Toggle menu
71
399
28
3.6K
Medusa: Coordinate Free Meshless Method implementation
Toggle preferences menu
Toggle personal menu
Not logged in
Your IP address will be publicly visible if you make any edits.

Hertzian contact: Difference between revisions

From Medusa: Coordinate Free Meshless Method implementation
No edit summary
Line 24: Line 24:
\begin{equation}
\begin{equation}
p_0 = \sqrt{\frac{PE^*}{\pi R}}.
p_0 = \sqrt{\frac{PE^*}{\pi R}}.
\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 from analytical solutions are available.  
For the case of nominal contact between cylinders closed from analytical solutions are available.  
\end{equation}
\end{equation}
= FreeFem++ numerical solution =
= FreeFem++ numerical solution =

Revision as of 15:00, 16 November 2016

Click on Solid Mechanics to go back.

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 from analytical solutions are available. \end{equation}

FreeFem++ numerical solution