Is stress tensor a 3x3 or 3x3x3 tensor?

AI Thread Summary
The discussion centers on the nature of the mechanical stress tensor, questioning whether it is a 3x3 tensor or a 3x3x3 tensor of scalars. It is clarified that the stress tensor is indeed a 3x3 tensor, with its nine entries representing scalar values, while diagrams often illustrate these values as vectors indicating force directions on a block's faces. The notation σ11 signifies the magnitude of the force component in a specific direction, emphasizing that stress is defined as force per unit area. The conversation confirms that stress and strain are both represented as 3x3 tensors. Overall, the stress tensor is understood to be a 3x3 tensor, with the vector representations in diagrams serving to illustrate force components.
Hassan2
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Hi all,

I have a fundamental question about ( mechanical) stress tensor. Stress tensor a 3x3 tensor whose 9 entries looks "scalars" but in figures, the stress is illustrated by nine "vectors". Does it mean the stress tensors is in fact a 3x3x3 tensor of scalars whose nonzero entries are ignored?
 
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Stress and strain are definitely 3x3 tensors.

If you mean diagrams of a rectangular block with arrows attached to the faces, the arrows are showing the direction of the forces acting on the face, i.e. the components of ##\sigma \cdot \bf{n}## where ##\bf{n}## is the normal vector to the face.

If you meant some other diagram, can you post a link to it?
 
Yes those diagrams that you mentioned. So when they write σ11 beside one of the arrows, the arrow is the force component in that defined direction andσ11 tells us about "magnitude" of the force. However it seems to be the force per unit area, otherwise the stress must be multiplied by the surface.

Thanks.
 
Hassan2 said:
So when they write σ11 beside one of the arrows, the arrow is the force component in that defined direction andσ11 tells us about "magnitude" of the force. However it seems to be the force per unit area, otherwise the stress must be multiplied by the surface.
Correct.
 
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