Understanding the Cauchy Stress Tensor for Beginners

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The first index in the Cauchy stress tensor indicates the direction of the normal to the surface on which the stress acts, while the second index represents the direction of the stress itself. For example, σ_xy signifies stress acting in the y direction on a plane normal to the x direction. The stress tensor is symmetric, meaning σ_xy equals σ_yx, which is necessary to avoid infinite angular accelerations in an infinitesimal element. This symmetry condition is typically valid under certain conditions, such as when the Knudsen number approaches 1. Understanding these relationships is crucial for analyzing stress states in materials.
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Hello,

I am not sure what the first indice in the cauchy stress tensor indicates

For example,


σ_xy means that the stress in the y direction, but does x mean the cross sectional area is normal to the x direction?
 
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I can't see how σ_xy is dependent on σ_yx, they are perpendicular to each other
 
Who said anything about these stresses being dependent on one another?
 
My textbook said that the entire stress state can be determined with just 6 of the 9 components of the stress tensor. Is that to mean something different than there is a dependency? Or even they are equal?
 
The Cauchy stress tensor must be SYMMETRIC.
The reason for this is apparent when you consider the TORQUES about an infinitesemal square element.
Unless the stress tensor is symmetric, you'll get infinite angular accelerations of the square element.

The symmetry condition on the stress tensor explains why s_xy=s_yx and so on.

It should be mentioned, as is done in the Wikipedia article, that the symmetry of the Cauchy stress tensor is a special case as the Knudsen number goes to 1, so that symmetry is not required generally
 
Woopydalan said:
Hello,

I am not sure what the first indice in the cauchy stress tensor indicates

For example,


σ_xy means that the stress in the y direction, but does x mean the cross sectional area is normal to the x direction?

Yes. There are three components of the stress vector acting on a plane oriented normal to the x direction. The (normal) component in the x direction is σxx. The (shear) component in the y direction is σxyyx. The (shear) component in the z direction is σxzzx.
 
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