Question

2. In the absence of body forces, do the following stress components satisfy the equations of equilibrium? 011 = a [až +v (zł

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Answer #1

Solution:

Given that:

011 = a 22 [23 +v(21 - 23)

\sigma _{22}=\alpha \left [ x_{1}^{2}+\nu\left ( x_{2}^{2}-x_{1}^{2} \right )\right ]

\sigma _{33}=\alpha \nu \left ( x_{1}^{2}+x_{2}^{2} \right )

\sigma _{12}=\sigma _{21}=-2\alpha \nu x_{1}x_{2}

\sigma _{13}=\sigma _{31}=0

\sigma _{23}=\sigma _{32}=0

\sigma =\begin{bmatrix} \sigma _{x} &\tau _{xy} &\tau _{xz} \\ \tau _{xy} & \sigma _{y} & \tau _{yz} \\ \tau _{xz} &\tau _{yz} & \sigma _{z} \end{bmatrix}

Equlibrium equation:

\frac{\partial \sigma _x}{\partial x_{1}}+\frac{\partial \tau _{xy}}{\partial x_{2}}+\frac{\partial \tau _{xz}}{\partial x_{3}}=0\, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \rightarrow 1

\frac{\partial \tau _{xy} }{\partial x_{1}}+\frac{\partial \sigma _{y} }{\partial x_{2}}+\frac{\partial \tau _{yz}}{\partial x_{3}}=0\, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \rightarrow 2

\frac{\partial \tau _{xz} }{\partial x_{1}}+\frac{\partial \tau _{yz} }{\partial x_{2}}+\frac{\partial \sigma _{z}}{\partial x_{3}}=0\, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \, \rightarrow 3

\sigma =\begin{bmatrix} \alpha \left [ x_{2}^{2}+\nu\left ( x_{1}^{2}-x_{2}^{2} \right )\right ]& -2\alpha\nu x_{1}x_{2} & 0\\ -2\alpha\nu x_{1}x_{2}&\alpha[x_{1}^{2}+\nu (x_{2}^{2}-x_{1}^{2})] & 0\\ 0 &0 &\alpha \nu (x_{1}^{2}+x_{2}^{2}) \end{bmatrix}

Equation 1 will be:

2\alpha\nu x_{1}-2\alpha\nu x_{1}=0

Equation 2 will be:

-2\alpha\nu x_{2}+2\alpha\nu x_{2}=0

Equation 3 will be:

0+0+0=0

Hence stress tensor satisfying the equilibrium equations.

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