Please use this identifier to cite or link to this item:
http://hdl.handle.net/10397/111483
| DC Field | Value | Language |
|---|---|---|
| dc.contributor | Department of Electrical and Electronic Engineering | - |
| dc.creator | Wong, KT | - |
| dc.creator | Morris, ZN | - |
| dc.creator | Nnonyelu, CJ | - |
| dc.date.accessioned | 2025-03-03T06:01:20Z | - |
| dc.date.available | 2025-03-03T06:01:20Z | - |
| dc.identifier.issn | 0001-4966 | - |
| dc.identifier.uri | http://hdl.handle.net/10397/111483 | - |
| dc.language.iso | en | en_US |
| dc.publisher | AIP Publishing LLC | en_US |
| dc.rights | © 2019 Acoustical Society of America. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the Acoustical Society of America. | en_US |
| dc.rights | The following article appeared in Kainam Thomas Wong, Zakayo Ndiku Morris, Chibuzo Joseph Nnonyelu; Rules-of-thumb to design a uniform spherical array for direction finding—Its Cramér–Rao bounds' nonlinear dependence on the number of sensors. J. Acoust. Soc. Am. 1 February 2019; 145 (2): 714–723 and may be found at https://doi.org/10.1121/1.5088592. | en_US |
| dc.title | Rules-of-thumb to design a uniform spherical array for direction finding : its Cramér–Rao bounds' nonlinear dependence on the number of sensors | en_US |
| dc.type | Journal/Magazine Article | en_US |
| dc.identifier.spage | 714 | - |
| dc.identifier.epage | 723 | - |
| dc.identifier.volume | 145 | - |
| dc.identifier.issue | 2 | - |
| dc.identifier.doi | 10.1121/1.5088592 | - |
| dcterms.abstract | This paper discovers rules-of-thumb on how the estimation precision for an incident source's azimuth-polar direction-of-arrival (ϕ,θ) depends on the number (L) of identical isotropic sensors spaced uniformly on an open sphere of radius R. This estimation's corresponding Cramér-Rao bounds (CRB) are found to follow these elegantly simple approximations, useful for array design: (i) For the azimuth arrival angle: 2π(R/λ)(σs/σn)2LMCRB(ϕ) sin(θ)≈(Le1/14)-1+3→L→∞3, ∀(ϕ,θ); and (ii) for the polar arrival angle: 2π(R/λ)(σs/σn)2LMCRB(θ)≈3-(Le6/7)-1→L→∞3, ∀(ϕ,θ). Here, M denotes the number of snapshots, λ refers to the incident signal's wavelength, and (σs/σn)2 symbolizes the signal-to-noise power ratio. | - |
| dcterms.accessRights | open access | en_US |
| dcterms.bibliographicCitation | Journal of the Acoustical Society of America, Feb. 2019, v. 145, no. 2, p. 714-723 | - |
| dcterms.isPartOf | Journal of the Acoustical Society of America | - |
| dcterms.issued | 2019-02 | - |
| dc.identifier.scopus | 2-s2.0-85061316253 | - |
| dc.identifier.pmid | 30823827 | - |
| dc.identifier.eissn | 1520-8524 | - |
| dc.description.validate | 202503 bcch | - |
| dc.description.oa | Version of Record | en_US |
| dc.identifier.FolderNumber | OA_Others | en_US |
| dc.description.fundingSource | Self-funded | en_US |
| dc.description.pubStatus | Published | en_US |
| dc.description.oaCategory | VoR allowed | en_US |
| Appears in Collections: | Journal/Magazine Article | |
Files in This Item:
| File | Description | Size | Format | |
|---|---|---|---|---|
| 714_1_online.pdf | 4.83 MB | Adobe PDF | View/Open |
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