Christopher W. Fairall

Dr. Christopher W. Fairall

orcid

Research Focus & Metrics

Academic Career Length

57Years (1970-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 February 2003 in Journal of Climate
Verified
Journal Article
Open access
CFChristopher W. Fairall
Christopher W. Fairall
EBE. F. Bradley
E. F. Bradley
JHJ. E. Hare
J. E. Hare
AGANDREY GRACHEV
ANDREY GRACHEV
JEJ. B. Edson
J. B. Edson
In 1996, version 2.5 of the Coupled Ocean–Atmosphere Response Experiment (COARE) bulk algorithm was published, and it has become one of the most frequently used algorithms in the air–sea interaction community. This paper describes steps taken to improve the algorithm in several ways. The number of iterations to solve for stability has been shortened from 20 to 3, and adjustments have been made to the basic profile stability functions. The scalar transfer coefficients have been redefined in terms of the mixing ratio, which is the fundamentally conserved quantity, rather than the measured water vapor mass concentration. Both the velocity and scalar roughness lengths have been changed. For the velocity roughness, the original fixed value of the Charnock parameter has been replaced by one that increases with wind speeds of between 10 and 18 m s−1. The scalar roughness length parameterization has been simplified to fit both an early set of NOAA/Environmental Technology Laboratory (ETL) experiments and... Abstract In 1996, version 2.5 of the Coupled Ocean–Atmosphere Response Experiment (COARE) bulk algorithm was published, and it has become one of the most frequently used algorithms in the air–sea interaction community. This paper describes steps taken to improve the algorithm in several ways. The number of iterations to solve for stability has been shortened from 20 to 3, and adjustments have been made to the basic profile stability functions. The scalar transfer coefficients have been redefined in terms of the mixing ratio, which is the fundamentally conserved quantity, rather than the measured water vapor mass concentration. Both the velocity and scalar roughness lengths have been changed. For the velocity roughness, the original fixed value of the Charnock parameter has been replaced by one that increases with wind speeds of between 10 and 18 m s−1. The scalar roughness length parameterization has been simplified to fit both an early set of NOAA/Environmental Technology Laboratory (ETL) experiments and...

15 February 1996 in Journal of Geophysical Research: Oceans
Verified
Journal Article
Closed access
PDF file
CFChristopher W. Fairall
Christopher W. Fairall
EBE. F. Bradley
E. F. Bradley
DRD. P. Rogers
D. P. Rogers
JEJ. B. Edson
J. B. Edson
GYG. S. Young
G. S. Young

1 August 2013 in Journal of Physical Oceanography
Verified
Journal Article
Closed access
JEJames B. Edson
James B. Edson
VJVenkata Jampana
Venkata Jampana
RWRobert A. Weller
Robert A. Weller
SBSebastien P. Bigorre
Sebastien P. Bigorre
APAlbert J. Plueddemann
Albert J. Plueddemann
HHHans Hersbach
Hans Hersbach
This study investigates the exchange of momentum between the atmosphere and ocean using data collected from four oceanic field experiments. Direct covariance estimates of momentum fluxes were collected in all four experiments and wind profiles were collected during three of them. The objective of the investigation is to improve parameterizations of the surface roughness and drag coefficient used to estimate the surface stress from bulk formulas. Specifically, the Coupled Ocean–Atmosphere Response Experiment (COARE) 3.0 bulk flux algorithm is refined to create COARE 3.5. Oversea measurements of dimensionless shear are used to investigate the stability function under stable and convective conditions. The behavior of surface roughness is then investigated over a wider range of wind speeds (up to 25 m s−1) and wave conditions than have been available from previous oversea field studies. The wind speed dependence of the Charnock coefficient α in the COARE algorithm is modified to , where m = 0.017 m−1 s and b = −0.005. When combined with a parameterization for smooth flow, this formulation gives better agreement with the stress estimates from all of the field programs at all winds speeds with significant improvement for wind speeds over 13 m s−1. Wave age– and wave slope–dependent parameterizations of the surface roughness are also investigated, but the COARE 3.5 wind speed–dependent formulation matches the observations well without any wave information. The available data provide a simple reason for why wind speed–, wave age–, and wave slope–dependent formulations give similar results—the inverse wave age varies nearly linearly with wind speed in long-fetch conditions for wind speeds up to 25 m s−1.

15 January 1996 in Journal of Geophysical Research: Oceans
Verified
Journal Article
Closed access
PDF file
CFChristopher W. Fairall
Christopher W. Fairall
EBE. F. Bradley
E. F. Bradley
JGJ. S. Godfrey
J. S. Godfrey
GWG. A. Wick
G. A. Wick
JEJ. B. Edson
J. B. Edson
GYG. S. Young
G. S. Young

7 May 2011 in Reviews of Geophysics
Verified
Journal Article
Closed access
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Gerrit de LeeuwGerrit de Leeuw
Gerrit de Leeuw
EAEdgar L Andreas
Edgar L Andreas
MAMagdalena D. Anguelova
Magdalena D. Anguelova
CFChristopher W. Fairall
Christopher W. Fairall
ELErnie R. Lewis
Ernie R. Lewis
SSStephen E. Schwartz
Stephen E. Schwartz

12 October 2002 in Journal of Geophysical Research: Oceans
Verified
Journal Article
Closed access
PDF file
PPP. Ola G. Persson
P. Ola G. Persson
CFChristopher W. Fairall
Christopher W. Fairall
EAEdgar L. Andreas
Edgar L. Andreas
PGPeter S. Guest
Peter S. Guest
DPDonald K. Perovich
Donald K. Perovich