Derivation problems for dilation

In summary: Therefore, in summary, if there are no body forces, the dilation (e) must satisfy the condition that the Laplacian of e is equal to zero, with the additional requirement that the divergence of the displacement vector is also equal to zero.
  • #1
roldy
237
2

Homework Statement


Show that, if there are no body forces, the dilation e ([itex] e=e_{xx} + e_{yy} + e_{zz} = div \;\vec{u}[/itex]) must satisfy the condition [itex]\nabla^2 e = 0[/itex]


Homework Equations


(1) [itex](\lambda + \mu)\frac{\partial e}{\partial x} + \mu \nabla^2U_x = 0[/itex]
(2) [itex](\lambda + \mu)\frac{\partial e}{\partial y} + \mu \nabla^2U_y = 0[/itex]
(3) [itex](\lambda + \mu)\frac{\partial e}{\partial z} + \mu \nabla^2U_z = 0[/itex]

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

[itex] e = e_{xx} + e_{yy} + e_{zz}[/itex]


The Attempt at a Solution


The homework gives hints to differentiate (1) with respect to x, (2) with respect to y, and (3) with respect to z. Then I add these up.

(1) [itex](\lambda + \mu)\frac{\partial^2 e}{\partial x^2} + \mu \nabla^2\frac{\partial U_x}{\partial x} = 0[/itex]
(2) [itex](\lambda + \mu)\frac{\partial^2 e}{\partial y^2} + \mu \nabla^2\frac{\partial U_y}{\partial y} = 0[/itex]
(3) [itex](\lambda + \mu)\frac{\partial^2 e}{\partial z^2} + \mu \nabla^2\frac{\partial U_z}{\partial z} = 0[/itex]

[itex] (\lambda + \mu)\left(\frac{\partial^2e}{\partial x}+\frac{\partial^2e}{\partial y}+\frac{\partial^2e}{\partial z}\right)+\mu(\nabla^2\frac{\partial U_x}{\partial x}+\nabla^2\frac{\partial U_y}{\partial y}+\nabla^2\frac{\partial U_z}{\partial z})=0[/itex]

[itex] (\lambda + \mu)\left(\frac{\partial^2e}{\partial x}+\frac{\partial^2e}{\partial y}+\frac{\partial^2e}{\partial z}\right)+\mu(\nabla^2e_{xx}+\nabla^2e_{yy}+\nabla^2e_{zz})=0[/itex]

[itex] (\lambda + \mu)\left(\frac{\partial^2e}{\partial x}+\frac{\partial^2e}{\partial y}+\frac{\partial^2e}{\partial z}\right)+\mu \nabla^2e=0[/itex]

[itex] (\lambda + \mu)\nabla^2e+\mu \nabla^2e=0[/itex]

From this I do not know how to arrive at the result. I can't see anything that I did wrong.

Edit:

Found my problem. The result should be

[itex] (\lambda + \mu)\nabla^2e+\mu \nabla^2 div \;\vec{U}=0[/itex]

[itex]div \;\vec{U} = 0[/itex]

Which leads me to [itex]\nabla^2 e = 0[/itex]
 
Last edited:
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  • #2
.

This is the correct result, but it is important to note that the divergence of the displacement vector (div U) must also be equal to zero in order for this condition to hold. This makes sense, as a non-zero divergence would indicate the presence of body forces, which contradicts the initial assumption.
 

FAQ: Derivation problems for dilation

What is dilation?

Dilation is a geometric transformation that changes the size of an object, but not its shape. It involves stretching or shrinking the object by a certain scale factor.

How do you perform dilation?

To perform dilation, you need to have a reference point, called the center of dilation, and a scale factor. The center of dilation is the fixed point around which the object is stretched or shrunk, and the scale factor determines the amount of stretching or shrinking. Multiply the coordinates of each point of the object by the scale factor to get the new coordinates after dilation.

What is the formula for dilation?

The formula for dilation is (x, y) → (kx, ky), where (x, y) represents the coordinates of a point on the original figure, k is the scale factor, and (kx, ky) represents the coordinates of the corresponding point on the dilated figure.

How do you determine the scale factor for dilation?

The scale factor for dilation can be determined by comparing the corresponding side lengths of the original figure and the dilated figure. The scale factor is equal to the ratio of the corresponding side lengths.

What are some real-life applications of dilation?

Dilation has various real-life applications, such as resizing images or fonts on a computer screen, creating enlargements or reductions in photography, and scaling maps or blueprints to different sizes. It is also used in medical imaging, architecture, and engineering for accurate measurements and designs.

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