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