Radiometric Dating History, Theory, Current Methods, Problems SRJC,
Radiometric Dating History, Theory, Current Methods, Problems SRJC, Physics 43, Spring 2011 Aaron Krive, Kevin Chee History Radioactive decay of Uranium was discovered in 1896 by French Scientist Henry Becquere. Possibility of dating using radioactivity was proposed by British scientist Lord Rutherford in 1905. The first list of geological ages based on radiometric dating published by Yale
radiochemist Professor B. B. Boltwood in 1907. US Geological Survey History Cont. Precise dating is supposed to have been accomplished from 1950 onward. List of the most common parent isotopes and daughter products: Parent Isotope Stable Daughter
Product Currently Accepted HalfLife Values Uranium-238 Lead-206 4.5 billion years Uranium-235 Lead-207
704 million years Thorium-232 Lead-208 14.0 billion years Rubidium-87 Strontium-87 48.8 billion years Potassium-40
Argon-40 1.25 billion years Samarium-147 US Geological Neodymium-143 Survey 106 billion years Theory of Radiometric Dating
Given initial conditions, the decay of a radioactive material into its stable daughter material should be constant. Thus, measuring the amounts of both the parent and daughter material ought to give an accurate date. Theory Cont. The mathematical expression that relates
radioactive decay to geologic time is called the age equation and is. This equation assume no initial daughter material US Geological Survey Theory Cont. This age equation takes into account the possibility of initial daughter material: D = D0 + N(ett 1) t = the age of the sample
D = the number of daughter atoms in the sample D0= the initial number of daughter atoms. N = the number of isotropic atoms at t, N = Noe-t tt t = the decay constant t=ln(2)/t1/2 Wikipedia http://en.wikipedia.org/wiki/Radiometric_d ating Uranium-Lead Dating One of the oldest and most refined of the radiometric dating methods Routine age range of ~1 million 4.5 billion years Routine precision in 0.1-1 % range
Method uses 2 distinct decay chains Uranium series: Actinium series: U 206Pb 235U 207Pb 238 Boltwood, B.B., 1907, On the ultimate disintegration products of the radio-active elements. Part II. The disintegration products of uranium: American Journal of Science 23: 77-88. Parrish, Randall R.; Noble, Stephen R., 2003. Zircon U-Th-Pb Geochronology by Isotope Dilution Thermal Ionization Mass Spectrometry (ID-TIMS). In Zircon (eds. J. Hanchar and P. Hoskin). Reviews in Mineralogy and Geochemistry, Mineralogical Society of America. 183-213.
The 2 UPb decay series: Uranium series: http://en.wikipedia.org/wiki/File:Decay_chain(4n%2B2,_Uranium_series).PNG Actinium series : http://en.wikipedia.org/wiki/File:Decay_scheme_U235.png Minerals used for dating: Zircon (ZrSiO4), is the preferred mineral analyzed: Zircon incorporates Uranium and Thorium atoms into its crystalline structure, but strongly rejects lead. Zircon has a high trapping temperature of 900C. Its clock is not easily disturbed by geologic events
not erosion or consolidation into sedimentary rocks, not even moderate metamorphism. Widespread in igneous rocks, which have no fossils to indicate their age. Tough, so easier to separate Zircon crystals from surrounding environment. http://geology.about.com/od/ geotime_dating/a/uraniumlead.htm Mineral / radioactive decay interaction (for Zircon) Each alpha decay damages the crystal structure of the Zircon In the decay steps where Pb is created, Pb is
ejected from the crystal lattice, again damaging the minerals structure. Thus, areas in mineral with high concentrations of Uranium and Thorium (early elements in decay chain) will have the most damage. Damage to the mineral structure can result in leaching of Pb from the Zircon sample, thus Romer, R.L. 2003. Alpha-recoil in U-Pb geochronology: Effectivedetermination. sample size matters. Contributions to effecting the precision of age
Mineralogy and Petrology 145, (4): 481-491. Mattinson, J.M., 2005. Zircon U-Pb Chemical abration (CA-TIMS) method: Combined annealing and multi-step dissolution analysis for Improved precision and accuracy of zircon ages. Chemical Geology. 200, 47-66. Process details: Given conditions where system is closed (no Pb lost) Age can be determined from: -The Pb/U ratios of each equation are plotted on the axis of the same graph. (Pb206/U238) plotted on the y-axis and (Pb207/U235) plotted on the x-axis. The plot results in a curved line called the concordia. A graph of a concordia can be seen 2 slides later. -The concordia represents ideal situations and can be
calculated directly from the equations and known half lives of our subject elements. -Proof of concept can be demonstrated by taking samples of varying ages from different locations, whos ratios (given closed system conditions) will all fall on the concordia line. ^ Dickin, A.P., 2005. Radiogenic Isotope Geology 2nd ed. Cambridge: Cambridge University Press. pp. 101. Process details (Pb losses): Zircon samples taken from a location are not usually perfect, thus some samples will have no loss while others will have varying degrees of Pb losses. Pb losses can be used to determine the time of disturbance events and age of samples.
Imagine a 1 billion year old zircon deposit. If there were no losses it would ride up the concordia perfectly to the 1 billion year point. (figure on next slide may be helpful in visualizing) Now imagine, at the 1 billion year birthdate , a strong disturbance (earthquake) which caused Pb losses of varying degrees in different areas of the zircon deposit. Pb loss follows a more linear type loss rate down to the origin. And samples with Pb losses from the same event would fall on a straight line from (1) the point on the concordia at time of disturbance to (2) the origin. This line is called the discordia. (A discordia can be seen in the next slide) After the disturbance, as time went along, the discordia would travel up with the growing concordia. The upper intercept of the two lines would be the current age of the sample The lower intercept would be the age of the disturbance.
^ Dickin, A.P., 2005. Radiogenic Isotope Geology 2nd ed. Cambridge: Cambridge University Press. pp. 101. Plot of concordia and discordia Standard age markers concordia Age of sample discordi a Data from samples with Pb losses Age of disturbance
http://www.talkorigins.org/faqs/dalrymple/radiometric_dating.html Problems With Radiometric Dating Based on assumptions (Constant decay, initial conditions) For many types of dating, there is no way to correct for leeching of the parent or daughter materials It is impossible to compare the results to the actual age and determine how accurate these results actually are. Constant Decay Daughter Material Current decay rates are cannot be verified as
constant over millions or billions of years. The decay rates are known to change because of environmental factors. Scientists must assume that there is no daughter material in the rock when it is formed. In the case of Uranium-Lead dating, scientists must assume that there was no lead in the rock when it formed. Relativity Dating institutions may use where the rock was found to help date the rock. For instance, the
Waikato Radiocarbon Dating Labs sample submission sheet asks for and estimate age and age limits. Science should not start with preconceptions, but with facts that lead to conclusions. Fossils with assumed ages are often used to give an approximate to strata when possible. However, dating the fossils with radiometric dating and using the fossils to give approximate dates is circular reasoning. http://www.radiocarbondating.com/ The End
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