sr + a beta particle ( = 1.42 x a -1 )  Rb behaves like K  micas and alkali feldspar  Sr behaves like Ca  plagioclase and apatite (but not clinopyroxene)  88 Sr : 87 Sr : 86 Sr : 84 Sr ave. sample = 10 : 0.7 : 1 : 0.07  86 Sr is a stable isotope, and not created by breakdown of any other parent

Isochron Technique Requires 3 or more cogenetic samples with a range of Rb/Sr Could be: 3 cogenetic rocks derived from a single source by partial melting, FX, etc.3 cogenetic rocks derived from a single source by partial melting, FX, etc. Figure 9-3. Change in the concentration of Rb and Sr in the melt derived by progressive batch melting of a basaltic rock consisting of plagioclase, augite, and olivine. From Winter (2001) An Introduction to Igneous and Metamorphic Petrology. Prentice Hall.

Isochron Technique Requires 3 or more cogenetic samples with a range of Rb/Sr Could be: 3 cogenetic rocks derived from a single source by partial melting, FX, etc.3 cogenetic rocks derived from a single source by partial melting, FX, etc. 3 coexisting minerals with different K/Ca ratios in a single rock3 coexisting minerals with different K/Ca ratios in a single rock

For values of t less than 0.1: e t -1  t Thus eq for t < 70 Ga (!!) reduces to: eq Sr/ 86 Sr = ( 87 Sr/ 86 Sr) o + ( 87 Rb/ 86 Sr) t y = b + x m = equation for a line in 87 Sr/ 86 Sr vs. 87 Rb/ 86 Sr plot Recast age equation by dividing through by stable 86 Sr 87 Sr/ 86 Sr = ( 87 Sr/ 86 Sr) o + ( 87 Rb/ 86 Sr)(e t -1) eq 9-17 = 1.4 x a -1

a bc toto 86 Sr 87 Sr o () 86 Sr 87 Sr 86 Sr 87 Rb Begin with 3 rocks plotting at a b c at time t o

After some time increment (t 0  t 1 ) each sample loses some 87 Rb and gains an equivalent amount of 87 Sr a bc a1a1 b1b1 c1c1 t1t1 toto 86 Sr 87 Sr 86 Sr 87 Rb 86 Sr 87 Sr o ()

At time t 2 each rock system has evolved  new line Again still linear and steeper line a bc a1a1 b1b1 c1c1 a2a2 b2b2 c2c2 t1t1 toto t2t2 86 Sr 87 Sr 86 Sr 87 Sr o () 86 Sr 87 Rb

Isochron technique produces 2 valuable things: 1. The age of the rocks (from the slope = t) 2. ( 87 Sr/ 86 Sr) o = the initial value of 87 Sr/ 86 Sr Figure 9-9. Rb-Sr isochron for the Eagle Peak Pluton, central Sierra Nevada Batholith, California, USA. Filled circles are whole-rock analyses, open circles are hornblende separates. The regression equation for the data is also given. After Hill et al. (1988). Amer. J. Sci., 288-A,

Figure Estimated Rb and Sr isotopic evolution of the Earth’s upper mantle, assuming a large-scale melting event producing granitic-type continental rocks at 3.0 Ga b.p After Wilson (1989). Igneous Petrogenesis. Unwin Hyman/Kluwer.