Introduction to Mineralogy Dr. Tark Hamilton Chapter 13: Lecture 20 Optical Mineralogy &...
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Transcript of Introduction to Mineralogy Dr. Tark Hamilton Chapter 13: Lecture 20 Optical Mineralogy &...
Introduction to MineralogyDr. Tark Hamilton
Chapter 13: Lecture 20Optical 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
fig_13_01
Optical Parameters for Amphiboles
AnthophylliteOrthorhombic mmm
γ = 1.664-1.708β = 1.647-1.689α = 1.639-1.671δ = 0.02+/-.003
CummingtoniteMonoclinic 2/mγ = 1.615-1.697β = 1.605-1.685α = 1.598-1.674δ = 0.02+/-.003
Klein (1964)Wabush Iron Fm
Labrador
(Mg,Fe)2(Mg,Fe)5(OH)2O22
Grunerite
Beware CrocidoliteFibrous amphiboles
fig_13_02
Electrical Vector of Plane Polarized Light: Time varying potential field at x
Light will travel according to this vector in “Field Free Space”Vector addition occurs in crystal fields according to “Optical Density”
fig_13_03
Snell’s Law & Refractive Index
Light is refracted towards the vertical forany angle < 90° entering denser media.
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
fig_13_04
Dispersion: different wavelengths refract at different angles
For light of a fixed frequency, since C = λ x ν , red lighthas a greater velocity than violet due to its longer wavelength
fig_13_05
Total Internal Reflection& the Critical Angle
Air, n = 1.0
DOD’ = Critical Angle, ni / nr sin i = 1.0No emergent light
(non destructive testing of gems)
fig_13_06
Pulfrich Refractometer
Nglass = 1.90 , C.A. = 50° nmineral = 1.455 Opal !
Unknown mineral
Glass hemisphere
telescope
fig_13_07
Plane Polarized Light
Circularly or randomly polarized light
fig_13_08
Polarizing Substances: transmission directions
Superposed Tourmaline Crystals Superposed “Ray-ban” sheets
fig_13_09
Polarized Light by Reflection & Refraction
Planar Surfaces (including minerals) absorb or scattervibration directions which are not parallel to the surface.Reflected or transmitted light becomes plane polarized.
Isotropic Minerals & Relief in n=1.54
Mineral Fluorite Sodalite Pyrope Diamond
Index of Refraction
1.433 1.483 1.714 –
1.750
2.417
Relief - Very low - Low + High + Extreme
fig_13_11
Isotropic Crystals & the Becke Line
Mineral in FocusShowing Relief
nmineral > noil
Mineral in Focus Lowered stage
nmineral > noil
Becke Line moves in
Mineral in Focus Lowered stage
nmineral < noil
Becke Line moves out