Difference between revisions of "Hertzian contact"

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(Normal contact)
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\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 16:00, 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 from analytical solutions are available. \end{equation}

FreeFem++ numerical solution