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LDTC1020 bảng dữ liệu(PDF) 4 Page - Wavelength Electronics, Inc. |
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LDTC1020 bảng dữ liệu(HTML) 4 Page - Wavelength Electronics, Inc. |
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4 / 7 page ![]() Case Study CS-LDTC11 Rev. A Page 4 © 2022 • Sales & Technical Support: (406) 587-4910 • email: sales@teamWavelength.com • web: www.teamWavelength.com Figure 5. Camera imagery, large-aperture integrated camera signals (red), and small-aperture integrated camera signals (green) are shown for four propagation cases: in air (batch 1, 0-m depth, upper-left panel), deeper ocean (batch 5, 179.0-m depth, upper-right panel), moderate ocean (batch 17, 62.0-m depth, lower-left panel), and shallower ocean (batch 23, 16.1-m depth, lower-right). The camera images provide the median frame from each batch for visual comparison. Plots of integrated camera signal vs. frame number facilitate test-case comparisons of frame-to-frame similarity.1 Supporting sensors also measured temperature, beam attenuation, backscattering, and temperature gradient in Figure 6. The thermocline region shows a significant change in ocean temperature and gradient which is related to the refractive index structure and inner scale of turbulence. In this region, the effect on beam propagation is clear. The beam attenuation and backscattering are both at extreme maximums, diminishing the resolution of imaging in the thermocline region. When temperature and temperature gradient have minimal changes, the beam attenuation and backscattering also decrease. The thermocline upper and lower limits are seen at 15 m and 70 m, respectively, highlighted in yellow. The pronounced attenuation and scattering in plots result from biological matter and particulates residing within the thermocline.1 |
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