A Stress tensor and pressure relationship

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The discussion revolves around understanding the notation and concepts in Currie's "Fundamental Mechanics of Fluids." There is confusion regarding the expression for the force acting in the x2 direction, specifically the relationship between the stress vector components and the normal vector. Clarifications indicate that the normal vector is a component of a vector rather than a vector itself, and the components of the stress vector on a surface are defined in terms of the stress tensor. The author’s simplification of notation is criticized for being unhelpful, leading to misunderstandings. Overall, the conversation emphasizes the importance of accurately interpreting vector components in fluid mechanics.
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I'm studying with Currie's Fundamental Mechanics of Fluids, Fourth edition.
I'm confusing with the above statement; the force acting in the x2 direction is P2=s12n1 which is n1 direction.
Is there anybody help me to understand this subject?
 
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Seyn said:
the force acting in the x2 direction is P2=s12n1 which is n1 direction.
No, ##P_2=\sigma_{12}n_1## is the second component of a vector. That vector is the result of multiplying your original normal vector by a matrix, so can be in an arbitrary direction. Its second component is the component in the direction of your second basis vector.

Note that I think the author has tried to simplify the notation slightly, and I think he's done it in an unhelpful way. The point is that there's a normal vector ##\vec n## which he has chosen to be parallel to the first basis vector, so in component form it is ##(n_1,0,0)^T##. So I'd say that "the unit normal vector ... is ##n_1##" is possibly confusing the issue - ##n_1## is a component of a vector (in this case, the only non-zero component, but still only a component), not a vector itself.
 
Ibix said:
No, ##P_2=\sigma_{12}n_1## is the second component of a vector. That vector is the result of multiplying your original normal vector by a matrix, so can be in an arbitrary direction. Its second component is the component in the direction of your second basis vector.

Note that I think the author has tried to simplify the notation slightly, and I think he's done it in an unhelpful way. The point is that there's a normal vector ##\vec n## which he has chosen to be parallel to the first basis vector, so in component form it is ##(n_1,0,0)^T##. So I'd say that "the unit normal vector ... is ##n_1##" is possibly confusing the issue - ##n_1## is a component of a vector, not a vector itself.
Do you mean the point is,
##\vec{P}=(P_1,P_2,P_3)## and,
##P_j=\sigma_{ij}n_i##
so
##\vec{P}=\sigma_{ij}n_i \hat{e_j}##??
 
Ibix said:
Yes.
Thank you for your kind explanation!
 
You are confused because the result the author gives is wrong. A unit vector in the 1 direction is (1,0,0). The components of the stress vector on the surface of constant x (i.e., 1) are ##P_1=\sigma_{ 11}##, ##P_2=\sigma_{ 12}##, and ##P_3=\sigma_{ 13}##. So the stress vector is ##(P_1,P_2,P_3)=(\sigma_{11},\sigma_{12},\sigma_{13})##
 
Chestermiller said:
You are confused because the result the author gives is wrong. A unit vector in the 1 direction is (1,0,0). The components of the stress vector on the surface of constant x (i.e., 1) are ##P_1=\sigma_{ 11}##, ##P_2=\sigma_{ 12}##, and ##P_3=\sigma_{ 13}##. So the stress vector is ##(P_1,P_2,P_3)=(\sigma_{11},\sigma_{12},\sigma_{13})##
Thanks for the reply. Do you mean the term ##n_i##s are the component of arbitrary surface vector##\vec{n}##, and the author chose an unit vector in the 1 direction as the surface vector for the first example which is ##(1,0,0)##? As a result, because ##n_1=1##, ##n_2=0##, ##n_3=0##, the surface force vector is ##P_j=\sigma_{ij} n_i=(1 \cdot \sigma_{11}+0 \cdot \sigma_{21}+0 \cdot \sigma_{31},1 \cdot \sigma_{12}+0 \cdot \sigma_{22}+0 \cdot \sigma_{23},1 \cdot \sigma_{13}+0 \cdot \sigma_{23}+0 \cdot \sigma_{33})=(\sigma_{11},\sigma_{12},\sigma_{13})##??
 
Seyn said:
Thanks for the reply. Do you mean the term ##n_i##s are the component of arbitrary surface vector##\vec{n}##, and the author chose an unit vector in the 1 direction as the surface vector for the first example which is ##(1,0,0)##? As a result, because ##n_1=1##, ##n_2=0##, ##n_3=0##, the surface force vector is ##P_j=\sigma_{ij} n_i=(1 \cdot \sigma_{11}+0 \cdot \sigma_{21}+0 \cdot \sigma_{31},1 \cdot \sigma_{12}+0 \cdot \sigma_{22}+0 \cdot \sigma_{23},1 \cdot \sigma_{13}+0 \cdot \sigma_{23}+0 \cdot \sigma_{33})=(\sigma_{11},\sigma_{12},\sigma_{13})##??
yes
 
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