Questions about derivation of equation

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    Derivation
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Discussion Overview

The discussion revolves around the derivation of a specific equation related to linear elasticity, focusing on the relationships between various strain components. Participants are exploring the mathematical relationships and procedures necessary to derive the equation from given definitions of strain.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant expresses difficulty in deriving the equation involving the second derivative of strain components.
  • Another participant suggests expanding the equation using the definitions of strain to simplify it, indicating that some terms will cancel out.
  • A participant questions the absence of displacement variables (U) in the final equation derived from the strain relationships.
  • Concerns are raised about the use of cyclic indices in the derivation process, with a preference for understanding the derivation without them.
  • Some participants speculate on the historical context of how the equation might have been developed, suggesting it arose from assumptions about shear strains.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the derivation process, with multiple viewpoints on the use of cyclic indices and the necessity of understanding the derivation without them. The discussion remains unresolved regarding the exact procedure for deriving the equation without cyclic indices.

Contextual Notes

Participants express uncertainty about the derivation steps and the implications of using cyclic indices. There is a lack of clarity on how to derive related equations for different strain components using the provided definitions.

roldy
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I'm studying linear elasticity and I came across an equation that I having problems figuring out the derivation. I want to understand this in case I may need to know it later in the course. The equation is as follows:

\frac{\partial^2e_{zz}}{\partial x \partial y} = \frac{\partial}{\partial z}\left(\frac{\partial e_{yz}}{\partial x} + \frac{\partial e_{zx}}{\partial y} - \frac{\partial e_{xy}}{\partial z}\right)

I'm trying to understand this derivation with the given relationships below.

e_{xx} = \frac{\partial U_x}{\partial x}
e_{yy} = \frac{\partial U_y}{\partial y}
e_{zz} = \frac{\partial U_z}{\partial z}

e_{xy} = 1/2\left(\frac{\partial U_y}{\partial x} + \frac{\partial U_x}{\partial y}\right)
e_{yz} = 1/2\left(\frac{\partial U_z}{\partial y} + \frac{\partial U_y}{\partial z}\right)
e_{zx} = 1/2\left(\frac{\partial U_x}{\partial z} + \frac{\partial U_z}{\partial x}\right)

The only thing that makes sense is that the derivative with respect to x and y was taken on e_{zz}.
 
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hi roldy! :smile:

if you expand \left(\frac{\partial e_{yz}}{\partial x} + \frac{\partial e_{zx}}{\partial y} - \frac{\partial e_{xy}}{\partial z}\right) by using those definitions,

you'll get 6 terms, of which 4 should cancel :wink:
 
I understand that. The problem I'm having is deriving the first equation from the other equations.
 
ok, so what did you get when you expanded \left(\frac{\partial e_{yz}}{\partial x} + \frac{\partial e_{zx}}{\partial y} - \frac{\partial e_{xy}}{\partial z}\right) ? :smile:
 
I would get \frac{\partial^2 e_{zz}}{\partial x \partial y} after simplifying. The question that I have is how to get the other relationships (without using cyclic indices) for \frac{\partial^2 e_{xx}}{\partial y \partial z} and \frac{\partial^2 e_{yy}}{\partial z \partial x} just by using the equations below. What is the procedure?

e_{xy} = 1/2\left(\frac{\partial U_y}{\partial x} + \frac{\partial U_x}{\partial y}\right)
e_{yz} = 1/2\left(\frac{\partial U_z}{\partial y} + \frac{\partial U_y}{\partial z}\right)
e_{zx} = 1/2\left(\frac{\partial U_x}{\partial z} + \frac{\partial U_z}{\partial x}\right)
 
(just got up :zzz:)
roldy said:
I would get \frac{\partial^2 e_{zz}}{\partial x \partial y} after simplifying.

i don't understand :redface:

why is there no U in there? :confused:
 
Why are you opposed to cycling the indices?
 
There is no U in the final equation because I end up with \frac{\partial^3 U_z}{\partial x \partial y \partial z} which when letting e_{zz} = \frac{\partial U_{zz}}{\partial z} the solution becomes \frac{\partial e_{zz}}{\partial x \partial y}

I'm opposed to using cyclic indices because I would like to know how this equation came to be. Sure, I could use cyclic indices for the other equations but if I am asked on a test to derive this relationship without cyclic indices I wouldn't know where to begin.
 
roldy said:
There is no U in the final equation because I end up with \frac{\partial^3 U_z}{\partial x \partial y \partial z} which when letting e_{zz} = \frac{\partial U_{zz}}{\partial z} the solution becomes \frac{\partial e_{zz}}{\partial x \partial y}

I'm opposed to using cyclic indices because I would like to know how this equation came to be. Sure, I could use cyclic indices for the other equations but if I am asked on a test to derive this relationship without cyclic indices I wouldn't know where to begin.
So your real question is "How did anyone ever think of this?" I think you already know the answer. What's your best guess? Incidentally, I've had more than a nodding acquaintance with stress analysis during my career, and I don't ever remember any practical application where this type of relationship was used.
 
  • #10
You are correct. I know we need this equation for constraining requirements. My best guess is that "they" assumed a relationship with all the shear strains. Then they figured out whether or not a particular shear strain is added or subtracted.
 
  • #11
roldy said:
You are correct. I know we need this equation for constraining requirements. My best guess is that "they" assumed a relationship with all the shear strains. Then they figured out whether or not a particular shear strain is added or subtracted.
I think that some person was just sitting around "playing" around with the equations, as many of us often do, and they came up with this result (which they found very interesting).
 

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