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ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

ARUP; ISBN: 978-0-9562121-5-3 - CMBBE 2012 - Cardiff University

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3.3.1 Centers of mass<br />

Table 1: Base parameter set for the individual-based model<br />

Parameter Symbol Units Value<br />

timestep ∆t s 0.5 ·10 −3<br />

simulation time Tend s 65 ·10 3<br />

conjugate gradient precision emax m/s 10 ·10 −12<br />

division size R0 m 4.5 ·10 −6<br />

division size sdev δdiv m 0.1 ·10 −6<br />

division force threshold Fd,max N 0.5 ·10 −9<br />

division time Td s 3.6 ·10 3<br />

growth time Tg s 7.2 ·10 3<br />

attr constant FLO + -FLO + σ++ J/m 2 8 ·10 −6<br />

attr constant FLO + - f lo − σ+− J/m 2 4.5 ·10 −6<br />

attr constant f lo − - f lo − σ−− J/m 2 1 ·10 −6<br />

youngs modulus Ec Pa 1600<br />

poisson ratio νc 0.4<br />

perpendicular friction coef. γ ⊥ kg/s 0.06 ·10 −6<br />

parallel friction coef. γ kg/s 0.2 ·10 −6<br />

viscosity µ Pa·s 0.7 ·10 −3<br />

temperature T K 310<br />

The easiest is to compare the centers of mass for the different constituents. We define<br />

<br />

<br />

<br />

ε = <br />

<br />

Nf lo− xi<br />

∑<br />

i=0<br />

mi<br />

NFLO +<br />

xi<br />

− ∑<br />

i=0<br />

mi<br />

<br />

<br />

<br />

<br />

<br />

<br />

/ 3<br />

Voltotal · 3<br />

4π<br />

which is normalized with the theoretical minimum radius of a cell-mass with the same volume for<br />

better comparison (see figure 3 (e)). For an ideally sorted and spherical flock, ε approaches zero.<br />

A problem of this method is, that ε becomes zero for completely randomly mixed flocks as well.<br />

3.3.2 Radial distribution function<br />

Another generic description of particle distribution in such a system that is often used, is the<br />

radial distribution function (also called pair-correlation or two-point correlation function). We<br />

encountered two problems with this approach: The statistics are even at the end of the simulation<br />

not very good, and the normalization is questionable, since the algorithm we employed uses the<br />

smallest rectangular box aligned with the global coordinate system, into which the whole colony<br />

fits. This leads to results comparable to figure 2, but both problems make it impossible to compare<br />

more than the first peaks of different realizations of the system. Therefore, we prefer to directly<br />

compare the average coordination numbers of the constituents (for which the first peak of the<br />

radial distribution function is indicative):<br />

3.3.3 Coordination number<br />

The average coordination number can be calculated by counting how many other cells a given cell<br />

has contact with - here we define contact as being closer than 102 % of the added radii of the cells.<br />

The precise number does not influence the outcome (see figure 3 (a) - (d)). We distinguish contacts<br />

between a FLO1 expressing cell (FLO + ) and a non-expressing cell ( f lo − ), etc.<br />

(5)

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