First- and Second-Order Closure Models for Wind in a Plant Canopy

J. D. Jean-Paul Pinard Department of Earth and Atmospheric Sciences, University of Alberta, Edmonton, Alberta, Canada

Search for other papers by J. D. Jean-Paul Pinard in
Current site
Google Scholar
PubMed
Close
and
John D. Wilson Department of Earth and Atmospheric Sciences, University of Alberta, Edmonton, Alberta, Canada

Search for other papers by John D. Wilson in
Current site
Google Scholar
PubMed
Close
Restricted access

Abstract

Katul and Chang recently compared the performance of two second-order closure models with observations of wind and turbulence in the Duke Forest canopy, noting that such models “alleviate some of the theoretical objections to first-order closure.” This paper demonstrates that, notwithstanding those (valid) theoretical objections, Duke Forest wind simulations of comparable quality can be obtained using a first-order closure, namely, eddy viscosity Kλk, where k is the turbulent kinetic energy and λ is a turbulence length scale. It is concluded that, most often, uncertainty in the drag coefficient will limit the accuracy of modeled wind statistics, regardless of the turbulence closure chosen.

Corresponding author address: J. D. Jean-Paul Pinard, Department of Earth and Atmospheric Sciences, 1-26 Earth Sciences Building, University of Alberta, Edmonton, AB T6G 2E3, Canada. jpinard@ualberta.ca

Abstract

Katul and Chang recently compared the performance of two second-order closure models with observations of wind and turbulence in the Duke Forest canopy, noting that such models “alleviate some of the theoretical objections to first-order closure.” This paper demonstrates that, notwithstanding those (valid) theoretical objections, Duke Forest wind simulations of comparable quality can be obtained using a first-order closure, namely, eddy viscosity Kλk, where k is the turbulent kinetic energy and λ is a turbulence length scale. It is concluded that, most often, uncertainty in the drag coefficient will limit the accuracy of modeled wind statistics, regardless of the turbulence closure chosen.

Corresponding author address: J. D. Jean-Paul Pinard, Department of Earth and Atmospheric Sciences, 1-26 Earth Sciences Building, University of Alberta, Edmonton, AB T6G 2E3, Canada. jpinard@ualberta.ca

Save
  • Katul, G. G. and W-H. Chang. 1999. Principal length scales in second-order closure models for canopy turbulence. J. Appl. Meteor 38:16311643.

    • Search Google Scholar
    • Export Citation
  • Massman, W. J. and J. C. Weil. 1999. An analytical one-dimensional second-order closure model of turbulence statistics and the Lagrangian time scale within and above plant canopies of arbitrary structure. Bound.-Layer Meteor 91:81107.

    • Search Google Scholar
    • Export Citation
  • Patankar, S. V. 1980. Numerical Heat Transfer and Fluid Flow. Hemisphere, 197 pp.

  • Raupach, M. R. and R. H. Shaw. 1982. Averaging procedures for flow within vegetation canopies. Bound.-Layer Meteor 22:7990.

  • Raupach, M. R., J. J. Finnigan, and Y. Brunet. 1996. Coherent eddies and turbulence in vegetation canopies: The mixing-layer analogy. Bound.-Layer Meteor 78:351382.

    • Search Google Scholar
    • Export Citation
  • Wilson, J. D. 1988. A second-order closure model for flow through vegetation. Bound.-Layer Meteor 42:371392.

  • Wilson, J. D. and T. K. Flesch. 1999. Wind and remnant tree sway in forest cutblocks. Part III: A windflow model to diagnose spatial variation. Agric. For. Meteor 93:259282.

    • Search Google Scholar
    • Export Citation
  • Wilson, J. D., J. J. Finnigan, and M. R. Raupach. 1998. A first-order closure for disturbed plant canopy flows, and its application to windflow through a canopy on a ridge. Quart. J. Roy. Meteor. Soc 124:705732.

    • Search Google Scholar
    • Export Citation
  • Wilson, N. R. and R. H. Shaw. 1977. A higher order closure model for canopy flow. J. Appl. Meteor 16:11971205.

All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 1044 725 17
PDF Downloads 127 28 3