Rheology - Structural Geology - Lecture Notes, Study notes of Geology

In these Lecture notes, Professor has tried to illustrate the following points : Rheology, Rocks, Mechanical Units, Polycrystalline Nature, Local Anisotropies, Rheological Models, Elastic Behavior, Applied Stress, Undeformed State, Spring Displacement

Typology: Study notes

2012/2013

Uploaded on 07/22/2013

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I. Continuum Models of Material Behavior
A. Continua: assumption that rocks behave as cohesive mechanical units,
averaging out effects of local anisotropies and polycrystalline nature
B. Rheological Models for Rock
1. Elastic Behavior
a. linear elastic behavior: material deforms by an amount
proportional to the applied stress
(1) when stress is released, material strain recovers to original
undeformed state
(2) Young's Relations
(a) Stress = E(strain)
b. Similar to Hooke's law for a spring (ideal elastic)
(1) Force = k(spring displacement)
c. Stress-strain diagram
(1) normal stress on y axis
(2) lengtening or shortening strain on x axis
(3) true elastic solid: linear relationship
2. Viscous Behavior
a. example fluid behavior
(1) stress applied to fluid: fluid deformation (motion)
(a) remove stress, fluid stops, but does not recover to
initial state
b. Viscous behavior: nonrecoverable strain
(1) Newtonian fluid
(a) linear relation between stress and strain rate
(b) > stress, > rate of strain (dx/dt)
(c) Newtonian stress-strain diagram
i) stress = y-axis
ii) strain rate = x-axis
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I. Continuum Models of Material Behavior A. Continua: assumption that rocks behave as cohesive mechanical units, averaging out effects of local anisotropies and polycrystalline nature B. Rheological Models for Rock

  1. Elastic Behavior a. linear elastic behavior: material deforms by an amountproportional to the applied stress (1) when stress is released, material strain recovers to original undeformed state (2) Young's Relations (a) Stress = E(strain) b. Similar to Hooke's law for a spring (ideal elastic) (1) Force = k(spring displacement) c. Stress-strain diagram (1) normal stress on y axis (2) lengtening or shortening strain on x axis (3) true elastic solid: linear relationship
  2. Viscous Behavior a. example fluid behavior (1) stress applied to fluid: fluid deformation (motion) (a) remove stress, fluid stops, but does not recover toinitial state

b. Viscous behavior: nonrecoverable strain (1) Newtonian fluid

(a) linear relation between stress and strain rate (b) > stress, > rate of strain (dx/dt) (c) Newtonian stress-strain diagram i) stress = y-axis ii) strain rate = x-axis

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iii) as stress --- 0, strain rate ----- 0, but strain does not recover (permanent deformation) (2) Bingham fluid (a) exponential relation between stress and strain rate (b) internal shear strength of fluid exists i)ii) (^) at high stress, strain rate > exponentiallyat low stress, strain rate is low (3) Rocks as Newtonian Fluids (a) (^) as viscous materialsunder higher temps. and press., rocks may behave

  1. Plastic Behavior a. Plastic materials (1) at low stress, materials undergo elastic deformation untilcritical yield stress is exceeded (yield strength)

(2) yield stress: critical stress (strength) of material, beyondwhich material undergoes permanent deformation (a) stress < yield strength = elastic deformation relations (linear, recoverable strain) (b) stress > yield strength = plastic deformation relations (non-linear, non-recoverable strain) i) material flow, ductile deformation

  1. Compound Behavior (Other continuum models) a. Visco-elastic (Maxwell solid) b. Elastic-elastic (Prandtl Material) c.d. Visco-plastic (Bingham Material)Firmo-viscous

II. Experimental Studies A. Overview and Philosophy of Rheologic Experimentation

  1. Procedures a. stress-strain diagram generation b. variables: temperature, pressure, material composition
  2. Mathematical Analysis

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