P69 Optical turbulence
estimation using WRF model
Wang, Yao,
and
Sukanta Basu, North Carolina State University
Small-scale
atmospheric turbulence in the inertial-convective range is referred as optical
turbulence, because the wave phase and amplitude of the optical and
electromagnetic wave is highly affected by the small-scale variation of
temperature and specific humanity. Documentation and prediction of optical
turbulence are significant to a wide range of applications: environmental
monitoring, optical communication, astronomy, sensing with detection,
reconnaissance and identification, guiding systems or directed-energy systems.
The refractive index structure parameter Cn2 which
depends on temperature structure parameter, Ct2 (if the minor wavelength and
humidity dependence are ignored) is chosen to describe the effect of the
optical turbulence.
Meso-scale
models can be utilized to estimate and predict the Ct2 from calculated heat and
momentum fluxes by using the traditional Monin-Obukhov
similarity theory (MOST) based functions. The functions in these
M-O similarity are empirically derived from fast-response turbulence
observations collected during different field campaigns where fluxes are
estimated over an area. In this study, surface heat flux, friction velocity,
temperature and pressure from Weather Research Forecasting (WRF) model with
Fast Four Dimensional Assimilation (FDDA) (surface data observational nudging)
was utilized to estimate the Ct2 in the case study. Three nights (23-26 October
1999) during CASES-99 study are selected because the turbulence intensities of
these nights differ significantly. The first night is intermittently turbulent,
the second is fully turbulent, and the third is mainly driven
by radiative cooling (hardly turbulent). The estimated results of Ct2
are evaluated by the observed Ct2 value from the state-of-the-art optical
turbulence measurement instrument, scitillometer to
see the performance of these traditional MOST based functions under different
atmospheric boundary layer turbulent stabilities.