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Architecture of Computing Systems (Lecture Notes in Computer ...

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110 K. Kloch et al.<br />

(a)<br />

<strong>in</strong>fection ratio K<br />

0.012<br />

0.010<br />

0.008<br />

0.006<br />

0.004<br />

N = 256<br />

N = 512<br />

N = 1024<br />

N = 2048<br />

2-parameter theory<br />

(N = 256; <strong>of</strong>fset = 0.0033,<br />

prefactor = 0.00105)<br />

0.002<br />

crossover<br />

scale dp 0.000<br />

0.0 0.5 1.0 1.5<br />

scaled radio range R/d p (b)<br />

Fig. 5. (a) Scal<strong>in</strong>g plot for the <strong>in</strong>fection ratio K <strong>in</strong> the third regime. The K values for<br />

different N (see legend) and L = 2000 are plotted versus the scaled radio range R/dp<br />

with dp taken from (9). The numerical curves are parallel with a small <strong>of</strong>fest <strong>in</strong> the<br />

third regime (R/dp > 1). The dashed grey l<strong>in</strong>e shows the analytic theory. Two fitt<strong>in</strong>g<br />

parameters are needed: a prefactor and an <strong>of</strong>fset; both will be different for N>256. (b)<br />

Illustration <strong>of</strong> the geometical constra<strong>in</strong>t determ<strong>in</strong><strong>in</strong>g cha<strong>in</strong> <strong>in</strong>fections for simultaneous<br />

<strong>in</strong>fection <strong>of</strong> three agents.<br />

the closeness <strong>of</strong> both crossovers for small ρ (and N). While the second regime is<br />

rather broad for N = 2048, it nearly vanishes for N = 256, where<br />

�� � �<br />

Rc1 π3 L L<br />

=<br />

/<br />

2 N 2 √ �<br />

=<br />

N<br />

� 2π3 /N ≈ 0.492<br />

Rc2<br />

compared with Rc1/Rc2 ≈ 0.174 for N = 2048. Therefore, K =0.05 is not fully<br />

reached for the lower values <strong>of</strong> N, and the curve <strong>in</strong> the third regime is consequently<br />

shifted downwards by a small amount as seen <strong>in</strong> Fig. 5. This, however,<br />

does not devaliate our analytical descriptions <strong>of</strong> both crossovers nor the unified<br />

scal<strong>in</strong>g behavior seen <strong>in</strong> the third regime.<br />

To derive the form <strong>of</strong> the scal<strong>in</strong>g curve for R/dp > 1<strong>in</strong>Fig.5,wehavetoconsider<br />

the geometric constra<strong>in</strong>ts for immediate cha<strong>in</strong> <strong>in</strong>fections. The probability<br />

<strong>of</strong> a cha<strong>in</strong> <strong>in</strong>fection is not related with the motion <strong>of</strong> the agents. Therefore, one<br />

need not consider trajectories, and the analysis is ma<strong>in</strong>ly geometrical. A newly<br />

<strong>in</strong>fected (second) agent is always located at distance R from the <strong>in</strong>fect<strong>in</strong>g agent,<br />

s<strong>in</strong>ce it would have been <strong>in</strong>fected earlier otherwise. Its radio range, i.e., the area<br />

<strong>in</strong> which a third agent could be <strong>in</strong>fected, thus overlaps with the radio range area<br />

A1 <strong>of</strong> the first agent (where no additional third agent could be <strong>in</strong>fected). This<br />

extended radio range area A2 is thus not a circle. Nevertheless, the correspond<strong>in</strong>g<br />

area can be calculated analytically. Figure 5(b) illustrates A1 (white) and A2<br />

(black). Without loss <strong>of</strong> generality, we assume that A2 is to the right <strong>of</strong> A1. A2<br />

is a half circle (π/2 R 2 ) plus twice the (nearly triangular) part with height R/2<br />

and length R; itsexactareais2.18918 R 2 . The additional <strong>in</strong>fection probability<br />

(first order term) is thus F1 =2.18918 ρR 2 .<br />

However, the cha<strong>in</strong> reaction can go on, s<strong>in</strong>ce there could be a fourth agent <strong>in</strong><br />

the radio range <strong>of</strong> the third agent. S<strong>in</strong>ce the third agent can be anywhere <strong>in</strong> A2

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