Estimating Cn2 Over Snow And Sea Ice From Meteorological Quantities

Because turbulent fluctuations in the atmospheric refractive index (n) at wavelength x are related to turbulent fluctuations in the temperature (t) and humidity (q) by n = A(x,P,T,9)t + B(x,P,T,Q)q, it is possible to estimate the refractive index structure parameter C in the atmospheric surface layer from meteorological quantities. I describe two such estimation procedures, one based on the velocity, temperature, and humidity scales u*' t*, and q*, and a second based on the routine meteorological quantities U,, T -Th, and %-Q,. Subscript h here denotes the wind speed (U,), temperature (TO, and humidity (Qh) at rVference height h; subscript s indicates the sUrface value. I tabulate the coefficients A and B as functions of λ, the atmospheric pressure (I)), and the ambient temperature (T) and humidity (Q) in four wavelength regions--visible (including near-infrared), an infrared window, near-millimeter, and radio. A sensitivity analysis of the two estimation procedures demonstrates that the accuracy of the Cn2 estimate is a strong function of the Bowen ratio (Bo), the ratio of sensible to latent heat flux at the surface. At two Bo values within the interval [-10,10], one dependent on λ and the other on enyironmental conditions, the uncertainty in the Cn2 estimate becomes infinite. I focus on C values over snow and sea ice, and my examples are for these surfaces, but the estimation procedures presented can be applied to any geophysical surface that is horizontally homogeneous.

[1]  E. F. Bradley,et al.  An alternative analysis of flux-gradient relationships at the 1976 ITCE , 1982 .

[2]  E. Gossard Power spectra of temperature, humidity and refractive index from aircraft and tethered balloon measurements , 1960 .

[3]  R. S. Lawrence,et al.  A survey of clear-air propagation effects relevant to optical communications , 1970 .

[4]  S. Clifford,et al.  Modified spectrum of atmospheric temperature fluctuations and its application to optical propagation , 1978 .

[5]  H. Panofsky,et al.  Atmospheric Turbulence: Models and Methods for Engineering Applications , 1984 .

[6]  Edgar L. Andreas,et al.  A theory for the scalar roughness and the scalar transfer coefficients over snow and sea ice , 1987 .

[7]  R. S. Lawrence,et al.  Saturation of optical scintillation by strong turbulence , 1974 .

[8]  E. L. Andreas Spectral Measurements in a Disturbed Boundary Layer over Snow , 1987 .

[9]  C. Paulson The Mathematical Representation of Wind Speed and Temperature Profiles in the Unstable Atmospheric Surface Layer , 1970 .

[10]  R. Hill,et al.  Measuring High-Frequency Humidity, Temperature and Radio Refractive Index in the Surface Layer , 1985 .

[11]  G. R. Ochs,et al.  A saturation-resistant optical scintillometer to measure Cn2† , 1978 .

[12]  Edgar L. Andreas,et al.  Estimating Cn 2 over snow and sea ice from meteorological data , 1988 .

[13]  R. S. Lawrence,et al.  Measurements of Atmospheric Turbulence Relevant to Optical Propagation , 1970 .

[14]  Theory of measuring the path-averaged inner scale of turbulence by spatial filtering of optical scintillation. , 1982, Applied optics.

[15]  Carl H. Gibson,et al.  Effects of temperature and humidity fluctuations on the optical refractive index in the marine boundary layer , 1975 .

[16]  E. F. Bradley,et al.  Flux-Profile Relationships in the Atmospheric Surface Layer , 1971 .

[17]  J. Kondo,et al.  Bulk transfer coefficient over a snow surface , 1986 .

[18]  Stuart A. Collins,et al.  Behavior of the Refractive-Index-Structure Parameter near the Ground* , 1971 .

[19]  M. L. Wesely,et al.  Diurnal cycles of the refractive index structure function coefficient , 1973 .