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Introduction to Mineralogy Dr
Introduction to Mineralogy Dr. Tark Hamilton Chapter 13: Lecture 20 Optical Mineralogy & Petrography: Snell’s Law Camosun College GEOS 250 Lectures: 9:30-10:20 M T Th F300 Lab: 9:30-12:20 W F300
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Optical Parameters for Amphiboles
Klein (1964) Wabush Iron Fm Labrador Cummingtonite Monoclinic 2/m γ = β = α = δ = 0.02+/-.003 (Mg,Fe)2(Mg,Fe)5(OH)2O22 Anthophyllite Orthorhombic mmm γ = β = α = δ = 0.02+/-.003 Grunerite Beware Crocidolite Fibrous amphiboles fig_13_01
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Light will travel according to this vector in “Field Free Space”
Electrical Vector of Plane Polarized Light: Time varying potential field at x fig_13_02 Light will travel according to this vector in “Field Free Space” Vector addition occurs in crystal fields according to “Optical Density”
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Snell’s Law & Refractive Index
Light is refracted towards the vertical for any angle < 90° entering denser media. fig_13_03
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Refractive Index, Optical Density & the Speed of Light in Media
C = 3 x 108 m/s or 3 x 1017 nm/s in vacuo Cm < in denser media (more electrons w/mass) n = C / Cm or n = Cair / Cmineral (Refractive Index) i = angle of incident PPL r = angle of refracted PPL Sin i / Sin r = ni / nr = ci / cr Sin r = (ni /nr ) Sin i C = λ x ν , velocity = wavelength x frequency
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Dispersion: different wavelengths refract at different angles
For light of a fixed frequency, since C = λ x ν , red light has a greater velocity than violet due to its longer wavelength fig_13_04
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Total Internal Reflection & the Critical Angle
Air, n = 1.0 DOD’ = Critical Angle, ni / nr sin i = 1.0 No emergent light (non destructive testing of gems) fig_13_05
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Pulfrich Refractometer
Unknown mineral telescope Glass hemisphere Nglass = 1.90 , C.A. = 50° nmineral = Opal ! fig_13_06
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Circularly or randomly polarized light
Plane Polarized Light Circularly or randomly polarized light fig_13_07
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Polarizing Substances: transmission directions
Superposed Tourmaline Crystals Superposed “Ray-ban” sheets fig_13_08
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Polarized Light by Reflection & Refraction
Planar Surfaces (including minerals) absorb or scatter vibration directions which are not parallel to the surface. Reflected or transmitted light becomes plane polarized. fig_13_09
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Isotropic Minerals & Relief in n=1.54
Fluorite Sodalite Pyrope Diamond Index of Refraction 1.433 1.483 1.714 – 1.750 2.417 Relief - Very low - Low + High + Extreme
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Isotropic Crystals & the Becke Line
Mineral in Focus Lowered stage nmineral < noil Becke Line moves out Mineral in Focus Showing Relief nmineral > noil Mineral in Focus Lowered stage nmineral > noil Becke Line moves in fig_13_11
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