Inverse modeling of beaver reservoir's water spectral reflectance.

Estimation of inherent optical properties (IOP) needed for water quality evaluation by remote sensing models is very complex, primarily due to the large number of model simulations needed to find optimal parameter values. This study presents an approach for optimally parameterizing the IOP values of a physical hyperspectral optical - Monte Carlo (PHO-MC) model. An artificial neural network (ANN) based pseudo simulator combined with the Nondominated Sorted Genetic Algorithm II (NSGA II) was used to efficiently perform a large number of model simulations and to search the optimal parameter values for IOP determination. Concentrations of suspended matter (sm), chlorophyll-a (chl), and total dissolved organic matter (DOM) along with the reflectance data at 16 different wavelengths were measured at 48 sampling stations in the Beaver Reservoir, Arkansas, between 2003 and 2005 and were used to evaluate the IOP values. Measured concentrations and reflectance data from 24 sampling stations were used to optimize IOP parameter values for sm, chl, and DOM. The data collected from the remaining 24 sampling stations were used for the validation of PHO-MC model-predicted reflectance by using optimized IOP values. PHO-MC predicted reflectance values were significantly correlated (r = 0.90, p < 0.01) with the corresponding measured reflectance values, indicating that the pseudo simulator combined with the NSGA II accurately estimated the IOP values. An estimated 1010 years of calculation time was reduced to less than 3 min by using the pseudo simulator and NSGA II to supplement the PHO-MC model for estimating the IOP values.

[1]  D. Risović Effect of suspended particulate-size distribution on the backscattering ratio in the remote sensing of seawater. , 2002, Applied optics.

[2]  B. A. Engel,et al.  Classification of multispectral remote sensing data using neural networks vs statistical methods. , 1990 .

[3]  Anatoly A. Gitelson,et al.  Remote sensing of chlorophyll in Lake Kinneret using highspectral-resolution radiometer and Landsat TM: spectral features of reflectance and algorithm development , 1995 .

[4]  H. Rief,et al.  Photon transport in three-dimensional structures treated by random walk techniques: Monte Carlo benchmark of ocean colour simulations , 1998 .

[5]  Indrajeet Chaubey,et al.  Evaluation of a hyperspectral optical - Monte Carlo remote sensing model in a water tank study. , 2009 .

[6]  Knut Stamnes,et al.  Parameterization and analysis of the optical absorption and scattering coefficients in a western Norwegian fjord: a case II water study. , 2003, Applied optics.

[7]  Lothar Thiele,et al.  Comparison of Multiobjective Evolutionary Algorithms: Empirical Results , 2000, Evolutionary Computation.

[8]  B. Mitchell,et al.  Comparison of the ocean inherent optical properties obtained from measurements and inverse modeling. , 2001, Applied optics.

[9]  K. Stamnes,et al.  Comparison of numerical models for computing underwater light fields. , 1993, Applied optics.

[10]  Dariusz Stramski,et al.  Estimation of the absorption and backscattering coefficients from inߚwater radiometric measurements , 2000 .

[11]  Dariusz Stramski,et al.  The role of seawater constituents in light backscattering in the ocean , 2004 .

[12]  I. V. Aleshin Optical methods and facilities for expeditious monitoring of the ecological status of sea water , 2001 .

[13]  D. Stramski,et al.  Modeling the optical properties of mineral particles suspended in seawater and their influence on ocean reflectance and chlorophyll estimation from remote sensing algorithms. , 2004, Applied optics.

[14]  R. Arnone,et al.  Deriving inherent optical properties from water color: a multiband quasi-analytical algorithm for optically deep waters. , 2002, Applied optics.

[15]  Sudhanshu Sekhar Panda,et al.  Analysis of remotely sensed aerial images for precision farming. , 2000 .

[16]  H. Gordon,et al.  Radiance-irradiance inversion algorithm for estimating the absorption and backscattering coefficients of natural waters: homogeneous waters. , 1997, Applied optics.

[17]  D. Stramski,et al.  Estimation of the inherent optical properties of natural waters from the irradiance attenuation coefficient and reflectance in the presence of Raman scattering. , 2000, Applied optics.

[18]  Dariusz Stramski,et al.  Optical properties of Asian mineral dust suspended in seawater , 2004 .

[19]  L. Prieur,et al.  A three-component model of ocean colour and its application to remote sensing of phytoplankton pigments in coastal waters , 1989 .

[20]  R. K. Ursem Multi-objective Optimization using Evolutionary Algorithms , 2009 .

[21]  T. Platt,et al.  Remote sensing of phytoplankton pigments: A comparison of empirical and theoretical approaches , 2001 .

[22]  Shubha Sathyendranath,et al.  Variations in the spectral values of specific absorption of phytoplankton , 1987 .

[23]  C. Mobley Light and Water: Radiative Transfer in Natural Waters , 1994 .

[24]  Trevor Platt,et al.  A two‐component model of phytoplankton absorption in the open ocean: Theory and applications , 2006 .

[25]  David McKee,et al.  Estimation of absorption and backscattering coefficients from in situ radiometric measurements: theory and validation in case II waters. , 2003, Applied optics.

[26]  Dariusz Stramski,et al.  Variations in the mass‐specific absorption coefficient of mineral particles suspended in water , 2004 .

[27]  Nicolas Hoepffner,et al.  Determination of the major groups of phytoplankton pigments from the absorption spectra of total particulate matter , 1993 .

[28]  R. Lacroix,et al.  EFFECTS OF DATA PREPROCESSING ON THE PERFORMANCE OF ARTIFICIAL NEURAL NETWORKS FOR DAIRY YIELD PREDICTION AND COW CULLING CLASSIFICATION , 1997 .

[29]  A. Bricaud,et al.  Modeling the inherent optical properties of the ocean based on the detailed composition of the planktonic community. , 2001, Applied optics.

[30]  Dariusz Stramski,et al.  Variations in the light absorption coefficients of phytoplankton, nonalgal particles, and dissolved organic matter in coastal waters around Europe , 2003 .

[31]  E. Fry,et al.  Absorption spectrum (380-700 nm) of pure water. II. Integrating cavity measurements. , 1997, Applied optics.

[32]  Kalyanmoy Deb,et al.  A fast and elitist multiobjective genetic algorithm: NSGA-II , 2002, IEEE Trans. Evol. Comput..

[33]  J R Zaneveld,et al.  In situ determination of the remotely sensed reflectance and the absorption coefficient: closure and inversion. , 1999, Applied optics.

[34]  D. E. Goldberg,et al.  Genetic Algorithm in Search , 1989 .

[35]  K. Baker,et al.  Optical properties of the clearest natural waters (200-800 nm). , 1981, Applied optics.

[36]  John J. Cullen,et al.  Assessment of the relationships between dominant cell size in natural phytoplankton communities and the spectral shape of the absorption coefficient , 2002 .

[37]  T. Platt,et al.  Bio‐optical properties of the Labrador Sea , 2003 .

[38]  S. Maritorena,et al.  Bio-optical properties of oceanic waters: A reappraisal , 2001 .

[39]  Dariusz Stramski,et al.  Light absorption by aquatic particles in the near‐infrared spectral region , 2002 .

[40]  D. K. Ranaweera,et al.  Application of radial basis function neural network model for short-term load forecasting , 1995 .

[41]  Goldberg,et al.  Genetic algorithms , 1993, Robust Control Systems with Genetic Algorithms.

[42]  K. Carder,et al.  Absorption Spectrum of Phytoplankton Pigments Derived from Hyperspectral Remote-Sensing Reflectance , 2004 .