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First 1002 results for ” S.; Capelle”

1. Physiological interpretation of a hyperspectral time series in a citrus orchard

   Hyperspectral remote sensing for monitoring horticultural production systems requires the underst...

   J Stuckens, S Dzikiti, WW Verstraeten, S Verreynne, R Swinnen, P Coppin | Status: published | Journal: Agricultural and Forest Meteorology | Year: 2011 | First page: 1002 | Last page: 1015 | doi: 10.1016/j.agrformet.2011.03.006

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2. Blue-green roofs with forecast-based operation to reduce the impact of weather extremes

   Conventional green roofs have often been criticised for their limited water buffer capacity durin...

   Tim Busker, Hans de Moel, Toon Haer, Maurice Schmeits, Bart van den Hurk, Kira Myers, Dirk Gijsbert Cirkel, and Jeroen Aerts | Journal: Journal of Environmental Management | Volume: 301 | Year: 2022 | doi: https://doi.org/10.1016/j.jenvman.2021.113750

   Publication

3. Comprehensible Control for Researchers and Developers Facing Data Challenges

   The DARE platform enables researchers and their developers to exploit more capabilities to handle...

   Malcolm Atkinson, Alessandro Spinuso | Journal: 15th International Conference on eScience (eScience) | Year: 2019 | doi: 10.1109/eScience.2019.00042

   Publication

4. Coupled sea surface-atmospheric model 2. Spectrum of short wind waves

   A physical model of the short wind wave spectrum in the wavelength range from a few millimeters ...

   VN Kudryavtsev, VK Makin, B Chapron | Status: published | Journal: J. Geophys. Res. | Volume: 104 | Year: 1999 | First page: 7625 | Last page: 7639

   Publication

5. A two-dimensional effective sound speed parabolic equation model for infrasound propagation with ground topography

   A terrain capable parabolic equation (PE) propagation algorithm for long range infrasound propaga...

   R Waxler, C Hetzer, JD Assink, PS Blom | Journal: Journal of the Acoustical Society of America | Volume: 152 | Year: 2022 | First page: 3659 | Last page: 3669 | doi: https://doi.org/10.1121/10.0016558

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