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    Velocity and Drag Evolution From the Leading Edge of a Model Mangrove Forest

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    Identificadores
    URI: http://hdl.handle.net/10902/15875
    DOI: 10.1002/2017JC012945
    ISSN: 2169-9275
    ISSN: 2169-9291
    ISSN: 0148-0227
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    Autoría
    Maza Fernández, María EmiliaAutoridad Unican; Adler, Katherine; Ramos, Diogo; Garcia, Adrian Mikhail; Nepf, Heidi
    Fecha
    2017
    Derechos
    ©American Geophysical Union. Maza, M., Adler, K., Ramos, D., Garcia, A. M., & Nepf, H. ( 2017). Velocity and drag evolution from the leading edge of a model mangrove forest. Journal of Geophysical Research: Oceans, 122, 9144? 9159. https://doi.org/10.1002/2017JC012945
    Publicado en
    Journal of Geophysical Research: Oceans, 122, 9144-9159
    Editorial
    John Wiley & Sons
    Enlace a la publicación
    https://agupubs.onlinelibrary.wiley.com/doi/full/10.1002/2017JC012945
    Resumen/Abstract
    An experimental study of unidirectional flow through a model mangrove forest measured both velocity and forces on individual trees. The individual trees were 1/12th scale models of mature Rhizophora, including 24 prop roots distributed in a three-dimensional layout. Thirty-two model trees were distributed in a staggered array producing a 2.5 m long forest. The velocity evolved from a boundary layer profile at the forest leading edge to a vertical profile determined by the vertical distribution of frontal area, with significantly higher velocity above the prop roots. Fully developed conditions were reached at the fifth tree row from the leading edge. Within the root zone the velocity was reduced by up to 50% and the TKE was increased by as much as fivefold, relative to the upstream conditions. TKE in the root zone was mainly produced by root and trunk wakes, and it agreed in magnitude with the estimation obtained using the Tanino and Nepf (2008) formulation. Maximum TKE occurred at the top of the roots, where a strong shear region was associated with the change in frontal area. The drag measured on individual trees decreased from the leading edge and reached a constant value at the fifth row and beyond, i.e., in the fully developed region. The drag exhibited a quadratic dependence on velocity, which justified the definition of a quadratic drag coefficient. Once the correct drag length-scale was defined, the measured drag coefficients collapsed to a single function of Reynolds number.
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    UNIVERSIDAD DE CANTABRIA

    Repositorio realizado por la Biblioteca Universitaria utilizando DSpace software
    Contacto | Sugerencias
    Metadatos sujetos a:licencia de Creative Commons Reconocimiento 4.0 España