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The Mohr Stress Diagram

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<strong>The</strong> <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong><br />

Edvard Munch as a young geologist!


<strong>The</strong> <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong><br />

A means by which two stresses acting on a plane of known<br />

orientation can be plotted as the components of normal and<br />

shear stresses (derived separately from each of the two stresses).<br />

<strong>The</strong> <strong>Mohr</strong> circle is thus an elegant way to determine the shear and<br />

normal stresses for a pair of stresses oriented obliquely to the plane<br />

in question. <strong>The</strong> <strong>Mohr</strong> circle allows you to quickly read this for<br />

planes of any orientation.<br />

It also makes it easy to visualize mean stress and differences in<br />

stress, or deviatoric stress and relate these to deformation.


Setting up the Problem (we did this previously for one stress)


Add another stress & calculate their normal and shear components<br />

<strong>The</strong> angle theta is the angle between the maximum !<br />

principle stress and the plane it is acting on…


Decompose two original stresses into their x and y components!<br />

After several trigonometric and algebraic manipulations,<br />

the two equations left are ……


<strong>Stress</strong> Equations<br />

Two perpendicular stresses oriented at any<br />

angle to a plane!<br />

Normal <strong>Stress</strong><br />

σ n = (σ 1 + σ 3 ) - (σ 1 - σ 3 ) cos 2Θ!<br />

2!<br />

2!<br />

Shear <strong>Stress</strong><br />

σ s = (σ 1 - σ 3 ) sin 2Θ!<br />

2!


<strong>The</strong> <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong><br />

σ n = (σ 1 + σ 3 ) - (σ 1 - σ 3 ) cos 2Θ!<br />

2!<br />

2!<br />

<strong>The</strong>ta = angle between !<br />

the maximum stress and<br />

the plane it is acting on.!<br />

σ s = (σ 1 - σ 3 ) sin 2Θ!<br />

2!


<strong>The</strong> <strong>Mohr</strong> Circle - (mean or average stress)<br />

Mean <strong>Stress</strong>!


<strong>The</strong> <strong>Mohr</strong> Circle – radius or deviatoric stress<br />

Deviatoric <strong>Stress</strong>!


<strong>The</strong> <strong>Mohr</strong> Circle – diameter or differential stress<br />

Differential <strong>Stress</strong>!


Laboratory Experiments in Rock Deformation<br />

Deformed marble rock cylinders


Laboratory Experiments in Rock Deformation<br />

<strong>Stress</strong> a rock sample until it fractures (or flows)


In-class exercise, work in groups of 4, turn in write up of answers.<br />

Given these samples, discuss how the magnitude of stresses likely<br />

varied relative to one another in these four experiments. Each<br />

cylinder was deformed in a different experiment, each with its<br />

own axial and radial load (which varied relative to one another).


In-class problem!<br />

1. For maximum and minimum stresses of 600 and 200<br />

mega-pascals (MPa) oriented as a vertical vector and a<br />

horizontal, E-W striking vector (respectively), determine<br />

the normal and shear stresses on a plane oriented North-<br />

South, 45 degrees East. It helps to first draw a block<br />

diagram.<br />

2. So max stress is oriented vertically and equal to 600 MPA<br />

3. Min stress is horizontal, oriented east-west and = 200 MPa


In-class problem!<br />

<strong>The</strong>re are two ways to solve these problems.<br />

Use the <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong> or<br />

Use the equations<br />

(extra credit if you do both…)


Determine the normal and shear stresses on a plane oriented N-S, 45 o E<br />

Maximum stress is oriented vertically and equal to 600 MPA<br />

Minimum stress is horizontal, oriented east-west and = 200 MPa<br />

Use the <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong>!


For maximum and minimum stresses of 600 and 200 (MPa) oriented as<br />

a vertical vector and a horizontal, E-W striking vector (respectively),<br />

determine the normal and shear stresses on a plane oriented North-<br />

South, 45 degrees East. It helps to first draw a block diagram.<br />

Use the Equations!<br />

σ n = (σ 1 + σ 3 ) - (σ 1 - σ 3 ) cos 2Θ!<br />

2!<br />

2!<br />

σ s = (σ 1 - σ 3 ) sin 2Θ!<br />

2!<br />

For the minimum and maximum principle stresses of 600 and 200<br />

megapascals (MPa) oriented as a vertical vector and a horizontal,<br />

E-W striking vector (respectively), determine the normal and shear<br />

stresses on a plane oriented North-South, 45 degrees East


2 For the stress state in the previous problem, determine the differential<br />

stress and mean stress. Start by plotting the solution for normal and<br />

shear stresses on the <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong>.<br />

Problem 2!<br />

3 Determine whether decreasing the dip of the fault will decrease or<br />

increase the shear stress acting on it.<br />

4 Discuss how a change in differential stress might affect whether a<br />

rock might be more or less likely to break. It may help by arbitrarily<br />

varying the stresses and looking at how they plot on the circle, or by<br />

imagining stress on a cube.<br />

5 Now discuss whether increasing the mean stress would cause a rock<br />

to break more readily. Would this be more or less likely with<br />

increasing depth in the crust<br />

6 Draw the stress state where the minimum and maximum stresses are<br />

both equal to 600 Mpa.


