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Optical Mineralogy in a Nutshell
Use of the petrographic microscope in two easy lessons Part II © Jane Selverstone
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Quick review Isotropic minerals –velocity changes as light enters mineral, but then is the same in all directions thru xtl; no rotation or splitting of light. These minerals are characterized by a single RI (because light travels with same speed throughout xtl) Anisotropic minerals –light entering xtls is split and reoriented into two plane-polarized components that vibrate perpendicular to one another and travel with different speeds. Uniaxial minerals have one special direction along which light is not reoriented; characterized by 2 RIs. Biaxial minerals have two special directions along which light is not reoriented; characterized by 3 RIs.
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We’ve talked about minerals as magicians - now let’s prove it!
calcite calcite calcite calcite calcite ordinary ray, w (stays stationary) extraordinary ray, e (rotates)
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Conclusions from calcite experiment
single light ray coming into cc is split into two rays e ray is refracted - changes direction & speed rays have different velocities, hence different RIs stationary ray=ordinary, rotating ray=extraordinary because refraction of e is so large, cc must have hi d (remember: d = nhi - nlo) If we were to look straight down c-axis, we would see only one dot – no splitting! C-axis is optic axis (true for all uniaxial minerals, but unfortunately not for biaxial minerals) More on this in a few minutes…
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Birefringence/interference colors
Thickness in microns Retardation in nanometers
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Back to birefringence/interference colors
Observation: frequency of light remains unchanged during splitting, regardless of material fast ray (low n) D mineral grain slow ray (high n) d F= V/l if light speed changes, l must also change plane polarized light l is related to color; if l changes, color changes waves from the two rays can be in phase or out of phase upon leaving the crystal lower polarizer
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Interference phenomena
When waves are in phase, all light gets killed When waves are out of phase, some component of light gets through upper polarizer and the grain displays an interference color; color depends on retardation When one of the vibration directions is parallel to the lower polarizer, no light gets through the upper polarizer and the grain is “at extinction” (=black) See Nesse, p (3rd edition)
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At time t, when slow ray 1st exits xtl:
Slow ray has traveled distance d Fast ray has traveled distance d+D Optional slide D=retardation time = distance/rate fast ray (low n) D mineral grain slow ray (high n) d plane polarized light D = thickness of t.s. x birefringence lower polarizer
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Uh oh... Let’s look at interference colors in a natural thin section:
Note that different grains of the same mineral show different interference colors – why?? ol plag Uh oh... If every grain of the same mineral looks different, how are we ever going to be able to identify anything?? Different grains of same mineral are in different orientations
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Time for some new tricks: the optical indicatrix
Thought experiment: Consider an isotropic mineral (e.g., garnet) Imagine point source of light at garnet center: turn light on for fixed amount of time, then map out distance traveled by light in that time What geometric shape is defined by mapped light rays?
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Isotropic indicatrix Light travels the same distance in all directions; n is same everywhere, thus: d = nhi-nlo = 0 = black Soccer ball (or an orange)
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anisotropic minerals - uniaxial indicatrix
c-axis Let’s perform the same thought experiment… c-axis calcite quartz
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Uniaxial indicatrix calcite quartz
c-axis c-axis tangerine = uniaxial (-) calcite Spaghetti squash = uniaxial (+) quartz (this is not strictly correct, but works for our purposes…)
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Uniaxial indicatrix nw ne nw
Circular section is perpendicular to the stem (c-axis)
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Uniaxial indicatrix (biaxial ellipsoid)
What can the indicatrix tell us about optical properties of individual grains?
