Finding $\mathbf{E}$ and $\mathbf{e}$ for a Deformation Field

In summary, the deformation field given by the equations x_1 = X_1 + alpha X_2, x_2 = X_2 - alpha X_1, and x_3 = X_3 can be represented as the matrix form of the tensors E and e. The circle of particles X_1^2 + X_2^2 = 1 deforms into the circle x_1^2 + x_2^2 = 1 + alpha^2, as shown by the solution for E and the calculation of C. The calculation for e may differ from the book answer, but assuming a typo, it can be shown that X_1^2 + X_2^2 = 1 de
  • #1
Dustinsfl
2,281
5
For the deformation field given by
$$
x_1 = X_1 + \alpha X_2,\quad x_2 = X_2 - \alpha X_1,\quad x_3 = X_3
$$
where ##\alpha## is a constant, determine the matrix form of the tensors ##\mathbf{E}## and ##\mathbf{e}##, and show that the circle of particles ##X_1^2+ X_2^2 = 1## deforms into the circle ##x_1^2 + x_2^2 = 1 + \alpha^2##.

How do I find ##\mathbf{e}## and the solution is
$$
\frac{1}{2(1+\alpha^2)}\begin{bmatrix}
-\alpha^2 & 0 & 0\\
0 & -\alpha^2 & 0\\
0 & 0 & 0
\end{bmatrix}
$$
First, we will find ##\mathbf{E}##.
$$
\mathbf{F} =
\begin{bmatrix}
1 & \alpha & 0\\
-\alpha & 1 & 0\\
0 & 0 & 1
\end{bmatrix}
$$
Then ##\mathbf{C} = \mathbf{F}^T\mathbf{F}##. So we have that
$$
\mathbf{C} =
\begin{bmatrix}
1 + \alpha^2 & 0 & 0\\
0 & 1 + \alpha^2 & 0\\
0 & 0 & 1
\end{bmatrix}
$$
which leads to
$$
\mathbf{E} = \frac{1}{2}
\begin{bmatrix}
\alpha^2 & 0 & 0\\
0 & \alpha^2 & 0\\
0 & 0 & 0
\end{bmatrix}.
$$
 
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  • #2
I found ##\mathbf{e} = \mathbf{F}^{-T}\mathbf{E}\mathbf{F}^{-1}## but this returns the negative of the book answer for ##\mathbf{e}##.
Assuming the book has a typo, how do I show ##X_1^2+X_2^2 = 1## deforms into ##x_1^2 + x_2^2 = 1 +\alpha^2##?
 

Related to Finding $\mathbf{E}$ and $\mathbf{e}$ for a Deformation Field

1. What is a deformation field?

A deformation field is a mathematical representation of the displacement or distortion of a space or object. It is typically used in the study of mechanics and physics to describe how a system changes over time.

2. How is the deformation field related to $\mathbf{E}$ and $\mathbf{e}$?

The deformation field is related to $\mathbf{E}$ and $\mathbf{e}$ through the stress-strain relationship in materials. $\mathbf{E}$ represents the elastic modulus, which describes the resistance of a material to deformation under stress. $\mathbf{e}$ represents the strain, or the amount of deformation that occurs in a material due to an applied stress.

3. How can I find $\mathbf{E}$ and $\mathbf{e}$ for a deformation field?

To find $\mathbf{E}$ and $\mathbf{e}$ for a deformation field, you will need to have information about the material properties, such as the Young's modulus and Poisson's ratio. You will also need to know the applied stress and the resulting strain in the material. With this information, you can use the stress-strain relationship to calculate $\mathbf{E}$ and $\mathbf{e}$.

4. What are some real-world applications of finding $\mathbf{E}$ and $\mathbf{e}$ for a deformation field?

Finding $\mathbf{E}$ and $\mathbf{e}$ for a deformation field is important in many fields, including materials science, engineering, and geology. It can be used to predict the behavior of materials under different stresses, to design structures that can withstand certain loads, and to understand the movement of tectonic plates.

5. Are there any limitations to finding $\mathbf{E}$ and $\mathbf{e}$ for a deformation field?

While finding $\mathbf{E}$ and $\mathbf{e}$ can provide valuable information about the behavior of materials, there are some limitations to this approach. It assumes that the material is linearly elastic, meaning that the relationship between stress and strain is constant. In reality, many materials exhibit non-linear behavior, which can complicate the analysis. Additionally, the stress-strain relationship may change over time due to factors such as fatigue or temperature changes.

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