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Medusa: Coordinate Free Meshless Method implementation
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Hertzian contact: Difference between revisions

From Medusa: Coordinate Free Meshless Method implementation
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\end{equation}
\end{equation}


The coordinate $x$ is measured perpendicular to that of the cylinder axes.
The coordinate $x$ is measured perpendicular to that of the cylinder axes. For the case of nominal contact between cylinders closed form analytical solutions are available.  


For the case of nominal contact between cylinders closed from analytical solutions are available.  
The surfaces stresses are given by the equations:
\end{equation}
 
[[File:Screenshot_2016-11-16_16-05-58.png|500px]]
 
[[File:Screenshot_2016-11-16_16-07-37.png|700px]]
 
[[File:Screenshot_2016-11-16_16-08-50.png|700px]]
 
The surface stresses and stresses along the line of symmetry are shown in the following two graphs. The $x$ and $z$ coordinates are normalized with the contact width $b$.
 
[[File:Screenshot_2016-11-16_16-13-26.png|300px]]            [[File:Screenshot_2016-11-16_16-12-32.png|300px]]
 
 
= References =


= FreeFem++ numerical solution =
= FreeFem++ numerical solution =

Revision as of 15:19, 16 November 2016

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Contact of two cylinders with axes parallel

Normal contact

If two circular cylinders with radii $R_1$ and $R_2$ are pressed together by a force per unit length of magnitude $P$ with their axes parallel, then the contact patch will be of half-width $b$ such that \begin{equation} b = \sqrt{\frac{2PR}{\pi E^*}} \end{equation} where $R$ and $E^*$ are the reduced radius of contact and the contact modulus defined by \begin{equation} \frac{1}{R} = \frac{1}{R_1} + \frac{1}{R_2}, \end{equation} \begin{equation} \frac{1}{E^*} = \frac{1-{\nu_1}^2}{E_1} + \frac{1-{\nu_2}^2}{E_2}. \end{equation}

The resulting pressure distribution $p(x)$ is semielliptical, i.e., of the form \begin{equation} p(x) = p_0 \sqrt{1-\frac{x^2}{b^2}} \end{equation} where the peak pressure \begin{equation} p_0 = \sqrt{\frac{PE^*}{\pi R}}. \end{equation}

The coordinate $x$ is measured perpendicular to that of the cylinder axes. For the case of nominal contact between cylinders closed form analytical solutions are available.

The surfaces stresses are given by the equations:

File:Screenshot 2016-11-16 16-05-58.png

File:Screenshot 2016-11-16 16-07-37.png

File:Screenshot 2016-11-16 16-08-50.png

The surface stresses and stresses along the line of symmetry are shown in the following two graphs. The $x$ and $z$ coordinates are normalized with the contact width $b$.

File:Screenshot 2016-11-16 16-13-26.png File:Screenshot 2016-11-16 16-12-32.png


References

FreeFem++ numerical solution