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Propagate light along the c-axis, note what happens to it in plane of thin section
nw - nw = 0 therefore, d=0: grain stays black (same as the isotropic case) nw
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Now propagate light perpendicular to c-axis
ne - nw > 0 therefore, d > 0 ne nw ne nw ne nw ne nw ne nw Grain changes color upon rotation. Grain will go black whenever indicatrix axis is E-W or N-S This orientation will show the true d of the mineral (highest interference colors)
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anisotropic minerals - biaxial indicatrix
feldspar clinopyroxene Now things get a lot more complicated…
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Biaxial indicatrix (triaxial ellipsoid)
2Vz The potato! There are 2 different ways to cut this and get a circle…
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Alas, the potato (indicatrix) can have any orientation within a biaxial mineral…
augite (cpx) olivine
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… but there are a few generalizations that we can make
The potato has 3 perpendicular principal axes of different length – thus, we need 3 different RIs to describe a biaxial mineral X direction = na (lowest) Y direction = nb (intermed; radius of circ. section) Z direction = ng (highest) Orthorhombic: axes of indicatrix coincide w/ xtl axes Monoclinic: Y axis coincides w/ one xtl axis Triclinic: none of the indicatrix axes coincide w/ xtl axes
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2V: a diagnostic property of biaxial minerals
When 2V is acute about Z: (+) When 2V is acute about X: (-) When 2V=90°, sign is indeterminate When 2V=0°, mineral is uniaxial 2V is measured using an interference figure… More in a few minutes
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How interference figures work (uniaxial example)
Converging lenses force light rays to follow different paths through the indicatrix Bertrand lens What do we see?? N-S polarizer Sample (looking down OA) Effects of multiple cuts thru indicatrix e w substage condensor W E
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Determining if mineral is uniaxial or biaxial
If uniaxial, isogyres define cross; arms remain N-S/E-W as stage is rotated biaxial or If biaxial, isogyres define curve that rotates with stage, or cross that breaks up as stage is rotated Reminder about how to get an interference figure Find a grain that stays dark as stage is rotated Go to highest power objective Insert Bertrand Lens Look down scope and rotate stage
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Use of interference figures, continued…
Determine the optic sign of the mineral: Rotate stage until isogyre is concave to NE (if biaxial) Insert gypsum accessory plate Note color in NE, immediately adjacent to isogyre -- Blue = (+) Yellow = (-) uniaxial (+) (+) biaxial
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Determining optic sign with the gypsum plate - what happens?
slow blue in NE = (+) Optional slide Gypsum plate has constant D of nm = 1st-order pink Isogyres = black: D=0 Background = gray: D=150 Add to/subtract from 530 nm: =680 nm = blue = (+) =380 nm = yellowish = (-) Addition = slow + slow Subtraction = slow + fast
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Biaxial interference figures
There are lots of types of biaxial figures… we’ll concentrate on only two 1. Optic axis figure - pick a grain that stays dark on rotation Will see one curved or straight isogyre determine sign w/ gypsum plate (+) (-) determine 2V from curvature of isogyre 90° 60° 40° See Nesse (p. 100, 3rd ed)
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Biaxial interference figures
2. Bxa figure (acute bisectrix) - obtained when you are looking straight down between the two O.A.s. Hard to find, but look for a grain with intermediate d. Use this figure to get sign and 2V: (+) 2V=20° 2V=40° 2V=60° See Nesse (p. 97, 3rd ed.) Now do questions 1 and 2
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Quick review of why we use indicatrix:
Indicatrix gives us a way to relate optical phenomena to crystallographic orientation, and to explain differences between grains of the same mineral in thin section hi d lo d Isotropic? Uniaxial? Biaxial? Sign? 2V? All of these help us to uniquely identify unknown minerals.
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Some new properties: Cleavage
Most easily observed in PPL (upper polarizer out), but visible in XN as well No cleavages: quartz, olivine 1 good cleavage: micas 2 good cleavages: amphiboles, pyroxenes
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Some new properties: Cleavage
2 cleavages intersecting at ~90° pyroxene 60° 120° 2 cleavages intersecting at 60°/120°: amphibole
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Some new properties: Twinning
Presence and style of twinning can be diagnostic Twins are usually most obvious in XN (upper polarizer in)
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Twinning - some examples
Clinopyroxene (augite) Simple twin on {100} Plagioclase Pericline twin on (h01) Polysynthetic albite twins on (010) Simple (Carlsbad) twin on (010)
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Some new properties: Extinction angle
Extinction behavior is a function of the relationship between indicatrix orientation and crystallographic orientation inclined extinction parallel extinction
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Extinction angle – parallel extinction
All uniaxial minerals show parallel extinction Orthorhombic minerals show parallel extinction (this is because xtl axes and indicatrix axes coincide) orthopyroxene XN PPL
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Extinction angle - inclined extinction
Monoclinic and triclinic minerals: indicatrix axes do not coincide with crystallographic axes These minerals have inclined extinction (and extinction angle helps to identify them) extinction angle clinopyroxene Now do questions 3 and 4
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Review – techniques for identifying unknown minerals
Start in PPL: Color/pleochroism Relief Cleavages Habit Then go to XN: Birefringence Twinning Extinction angle Uniaxial or biaxial? 2V if biaxial Positive or negative?
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Go to Nesse or similar book…
Chemical formula Crystal system Uni or biaxial, (+) or (-) RIs: lengths of indicatrix axes Birefringence 2V if biaxial Diagrams: Crystallographic axes Indicatrix axes Optic axes Cleavages Extinction angles
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Another example Crystallographic axes: a, b, c
Optic axes Indicatrix axes: X, Y, Z Cleavages Extinction angles Then read text re color, pleochroism, habit, cleavage, twinning, distinguishing features, occurrence – make sure properties match your observations. If not, check another mineral…
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On to real rocks… …good luck and have fun!
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