2012
DOI: 10.1109/tap.2012.2207070
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Comparison of 2D and 3D Electromagnetic Approaches to Predict Tropospheric Turbulence Effects in Clear Sky Conditions

Abstract: Two-dimensional electromagnetic simulations are often used to evaluate the atmospheric turbulence effects on radiowave propagation in clear sky conditions. However, turbulence is clearly a three-dimensional atmospheric process. Therefore, errors potentially introduced by 2D propagation schemes to predict 3D scintillation effects have to be quantitatively assessed. On the one hand, as part of an analytical approach and starting from the Kolmogorov-von Karman turbulent spectrum, 2D formulations for log-amplitude… Show more

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Cited by 18 publications
(35 citation statements)
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“…The classical assumption is then to consider that the dimensional reduction lies in a cross section of the real medium along the longitudinal plane ℘. From a spectral point of view, this leads to define SnormalΔNe2normalD()Ktrue→ as the integral of SnormalΔNe3normalD()Ktrue→ along the dimension transverse to ℘, i.e., the dimension disregarded by the reduction 3‐D/2‐D [ Fabbro and Féral , ]. As an illustration but without loss of generality, if the dimensional reduction is conducted along the plane ℘ = ( X , Z ) defined in Figure , then SnormalΔNe2normalD()Ktrue→=SnormalΔNe2normalD(),KXKZ is given by SnormalΔNe2normalD(),KXKZ=truetrue∫+dKYSnormalΔNe3normalD(),,KXKYKZ. …”
Section: Statistical Description Of Ionospheric Irregularitiesmentioning
confidence: 99%
“…The classical assumption is then to consider that the dimensional reduction lies in a cross section of the real medium along the longitudinal plane ℘. From a spectral point of view, this leads to define SnormalΔNe2normalD()Ktrue→ as the integral of SnormalΔNe3normalD()Ktrue→ along the dimension transverse to ℘, i.e., the dimension disregarded by the reduction 3‐D/2‐D [ Fabbro and Féral , ]. As an illustration but without loss of generality, if the dimensional reduction is conducted along the plane ℘ = ( X , Z ) defined in Figure , then SnormalΔNe2normalD()Ktrue→=SnormalΔNe2normalD(),KXKZ is given by SnormalΔNe2normalD(),KXKZ=truetrue∫+dKYSnormalΔNe3normalD(),,KXKYKZ. …”
Section: Statistical Description Of Ionospheric Irregularitiesmentioning
confidence: 99%
“…The constraint of applying a 2D propagation scheme to predict 3D turbulence effects has been discussed [26]. The phase variance of the 2D model is slightly overestimated.…”
Section: Refractive-index Fluctuationmentioning
confidence: 99%
“…The PWE-MPS is a resolution of the scalar wave Helmholtz equation only considering forward propagation and taking into account turbulence effect via phase screen generations. For more details, the reader should refer to [10] and [2]. The refractive index is decomposed in n(x, y, z) = n 0 (x, y, z) + n 1 (x, y, z), with n 0 (x, y, z) the stable component of the modified refractive index, and n 1 (x, y, z) the turbulent component of the refractive index.…”
Section: Turbulent Tropospherementioning
confidence: 99%
“…E(x 0 , y, z)e −j(k y y+k z z) e j(k y y+k z z) (2) where along x the range step is δx, y and z are the transverse coordinates, k y and k z are the spatial wave number dual of y and z in Fourier space. For one step forward, the turbulent propagation index n 1 is integrated over the propagation step by generation of a phase screen φ (y, z) [10]:…”
Section: Turbulent Tropospherementioning
confidence: 99%
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