normal stresses

9
Stress Tensor Stress Tensor

description

mohar circle, principle stresses ,principle planes

Transcript of normal stresses

Page 1: normal stresses

Stress TensorStress Tensor

Page 2: normal stresses

Normal StressNormal Stress

A stress measures the A stress measures the surface force per unit area.surface force per unit area.• Elastic for small changesElastic for small changes

A normal stress acts normal A normal stress acts normal to a surface.to a surface.• Compression or tensionCompression or tension

F

A

A

Ft

F

A

x

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Shear StressShear Stress

A shear stress acts parallel A shear stress acts parallel to a surface.to a surface.• Also elastic for small Also elastic for small

changeschanges

Ideal fluids at rest have no Ideal fluids at rest have no shear stress.shear stress.• SolidsSolids

• Viscous fluidsViscous fluids

F

A

x

A (goes into screen)

L

F

A

Ft

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Volume StressVolume Stress

Fluids exert a force in all Fluids exert a force in all directions.directions.• Same force in all directionsSame force in all directions

The force compared to the The force compared to the area is the pressure.area is the pressure.

F

A

A

FP

F

F

P

V

V

A (surface area)

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Surface ForceSurface Force

Any area in the fluid Any area in the fluid experiences equal forces experiences equal forces from each direction.from each direction.• Law of inertiaLaw of inertia

• All forces balancedAll forces balanced

Any arbitrary volume in the Any arbitrary volume in the fluid has balanced forces.fluid has balanced forces.

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Force PrismForce Prism

Consider a small prism of Consider a small prism of fluid in a continuous fluid.fluid in a continuous fluid.• Stress vector Stress vector tt at any point at any point

• Normal area vectors Normal area vectors SS form form a trianglea triangle

The stress function is linear.The stress function is linear.

1Sd

2Sd

21 SdSd

)( 2Sdt

)( 1Sdt

)( 21 SdSdt

)()( SdtcScdt

)()( SdtSdt

)()()( 2121 SdSdtSdtSdt

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Stress TensorStress Tensor

Represent the stress Represent the stress function by a tensor.function by a tensor.• Normal vector Normal vector n = dSn = dS

• TTijij component acts on component acts on

surface elementsurface element

The components transform The components transform like a tensor.like a tensor.• Transformation Transformation ll

• Dummy subscript changesDummy subscript changes

),(),,( txTnSdtxt ijij

ijij Tnt

ijqqippj Tnltl

ijqqiipipj TnlTnl

ijqqirjipipjrj TnllTnll

ijqqirjiriipirp TnllTnTn

ijrjqiqqrq TllnTn ijrjqiqr TllT

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Symmetric FormSymmetric Form

The stress tensor includes The stress tensor includes normal and shear stresses.normal and shear stresses.• Diagonal normalDiagonal normal• Off-diagonal shearOff-diagonal shear

An ideal fluid has only pressure.An ideal fluid has only pressure.• Normal stressNormal stress• IsotropicIsotropic

A viscous fluid includes shear.A viscous fluid includes shear.• Symmetric Symmetric • 6 component tensor6 component tensor

ijij PT

33231

23221

13121

T

jiij TT

32313

23212

13121

T

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Force DensityForce Density

The total force is found by The total force is found by integration.integration.• Closed volume with Gauss’ Closed volume with Gauss’

lawlaw

• Outward unit vectorsOutward unit vectors

A force density due to stress A force density due to stress can be defined from the can be defined from the tensor.tensor.• Due to differences in stress Due to differences in stress

as a function of positionas a function of position

S

dSnF ˆT

V

dVF T

PSf

S

SdF

T

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