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Stress and strain
StrainLecture 3 โ deformation, strain
Mechanical Engineering Design - N.Bonora 2018
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Stress and strain
Introduction
โข Real bodies are deformable
โข Under the action of an external loading, the body transforms from a reference configurationto a current configuration.
โข A โconfigurationโ is a set containing the positions of all particles of the body
โข This transformation is called: deformation.
A deformation may be caused by:
โข external loads,
โข body forces (such as gravity or electromagnetic forces),
โข changes in temperature, moisture content, or chemical reactions, etc.
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Deformation of a thin rope
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Stress and strain
Deformation vs strain
โข Strain is a measure of deformation representing the displacement between particles in the body relative to a reference length.
โข In a continuous body, a deformation field results from a stress field induced by applied forces or is due to changes in the temperature field inside the body.
โข The relation between stresses and induced strains is expressed by constitutive equations, e.g., Hooke's law for linear elastic materials.
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Deformation of a thin rope
Lf
L0
L0
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Stress and strain
Deformation and strain
โข Strain is a measure of deformation representing the displacement between particles in the body relative to a reference length.
โข A general deformation of a body can be expressed in the form x=F(X), where X is the reference position of the body
โข This definition does not distinguish between rigid body motions (translations and rotations) and changes in shape (and size) of the body
โข Strains are dimensionless
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Deformation of a thin rope
L0
๐บ =๐
๐๐ฟ๐ โ ๐ฟ = ๐ญโฒ โ ๐ฐ
Lf
L0
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Stress and strain
Strain measures
โข Depending on the amount of strain, three main theories are for the analysis of deformation:
โข Infinitesimal strain theory
โข Finite strain theory
โข Large-displacement (large rotation) theory
Mechanical Engineering Design - N.Bonora 2018
Deformation of a thin rope
L0
Lf
L0
![Page 6: Lecture 1 - Introduzioneย ยท 1 2 ๐2โ๐ 0 2 ๐0 2 ... Lecture 1 - Introduzione Author: Nicola Bonora Created Date: 11/16/2018 10:53:43 AM](https://reader034.vdocument.in/reader034/viewer/2022042404/5f1ae0103e6ac2217474bbf9/html5/thumbnails/6.jpg)
Stress and strain
Strain measures
โข Infinitesimal strain theory
โข Also called small strain theory, small deformation theory, small displacement theory, or small displacement-gradient theory.
โข Strains and rotations are both small. The undeformed and deformed configurations of the body can be assumed identical.
โข The infinitesimal strain theory is used in the analysis of deformations of materials exhibiting elastic behavior, such as materials found in mechanical and civil engineering applications, e.g. concrete and steel.
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L0
๐ฟ๐ = ๐ฟ๐ + ฮ๐ฟ
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Stress and strain
Strain measures
โข Finite strain theory
โข also called large strain theory, large deformation theory
โข Deals with deformations in which both rotations and strains are arbitrarily large. In this case, the undeformed and deformed configurations of the continuum are significantly different and a clear distinction has to be made between them.
โข This is commonly the case with elastomers, plastically-deforming materials and other fluids and biological soft tissue.
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L0
๐ฟ๐
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Stress and strain
Strain measures
โข Large strain theory
โข Large-displacement or large-rotation theory, which assumes small strains but large rotations and displacements.
Mechanical Engineering Design - N.Bonora 2018
L0
๐ฟ๐
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Stress and strain
Strain measures
โข In each theory the definition of strain is different
โข Engineering strain. The Cauchy strain or engineering strain is expressed as the ratio of total deformation to the initial dimension of the material body in which the forces are being applied.
โข Engineering normal strain of a material line element or fiber axially loaded is given by the change in length ฮL per unit of the original length L of the line element or fibers. The normal strain is positive if the material fibers are stretched and negative if they are compressed.
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ํ =๐ฟ๐ โ ๐ฟ0
๐ฟ0
๐ฟ๐
๐ฟ0
๐ฟ๐ โ ๐๐ฅ +๐๐ข
๐๐ฅ๐๐ฅ
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Stress and strain
Strain measures
โข In each theory the definition of strain is different
โข Engineering strain. The Cauchy strain or engineering strain is expressed as the ratio of total deformation to the initial dimension of the material body in which the forces are being applied.
โข Engineering shear strain is defined as the change in angle between lines AC and AB.
