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Take a long piece of tape (about 8 or so squares length) and lay it face-up on the table.
Take another piece of tape (about 4 or so squares length) and cross it face-up, perpendicularly across the other, exactly one square's length from one end of the longer tape.
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The square length varies from 150 to 400 m.
In this experiment, we set the square length, number of nodes.
In this experiment, the square length, transmission radius, and duty cycle are fixed at 200 m, 30 m, and 0.05, respectively.
Figure 4 presents the average broadcast latencies of CFBS and OTAB when we vary the network size, which is denoted by the square length l.
We fix the square length to 200 m, the number of nodes to 400, and the transmission radius to 20 m.
The simulations indicate that there is a deviation from the inverse square length dependence of critical forces predicted from traditional linear elastic Bernoulli Euler and Timoshenko beam theories, where the nature of the deviation from the perfect inverse square length behavior differs for different crystallographic systems.
We place wireless nodes in a square area of l×l m2 uniformly and randomly while changing the square length l, number of nodes, transmission radius, and duty cycle.
We note that p ― Open image in new window and g ― Open image in new window are forces per unit length and unit square length of the shell, respectively.
Furthermore, CFBS performs much better than OTAB, i.e., when the square length is set to 350 m, the broadcast latency of CFBS is only 1 8 that of OTAB.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com