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Wireless Sensor and Actuator Networks for Lighting Energy ...

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too sensitive to failures. Parameters m e <strong>and</strong> m were tuned so as to optimize the<br />

response of the algorithm to the lighting environment. m e , m , m dif <strong>and</strong> m mov were tuned<br />

separately <strong>for</strong> the two majority voting schemes. The constant scaling factor was<br />

chosen to be large in order not to result in an obvious lag in the fused value by<br />

weighting the previous predicted value too heavily.<br />

4.4.3 Simulation <strong>and</strong> Real-time Testing Results<br />

Figure 4-6 shows the real-time implementation of the mote-FVF algorithm using<br />

the median value majority voting scheme on the six-mote sensor network. The small<br />

cross signs are the raw sensed data from each mote, the dashed line is the true<br />

illuminance measured by the high fidelity light meter, <strong>and</strong> the solid line is the fused<br />

value. The figure reveals that the algorithm accurately followed the sensed data <strong>and</strong><br />

reflected the illuminance pertinently with a maximum error of 3.36% regardless of the<br />

lag in the transient mode. Similarly, the algorithm with Gaussian correlation majority<br />

voting scheme run off-line on the same set of data, shown in Figure 4-7, revealed a<br />

maximum error of 4.01%. These errors include calibration errors when mapping raw<br />

digital readings to units of lux <strong>and</strong> the variation of illuminance in the spatial position on<br />

the testbed. From a physical point of view, the 4.01% error represents about a 30 lux<br />

difference, to which a human being is insensitive. Furthermore, the choice of majority<br />

voting mechanism didn’t seem to have a noticeable impact on the per<strong>for</strong>mance of the<br />

algorithm.<br />

57

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