next up previous
Next: Layered Packings For Cylinders Up: Origins of Stochasticity: Turbulent Previous: Sedimentation Concentration

Calculating Random Fibre Contacts

Expected number of fibres in cube of side $\lambda$
\begin{displaymath}
n_{crowd} \ \frac{6 \lambda^3}{\pi \lambda^3} = 
\frac{6}{\pi}\ n_{crowd}\end{displaymath} (2)

Number of intersections with one fibre
\begin{displaymath}
\frac{[\lambda\overline{\sin\theta}]\times 2 [width]}
{[Area \ of \ base \ of \ cube]}\times \frac{6 n_{crowd}}{\pi}\end{displaymath} (3)

Here, $\lambda\overline{\sin\theta}$ is the mean projected length of one fibre onto cube base:
\begin{displaymath}
\lambda\overline{\sin\theta} = 
\frac{\lambda}{4\pi}\int_{\p...
 ...{2\pi} 
\sin^2\theta \ d\theta \ d\phi = 
\frac{\pi \lambda}{4}\end{displaymath} (4)
Hence
\begin{displaymath}
n_{contacts}=\frac{6}{\pi} \ n_{crowd}\ 
\frac{\pi \omega}{2...
 ...\frac{3\omega }{\lambda} \ n_{crowd} = 
\frac{3}{A} \ n_{crowd}\end{displaymath} (5)

Variance of fibre contacts per fibre
We expect the number of contacts per fibre to vary from fibre to fibre as a Poisson random variable, so has variance equal to the mean in the random case; variance exceeding the mean for flocculated.

For more information see Dodson [5].



C.T.J. Dodson
11/26/1998