ANALYTICAL MODEL OF PROPAGATING SAND RIPPLES

Authors
Citation
Rb. Hoyle et Aw. Woods, ANALYTICAL MODEL OF PROPAGATING SAND RIPPLES, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 56(6), 1997, pp. 6861-6868
Citations number
18
ISSN journal
1063651X
Volume
56
Issue
6
Year of publication
1997
Pages
6861 - 6868
Database
ISI
SICI code
1063-651X(1997)56:6<6861:AMOPSR>2.0.ZU;2-K
Abstract
We formulate a simple phenomenological model of aeolian sand ripple mi gration based upon a balance between grain hopping driven by saltation and grain rolling or avalanching under gravity. We develop a set of m odel equations governing the evolution of the ripple slope. The model has solutions describing steadily Propagating isolated ripples, produc ed by a horizontal saltation flux, and periodic trains of ripples, whi ch develop when the saltation flux is inclined to the horizontal. In t he case of an inclined saltation flux, the ripple wavelength is contro lled by the length of the shadow zone, as suggested by R. P. Sharp [J. Geol. 71, 617 (1963)]. Although very simple, our model predicts some of the qualitative features shown by sand ripples in experimental or f ield studies [R. A. Bagnold, The Physics of Blown Sand and Desert Dune s (Methuen and Co., London, 1941); R. P. Sharp, J. Geol. 71, 617 (1963 )]. We find that ripples only develop above a certain threshold value of the saltation flux intensity. Furthermore, at relatively low saltat ion fluxes, the lee slope of the ripple is a smooth curve, whereas abo ve a critical value of the saltation flux, a slip face develops near t he crest. The model predicts a decrease in the speed of propagation as the ripple becomes larger, consistent with observations that smaller ripples are eliminated by ripple merger [IR. P. Sharp, J. Geol. 71, 61 7 (1963)], and also with numerical simulations [R. S. Anderson, Earth- Sci. Rev. 29, 77 (1990); S. B. Forrest and P. K. Haff, Science 255, 12 40 (1992); W. Landry and B. T. Werner, Physica D 77, 238 (1994)].