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๐พ๐ฅ๐ฆ =๐๐ข๐ฆ
๐๐ฅ+๐๐ข๐ฅ๐๐ฆ
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Stress and strain
Strain measures
โข Different definitions
โข Engineering strain:
โข True engineering strain
โข Green strain
โข Almansi strain
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ํ๐๐๐ =ฮ๐
๐0
ํ = ๐๐
๐= ๐๐ 1 +
ฮ๐
๐0
ํ๐บ =1
2
๐2 โ ๐02
๐02
ํ๐บ =1
2
๐2 โ ๐02
๐2
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Stress and strain
Examples of homogeneous deformation
Straight lines remain straight, parallel lines remains parallel
โข uniform extension
โข pure dilation
โข simple shear
โข pure shear
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ํ =ํ 00 ํ
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Stress and strain
Strain tensor
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STRAIN TENSOR (infinitesimal deformations). A tridimensional deformation state is described by the strain tensor e
Same properties as for the stress tensor: strain invariants
ํ๐๐ =
ํ11 ํ12 ํ13ํ21 ํ22 ํ23ํ31 ํ32 ํ33
๐ผ1 = ํ11 + ํ22 + ํ33
๐ผ2 = ํ11ํ22 + ํ22ํ33 + ํ33ํ11 โ ํ122 โ ํ23
2 โ ํ312
๐ผ3 = ๐๐๐ก ํ๐๐
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Stress and strain
Strain tensor
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PRINCIPAL STRAIN. At every point in a deformed body there are at least three planes, called principal planes, with normal vectors, called principal directions, where the corresponding strain vector is perpendicular to the plane and where there are no shear strain.
The three strain normal to these principal planes are called principal strains.
ํ๐๐ =
ํ11 0 00 ํ22 00 0 ํ33
VOLUMETRIC STRAIN. The dilatation (the relative variation of the volume) is the trace of the tensor:
ํ๐๐ = ๐ฟ =ฮ๐
๐0= ํ11+ํ22+ํ33
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Stress and strain
Strain tensor
Mechanical Engineering Design - N.Bonora 2018
PRINCIPAL STRAIN. At every point in a deformed body there are at least three planes, called principal planes, with normal vectors, called principal directions, where the corresponding strain vector is perpendicular to the plane and where there are no shear strain.
The three strain normal to these principal planes are called principal strains.
ํ๐๐ =
ํ11 0 00 ํ22 00 0 ํ33
STRAIN DEVIATOR. The infinitesimal strain tensor, similarly to the Cauchy stress tensor, can be expressed as the sum of two other tensors. The strain deviator account for distortion.
ํ๐๐ = ํโฒ๐๐ +1
3ํ๐๐๐ฟ๐๐
ํโฒ๐๐ =โก
ํ11 โ ๐ฟ ํ12 ํ13ํ21 ํ๐ฆ โ ๐ฟ ํ23ํ31 ํ32 ํ๐ง โ ๐ฟ
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Stress and strain
Strain tensor
Mechanical Engineering Design - N.Bonora 2018
OCTAHEDRAL STRAINS. An octahedral plane is one whose normal makes equal angles with the three principal directions.
The engineering shear strain on an octahedral plane is called the octahedral shear strain and is given by
๐พ๐๐๐ก =2
3ํ1 โ ํ2
2 + ํ2 โ ํ32 + ํ3 โ ํ1
2
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Stress and strain
Strain tensor: special cases
Mechanical Engineering Design - N.Bonora 2018
PLANE STRAIN. The plane strain condition is when there are no shear strain in any plane normal to the plane considered and the strain component normal to such plane is zero
ํ๐๐ =ํ11 ํ12 0ํ21 ํ22 00 0 0
ANTIPLANE STRAIN. This state of strain is achieved when the displacements in the body are zero in the plane of interest but nonzero in the direction perpendicular to the plane.
ํ๐๐ =
0 0 ํ130 0 ํ23ํ31 ํ32 0
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Stress and strain
Symmetry and additivity
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Stress and strain
Symmetry and additivity
Mechanical Engineering Design - N.Bonora 2018
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Stress and strain
STRAIN RATE
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Engineering strain rate
True strain rate
ํ๐๐๐ =๐ํ๐๐๐
๐๐ก=๐
๐๐ โ ๐0๐0๐๐ก
=1
๐0
๐๐
๐๐ก=
๐ฃ
๐0
ํ ==๐ ๐๐
๐๐0
๐๐ก=1
๐
๐๐
๐๐ก=๐ฃ
๐
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Stress and strain
Suggested readings
โข http://www.mech.utah.edu/~brannon/public/Mohrs_Circle.pdf
โข Schaum's Outline of Strength of Materials, Fifth Edition (Schaum'sOutline Series) Fifth (5th) Edition Paperback โ September 12, 2010
โข Strength of Materials (Dover Books on Physics) Reprinted Edition by J. P. Den Hartog, ISBN-10: 0486607550
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