I'm not very patient, and I will spend more time trying to fiddle with a program to get it to do what I want rather than read through documentation. I will also try Google. So, I was very happy when I found a very simple and thorough video about exactly what I wanted: how to measure porosity in a thin section using ImageJ.
Thin Section Porosity ImageJ uploaded by Chris Liner on YouTube gives simple, step-by-step instructions on calculating porosity in a thin section.
I hope this helps other people looking for the same thing!
Requirements: ImageJ, thin section photographs
Tuesday, March 3, 2015
Sunday, March 16, 2014
Isostasy - Airy & Pratt
Isostasy
mountains have a crustal root that compensates for the additional relief (variation in thickness)
Pratt Isostasy
density varies laterally, so that mountains have a lower density than higher density, thinner portions of crust
- describes the state of equilibrium of a lithospheric plate floating on the asthenosphere
- the weight of columns of rock, at some depth called the depth of compensation, is everywhere equal
mountains have a crustal root that compensates for the additional relief (variation in thickness)
Pratt Isostasy
density varies laterally, so that mountains have a lower density than higher density, thinner portions of crust
Possible Mechanisms of Crustal Subsidence
Mechanisms that can generate sufficient subsidence to create basins:
Crustal thinning extensional stretching, erosion during uplift, and magmatic withdrawal
Mantle-lithospheric thickening cooling of lithosphere following either cessation of stretching or heating due to adiabatic melting or rise of asthenospheric melts
Sedimentary and volcanic loading local isostatic compensation of crust and regional lithospheric flexure, dependent on flexural rigidity of lithosphere, during sedimentation and volcanism
Tectonic loading local isostatic compensation of crust and regional lithospheric flexure, dependent on flexural rigidity of underlying lithosphere, during overthrusting and/or underpulling
Subcrustal loading lithospheric flexure during underthrusting of dense lithosphere
Asthenospheric flow dynamic effects of asthenospheric flow, commonly due to descent or delamination of subducted lithosphere
Crustal densification increased density of crust due to changing pressure/temperature conditions and/or emplacement of higher-density melts into lower-density crust
Principles of Sedimentology and Stratigraphy (5th ed.), Sam Boggs, Jr.
Crustal thinning extensional stretching, erosion during uplift, and magmatic withdrawal
Mantle-lithospheric thickening cooling of lithosphere following either cessation of stretching or heating due to adiabatic melting or rise of asthenospheric melts
Sedimentary and volcanic loading local isostatic compensation of crust and regional lithospheric flexure, dependent on flexural rigidity of lithosphere, during sedimentation and volcanism
Tectonic loading local isostatic compensation of crust and regional lithospheric flexure, dependent on flexural rigidity of underlying lithosphere, during overthrusting and/or underpulling
Subcrustal loading lithospheric flexure during underthrusting of dense lithosphere
Asthenospheric flow dynamic effects of asthenospheric flow, commonly due to descent or delamination of subducted lithosphere
Crustal densification increased density of crust due to changing pressure/temperature conditions and/or emplacement of higher-density melts into lower-density crust
Principles of Sedimentology and Stratigraphy (5th ed.), Sam Boggs, Jr.
Monday, January 27, 2014
Seismic Waves
Body Waves
- penetrate the body of the Earth
- travel faster in more elastic rocks
- body wave velocities increase with depth in the interior of the Earth
- subject to refraction and reflection
- increased rock temperature = decreased velocity
- increased confining pressure = increased velocity
Figure 1. A) P-wave motion. B) S-wave motion.
P-Waves
- primary waves, compressional waves
- fastest seismic waves
- wave motion: energy moves as a succession of compressions and expansions in the direction of wave travel - an accordion-like push-pull movement
- each square in the figure changes from square to rectangle to square again as the waves move through the rock
- travel through solids, liquids, & gases
S-Waves
- secondary waves, shear waves
- slower than P-waves
- wave motion: rock segments vibrate perpendicularly (at right angles, up-and-down or side-to-side) to the direction of wave travel - this more complex motion causes S-waves to travel more slowly
- travel through solids only
Surface Waves
- large-motion waves that travel through the outer crust of the Earth
- wave pattern resembles ripples caused when a pebble is dropped in a pond
- slowest seismic waves
- cause of destruction during an earthquake since they are channeled through the thin crust and their energy is less rapidly dissipated than body waves
Figure 2. a) Rayleigh wave motion. b) Love wave motion.
c) Surface expression of wave motion of Rayleigh & Love waves
Rayleigh Waves
- wave motion is similar to waves in an ocean (see figure)
Love Waves
- wave motion is a shear which moves the surface from side to side
Tuesday, January 14, 2014
Metamorphic Index Minerals
Metamorphic index minerals form under specific temperature and pressure conditions.
Another version showing kyanite.
This diagram shows shale being metamorphosed.
Chlorite and muscovite form at relatively low temperatures. Garnet forms at higher temperatures and pressures. Sillimanite indicates the highest level of temperatures and pressures.
Shale is metamorphosed to slate and then to phyllite. Schist is next to form, then gneiss when high-grade metamorphism is reached. Beyond 800°C, the rock may completely deform by melting.
Another version showing kyanite.
Monday, January 13, 2014
Bowen's Reaction Series
Bowen's Reaction Series is the order of mineral crystallization as a magma slowly cools.
The right branch of the chart is the continuous series of crystallization because the plagioclase minerals maintain the same basic crystal structure but change continuously in calcium and sodium content away from calcium-rich plagioclase towards a sodium-rich variety.
The left branch of the chart is the discontinuous series of crystallization because the reactions result in minerals of distinctly different structure.
Potassium feldspar, muscovite mica, and quartz do not react with the melt. By the time they crystallize, there is little liquid left.
Bowen's Reaction Series allows geologists to recognize why mineral variations exist in igneous rocks. A volcanic rock from an early eruption may be rich in iron, magnesium, and calcium and thus produce basalt. Therefore, later eruptions might be depleted in iron, magnesium, and calcium but enriched in potassium, sodium, and silica. These rocks would be less basaltic and more andesitic in composition.
Source: The Earth Through Time by Harold Levin
The right branch of the chart is the continuous series of crystallization because the plagioclase minerals maintain the same basic crystal structure but change continuously in calcium and sodium content away from calcium-rich plagioclase towards a sodium-rich variety.
The left branch of the chart is the discontinuous series of crystallization because the reactions result in minerals of distinctly different structure.
Potassium feldspar, muscovite mica, and quartz do not react with the melt. By the time they crystallize, there is little liquid left.
Bowen's Reaction Series allows geologists to recognize why mineral variations exist in igneous rocks. A volcanic rock from an early eruption may be rich in iron, magnesium, and calcium and thus produce basalt. Therefore, later eruptions might be depleted in iron, magnesium, and calcium but enriched in potassium, sodium, and silica. These rocks would be less basaltic and more andesitic in composition.
Source: The Earth Through Time by Harold Levin
Friday, August 30, 2013
Principle of Superposition
The principle of superposition states that in a sequence of undisturbed sedimentary layers, the oldest layers are on the bottom and the youngest layers are on the top.
This principle was formulated by Nicolas Steno in the 17th century.
Thrust faults can alter the understanding of the principle of superposition because they occur parallel to bedding and can be hard to detect. They can create situations where older layers overly younger layers. Scientists of Nicolas Steno's time were unaware of thrust faults.
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