TEXTURAL AND MICROANALYSIS OF IGNEOUS ROCKS: TOOLS ...
TEXTURAL AND MICROANALYSIS OF IGNEOUS ROCKS: TOOLS ...
TEXTURAL AND MICROANALYSIS OF IGNEOUS ROCKS: TOOLS ...
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where R is the gas constant, T is temperature (Kelvin), i is the element of interest,<br />
and XAn is the mole fraction of anorthite. Using equation 3.1, Ginibre et al.<br />
[59] noted that temperatures in the range of 850-1,000 ◦ C had miniscule effect on<br />
calculated melt concentrations for Sr and Ba (within their analytical uncertainty).<br />
Likewise, Bindeman et al. [7] showed that variations of ∼150 ◦ C produce < 10%<br />
differences for particular partition coefficients, which were often within error of<br />
the respective D values.<br />
Blundy and Wood [11] presented an alternative model for quantitative predic-<br />
tion of D values based upon thermodynamic principles and lattice strain theory<br />
(i.e., [15]). Specifically, they noted the dominant roles of cation size, lattice site<br />
size, and elasticity of the lattice site related to cation substitution in minerals.<br />
The elastic response of a lattice site to cation substitution is measured by Young’s<br />
Modulus (E), and the value of E plag is dependent upon plagioclase An content<br />
and the charge of the substituent cation [11, 12]. Equation 3.2 (Equation 2 of<br />
Blundy and Wood [11]) is the basis of their predictive D model that I apply to<br />
plagioclase,<br />
Di = D z+<br />
o<br />
∗ exp<br />
−4πEplagNA<br />
<br />
ro<br />
2 (r2 o − r2 1<br />
i ) + 3 (r3 i − r3 o )<br />
<br />
RT<br />
(3.2)<br />
where Di of a trace element (i) is a function of the strain compensated partition<br />
coefficient for the divalent (D 2+<br />
0 ) or trivalent (D 3+<br />
0 ) substituent cation, Young’s<br />
Modulus for the plagioclase M lattice site (E plag), NA (Avogadro’s Number), the<br />
radius of the plagioclase M site (ro), the radius of the substituent cation (ri),<br />
the gas constant (R), and crystallization temperature (T). For a more thorough<br />
discussion of this model see Blundy and Wood [11, 12].<br />
99