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TEXTURAL AND MICROANALYSIS OF IGNEOUS ROCKS: TOOLS ...

TEXTURAL AND MICROANALYSIS OF IGNEOUS ROCKS: TOOLS ...

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mm diameter tip (which also corresponds to the smallest measurable crystal size).<br />

The tracings were digitized via high resolution scanning with a flatbed scanner.<br />

Crystal intersection areas were shaded gray, detected, and measured according<br />

to a best fit ellipse routine using the freeware program UTHSCSA ImageTool<br />

(http://ddsdx.uthscsa.edu/dig/itdesc.html). The best fit ellipse major and minor<br />

axis results were input into the spreadsheet program CSDslice written by Morgan<br />

and Jerram [106] to estimate the three-dimensional crystal habit. The crystal<br />

major axis data, the estimated 3D crystal habit, rock fabric, total area measured,<br />

and an estimate of crystal roundness were input into the program CSDcorrections<br />

version 1.37 written by Michael Higgins [68] to covert two-dimensional CSD data<br />

to true three-dimensional CSDs as outlined by Marsh [96]. The areas and numbers<br />

of crystals measured in each thin section are listed in table 3.1. Modal abundances<br />

of plagioclase (and olivine for Site 1203 Units 11 and 16) were measured as the<br />

percentage of the phase in the traced area, which Higgins [69] determined to be<br />

an accurate method for estimation of modal abundance.<br />

3.4.3 Electron Probe Microanalysis (EPMA) and Scanning Electron Microscopy<br />

Backscatter electron images and major element analyses were performed us-<br />

ing a JEOL JXA-8600 Superprobe electron microprobe at the University of Notre<br />

Dame. Backscatter electron images were collected using a 1 µm beam, an acceler-<br />

ating voltage of 20 kV, and a probe current of 25-50 nA. Microprobe analyses were<br />

performed using a 10 µm defocused beam, accelerating voltage of 15 kV, a probe<br />

current of 20 nA, 15 second on-peak counting time, and two background measure-<br />

ments per peak. Sodium was measured first to minimize loss via volatilization.<br />

Microprobe data were corrected for matrix effects using a ZAF correction rou-<br />

95

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