Following set of slides should be copied and handed out to students for<br />

exercises. Work in groups of 4, so for a class of 80 students, print out 20<br />

sets.


In-class exercise, work in groups of 4 & turn in a write up of your answers.<br />

Problem 1.1 Given these samples, discuss how the magnitude and<br />

mean stresses likely varied relative to one another in these four samples.<br />

Each cylinder was deformed in a different experiment, each with its<br />

own axial and radial load (which varied relative to one another).


In-class problem 1.2<br />

For maximum and minimum stresses of 600 and 200 megapascals<br />

(MPa) oriented as a vertical vector and a horizontal, E-<br />

W striking vector (respectively), determine the normal and shear<br />

stresses on a plane oriented North-South, 45 degrees East. It<br />

helps to first draw a block diagram.<br />

So max stress is oriented vertically and equal to 600 MPA<br />

Min stress is horizontal, oriented east-west and = 200 MPa


For maximum and minimum stresses of 600 and 200 megapascals<br />

(MPa) oriented as a vertical vector and a horizontal, E-W striking<br />

vector (respectively), determine the normal and shear stresses on a<br />

plane oriented North-South, 45 degrees East. It helps to first draw a<br />

block diagram.<br />

Use the Equations!<br />

σ n = (σ 1 + σ 3 ) - (σ 1 - σ 3 ) cos 2Θ!<br />

2!<br />

2!<br />

σ s = (σ 1 - σ 3 ) sin 2Θ!<br />

2!


Or use the <strong>Mohr</strong> Circle!


For the stress state in the previous problem, determine the differential<br />

stress and mean stress. Start by plotting the solution for normal and shear<br />

stresses on the <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong>.<br />

Determine whether decreasing the dip of the fault will decrease or<br />

increase the shear stress acting on it.<br />

Discuss how a change in differential stress might make the sample more<br />

or less likely to break. It may help by arbitrarily varying the stresses and<br />

looking at how they plot on the circle, or by imagining stress on a cube.<br />

Now discuss whether increasing just the mean stress would cause a rock<br />

to break more readily. Would this be more or less likely with increasing<br />

depth in the crust<br />

Draw the stress state where the minimum and maximum stresses are both<br />

equal to 600 MPa. What is the differential stress. Would you expect the<br />

rock to deform under these conditions


In-class problem 2.2<br />

1. For the stress state in the previous problem, determine the<br />

differential stress and mean stress. Start by plotting the<br />

solution for normal and shear stresses on the <strong>Mohr</strong> <strong>Stress</strong><br />

<strong>Diagram</strong>.


In-class problem 2.3<br />

1. Determine whether decreasing the dip of the fault will<br />

decrease or increase the shear stress acting on it.


In-class problem 2.4<br />

Discuss how a change in differential stress might make the<br />

sample more or less likely to break. It may help by<br />

arbitrarily varying the stresses and looking at how they<br />

plot on the circle, or by imagining stress on a cube.


In-class problem 2.5<br />

1. Now discuss whether increasing the mean stress would cause<br />

a rock to break more readily. Would this be more or less likely<br />

with increasing depth in the crust


In-class problem 2.6<br />

1. Draw the stress state where the minimum and maximum<br />

stresses are both equal to 600 Mpa. What is the differential<br />

stress Would you expect the rock to deform under these<br />

conditions


In-class problem 2<br />

For the stress state in the previous problem, determine the differential stress<br />

and mean stress. Start by plotting the solution for normal and shear stresses<br />

on the <strong>Mohr</strong> <strong>Stress</strong> <strong>Diagram</strong>.<br />

Determine whether decreasing the dip of the fault will decrease or increase<br />

the shear stress acting on it.<br />

Discuss how a change in differential stress might make the sample more or<br />

less likely to break. It may help by arbitrarily varying the stresses and looking<br />

at how they plot on the circle, or by imagining stress on a cube.<br />

Now discuss whether increasing just the mean stress would cause a rock to<br />

break more readily. Would this be more or less likely with increasing depth in<br />

the crust<br />

Draw the stress state where the minimum and maximum stresses are both<br />

equal to 600 Mpa. What is the differential stress. Would you expect the rock<br />

to deform under these conditions

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