Elastic Deformation of Materials Flashcards
How can we get from displacement to strain?
Differentiate
How can we change strain for stress?
With Hooke’s law.
If displacement is constant everywhere is there any strain?
No, the body has been translated.
Define tensor shear strain.
Check
Write out the general strain tensor.
Check
Is the strain tensor symmetric?
Yes
Is stress a tensor property of a material?
Yes
Give an equation for stress using stress as a tensor.
F = ∑sigma A
By resolving the turning moment on a small element cube, show that sigmaij=sigmaji.
Check
Give an expression for hydrostatic stress in terms of normal stress.
Check
Give an expression for hydrostatic pressure of a body in terms of normal stress.
Check (should be minus the hydrostatic stress).
Note, not the same as external pressure
Relate stress and strain using the fact that the stress and strain tensors are symmetric.
Check, should get the compliance matrix.
When working with the compliance matrix, are the shear strains simple or pure?
Simple, so must convert to pure for Mohr’s circle.
State the Hooke’s law equations relating strain and stress by superposition of stress.
Check
Derive the Hooke’s law relation between stress and sum of strains.
Check
Give the Hooke’s law relation between stress and sum of strains.
Check
In the Hooke’s law relation between stress and sum of strains, does epsilon mm have any physical meaning?
Yes, it is the fractional change in volume.
Derive an expression for bulk modulus using Hooke’s law and hydrostatic pressure.
Check
Show how for Hooke’s law relating shear stress and strain, Mohr’s circle can be used to turn it into a normal stress and strain problem.
Show.
Derive the stress equilibrium equations.
Check
Why do we need strain compatibility equations?
There are 6 components of strain at every point.
There are 3 components of displacement at every point.
The strain components then cannot be independent.
Derive a strain compatibility equation.
Check