| Literature DB >> 27330904 |
Kaijuan Yuan1, Fuyuan Xiao1, Liguo Fei1, Bingyi Kang1, Yong Deng2.
Abstract
Wireless sensor network plays an important role in intelligent navigation. It incorporates a group of sensors to overcome the limitation of single detection system. Dempster-Shafer evidence theory can combine the sensor data of the wireless sensor network by data fusion, which contributes to the improvement of accuracy and reliability of the detection system. However, due to different sources of sensors, there may be conflict among the sensor data under uncertain environment. Thus, this paper proposes a new method combining Deng entropy and evidence distance to address the issue. First, Deng entropy is adopted to measure the uncertain information. Then, evidence distance is applied to measure the conflict degree. The new method can cope with conflict effectually and improve the accuracy and reliability of the detection system. An example is illustrated to show the efficiency of the new method and the result is compared with that of the existing methods.Entities:
Keywords: Belief function; Dempster–Shafer evidence theory; Deng entropy; Evidential conflict; Wireless sensor network data fusion
Year: 2016 PMID: 27330904 PMCID: PMC4870490 DOI: 10.1186/s40064-016-2205-6
Source DB: PubMed Journal: Springerplus ISSN: 2193-1801
Fig. 1The flowchart of the new method
BPAs for the example
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| 0.41 | 0.29 | 0.3 | 0 |
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| 0 | 0.9 | 0.1 | 0 |
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| 0.58 | 0.07 | 0 | 0.35 |
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| 0.55 | 0.1 | 0 | 0.35 |
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| 0.6 | 0.1 | 0 | 0.3 |
Fusion results with different combination rules
| Combination rule | Fusion results | |||
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| Dempster | m(A) = 0 | m(A) = 0 | m(A) = 0 | m(A) = 0 |
| m(B) = 0.8969 | m(B) = 0.6575 | m(B) = 0.3321 | m(B) = 0.1422 | |
| m(C) = 0.1031 | m(C) = 0.3425 | m(C) = 0.6679 | m(C) = 0.8578 | |
| Yager | m(A) = 0 | m(A) = 0.4112 | m(A) = 0.6508 | m(A) = 0.7732 |
| m(B) = 0.2610 | m(B) = 0.0679 | m(B) = 0.0330 | m(B) = 0.0167 | |
| m(C) = 0.0300 | m(C) = 0.0105 | m(C) = 0.0037 | m(C) = 0.0011 | |
| m(AC) = 0 | m(AC) = 0.2481 | m(AC) = 0.1786 | m(AC) = 0.0938 | |
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| Murphy | m(A) = 0.0964 | m(A) = 0.4619 | m(A) = 0.8362 | m(A) = 0.9620 |
| m(B) = 0.8119 | m(B) = 0.4497 | m(B) = 0.1147 | m(B) = 0.0210 | |
| m(C) = 0.0917 | m(C) = 0.0794 | m(C) = 0.0410 | m(C) = 0.0138 | |
| m(AC) = 0 | m(AC) = 0.0090 | m(AC) = 0.0081 | m(AC) = 0.0032 | |
| Deng et al. | m(A) = 0.0964 | m(A) = 0.4674 | m(A) = 0.9089 | m(A) = 0.9820 |
| m(B) = 0.8119 | m(B) = 0.4054 | m(B) = 0.0444 | m(B) = 0.0039 | |
| m(C) = 0.0917 | m(C) = 0.0888 | m(C) = 0.0379 | m(C) = 0.0107 | |
| m(AC) = 0 | m(AC) = 0.0084 | m(AC) = 0.0089 | m(AC) = 0.0034 | |
| Zhang et al. | m(A) = 0.0964 | m(A) = 0.5681 | m(A) = 0.9142 | m(A) = 0.9820 |
| m(B) = 0.8119 | m(B) = 0.3319 | m(B) = 0.0395 | m(B) = 0.0034 | |
| m(C) = 0.0917 | m(C) = 0.0929 | m(C) = 0.0399 | m(C) = 0.0115 | |
| m(AC) = 0 | m(AC) = 0.0084 | m(AC) = 0.0083 | m(AC) = 0.0032 | |
| Proposed method | m(A) = 0.2849 | m(A) = 0.8274 | m(A) = 0.9596 | m(A) = 0.9886 |
| m(B) = 0.5306 | m(B) = 0.0609 | m(B) = 0.0032 | m(B) = 0.0002 | |
| m(C) = 0.1845 | m(C) = 0.0986 | m(C) = 0.0267 | m(C) = 0.0072 | |
| m(AC) = 0 | m(AC) = 0.0131 | m(AC) = 0.0106 | m(AC) = 0.0039 | |
Fig. 2The fusion results comparison of different rules