Test of Scintillometer Saturation Correction Methods Using Field Experimental Data

Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occu...

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Published in:Boundary-layer meteorology Vol. 137; no. 3; pp. 493 - 507
Main Authors: Kleissl, J, Hartogensis, O. K, Gomez, J. D
Format: Journal Article
Language:English
Published: Dordrecht Dordrecht : Springer Netherlands 01-12-2010
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Abstract Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occurs at [graphic removed] , where [graphic removed] is the structure parameter of the refractive index, D is the aperture size, λ is the wavelength, L is the transect length, which is smaller than theoretically derived saturation limits. At a transect length of 1 km, a height of 2.5 m, and aperture ≈0.15 m the correction factor exceeds 5% already at [graphic removed] , which will affect many practical applications of scintillometry. The Clifford correction method, which only depends on [graphic removed] and the transect geometry, provides good saturation corrections over the range of conditions observed in our study. The saturation correction proposed by Ochs and Hill results in correction factors that are too small in large saturation regimes. An inner length scale dependence of the saturation correction factor was not observed. Thus for practical applications the Clifford correction method should be applied.
AbstractList Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occurs at [graphic removed] , where [graphic removed] is the structure parameter of the refractive index, D is the aperture size, λ is the wavelength, L is the transect length, which is smaller than theoretically derived saturation limits. At a transect length of 1 km, a height of 2.5 m, and aperture ≈0.15 m the correction factor exceeds 5% already at [graphic removed] , which will affect many practical applications of scintillometry. The Clifford correction method, which only depends on [graphic removed] and the transect geometry, provides good saturation corrections over the range of conditions observed in our study. The saturation correction proposed by Ochs and Hill results in correction factors that are too small in large saturation regimes. An inner length scale dependence of the saturation correction factor was not observed. Thus for practical applications the Clifford correction method should be applied.
(ProQuest: Abstract omitted; see image)[PUBLICATION ABSTRACT]
Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occurs at C super(2) sub(n) approximately 0.074 D super(5/3) lambda super(1/3) L super(-8/3), where C super(2) sub(n) is the structure parameter of the refractive index, D is the aperture size, lambda is the wavelength, L is the transect length, which is smaller than theoretically derived saturation limits. At a transect length of 1km, a height of 2.5 m, and aperture approximately 0.15 m the correction factor exceeds 5% already at C super(2) sub(n) = 2 x 10 super(-12) m super(-2/3), which will affect many practical applications of scintillometry. The Clifford correction method, which only depends on C super(2) sub(n) and the transect geometry, provides good saturation corrections over the range of conditions observed in our study. The saturation correction proposed by Ochs and Hill results in correction factors that are too small in large saturation regimes. An inner length scale dependence of the saturation correction factor was not observed. Thus for practical applications the Clifford correction method should be applied.
Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occurs at C n 2 approximately 0.074 D 5 / 3 lambda 1 / 3 L - 8 / 3 , where C n 2 is the structure parameter of the refractive index, D is the aperture size, lambda is the wavelength, L is the transect length, which is smaller than theoretically derived saturation limits. At a transect length of 1km, a height of 2.5 m, and aperture approximately 0.15 m the correction factor exceeds 5% already at C n 2 = 2 10 - 12 m - 2 / 3 , which will affect many practical applications of scintillometry. The Clifford correction method, which only depends on C n 2 and the transect geometry, provides good saturation corrections over the range of conditions observed in our study. The saturation correction proposed by Ochs and Hill results in correction factors that are too small in large saturation regimes. An inner length scale dependence of the saturation correction factor was not observed. Thus for practical applications the Clifford correction method should be applied.
Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occurs at [C.sup.2.sub.n] ≅ 0.074[D.sup.5/3][λ.sup.1/3][L.sup.-8/3], where [C.sup.2.sub.n] is the structure parameter of the refractive index, D is the aperture size, X is the wavelength, L is the transect length, which is smaller than theoretically derived saturation limits. At a transect length of 1 km, a height of 2.5 m, and aperture ≅ 0.15 m the correction factor exceeds 5% already at [C.sup.2.sub.n] = 2 x [10.sup.-12][m.sup.-2/3], which will affect many practical applications of scintillometry. The Clifford correction method, which only depends on [C.sup.2.sub.n] and the transect geometry, provides good saturation corrections over the range of conditions observed in our study. The saturation correction proposed by Ochs and Hill results in correction factors that are too small in large saturation regimes. An inner length scale dependence of the saturation correction factor was not observed. Thus for practical applications the Clifford correction method should be applied. Keywords Large aperture scintillometer * Sensible heat flux * Signal saturation * Wave propagation
Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occurs atC2n˜ 0.074D5/3¿1/3L-8/3, where C2n is the structure parameter of the refractive index, D is the aperture size, ¿ is the wavelength, L is the transect length, which is smaller than theoretically derived saturation limits. At a transect length of 1 km, a height of 2.5 m, and aperture ˜0.15 m the correction factor exceeds 5% already at C2n= 2 × 10-12m-2/3, which will affect many practical applications of scintillometry. The Clifford correction method, which only depends on C2 n and the transect geometry, provides good saturation corrections over the range of conditions observed in our study. The saturation correction proposed by Ochs and Hill results in correction factors that are too small in large saturation regimes. An inner length scale dependence of the saturation correction factor was not observed. Thus for practical applications the Clifford correction method should be applied
Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of different aperture sizes and path lengths was performed to investigate the onset of, and corrections for, signal saturation. Saturation already occurs at , where is the structure parameter of the refractive index, D is the aperture size, λ is the wavelength, L is the transect length, which is smaller than theoretically derived saturation limits. At a transect length of 1 km, a height of 2.5 m, and aperture ≈0.15 m the correction factor exceeds 5% already at , which will affect many practical applications of scintillometry. The Clifford correction method, which only depends on and the transect geometry, provides good saturation corrections over the range of conditions observed in our study. The saturation correction proposed by Ochs and Hill results in correction factors that are too small in large saturation regimes. An inner length scale dependence of the saturation correction factor was not observed. Thus for practical applications the Clifford correction method should be applied.
Audience Academic
Author Kleissl, J
Gomez, J. D
Hartogensis, O. K
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  fullname: Gomez, J. D
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Issue 3
Keywords Signal saturation
Large aperture scintillometer
Wave propagation
Sensible heat flux
sensible heat
saturation
corrections
Height
refractive index
Scintillation counter
heat transfer
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Snippet Saturation of large aperture scintillometer (LAS) signals can result in sensible heat flux measurements that are biased low. A field study with LASs of...
(ProQuest: Abstract omitted; see image)[PUBLICATION ABSTRACT]
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SubjectTerms algorithms
Analysis
Apertures
Atmospheric Protection/Air Quality Control/Air Pollution
Atmospheric Sciences
atmospheric surface-layer
Boundaries
calibration
Convection, turbulence, diffusion. Boundary layer structure and dynamics
Earth and Environmental Science
Earth Sciences
Earth, ocean, space
Exact sciences and technology
External geophysics
Flux
fluxes
inner-scale
Large aperture scintillometer
Meteorology
Methods
optical scintillation
Refractive index
Refractivity
Remote sensing
Saturation
Scintillation counters
Sensible heat flux
Signal saturation
sonic anemometer
strong turbulence
temperature
Wave propagation
Wavelengths
Title Test of Scintillometer Saturation Correction Methods Using Field Experimental Data
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Volume 137
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