Spatiotemporal characteristics of photosynthetically active radiation in China

[1] Photosynthetically active radiation (PAR) plays an important part in climate change and ecological processes. Few PAR measurements are usually available, especially in China. Thus it is important and significant to investigate the spatiotemporal characteristics of PAR in China for radiation budget and ecosystem studies. In order to study the spatiotemporal characteristics of PAR, photosynthetic photon flux density (Qp) and broadband solar radiation (Rs) measurement data were analyzed for the period of January 2005 to June 2006. Qp increases gradually from spring and reaches its maximum and minimum in summer and winter, respectively. The highest value of annual mean daily Qp (40.9 ± 4.1 mol m−2 d−1) appears in the Qinghai-Tibet Plateau region, along with higher atmospheric transmission; and the lowest value (17.4 ± 9.03 mol m−2 d−1) is found in the northern subtropics, along with the largest aerosol optical depth (AOD) and a lower water vapor content. PAR fraction shows a similar seasonal trend as that of Qp at all sites except for some near to lakes and sea. The annual mean daily value of PAR fraction varies from 1.75 ± 0.12 to 2.3 ± 0.15 mol MJ−1 over China. The largest value appears in tropical regions because of higher relative humidity (RH). The lowest value is observed at the Luancheng site, which features low humidity and an abundance of fine aerosols, instead of sites in China's driest northern desert region. The variability of PAR fraction is mainly controlled by the selective scattering of aerosol particles and absorption of water vapor. Two different diurnal trends of PAR fraction are observed in China. In most sites, PAR fraction tends to peak during sunrise or sunset and reaches its lowest value around noon. However, it exhibits an opposite trend in the northern desert area because of the distinctive diurnal variation of water vapor in this region. Further analysis of annual mean hourly PAR fraction shows that the national average is 1.82 ± 0.11 and 2.00 ± 0.08 μmol J−1 for clear and cloudy days, respectively. The cloudy day's ratio is therefore 10% higher than that for clear days. The altitude dependency of PAR fraction is very weak below 1500 m because of uneven distributions of water vapor, clouds, and aerosols. Above 1500 m, PAR fraction increases gradually with altitude on both cloudy and clear days, attributed to the weaker extinction of Qp at higher-altitude sites. The distribution pattern of annual mean daily PAR fraction is similar to that of the hourly value. Its magnitude is medial to the hourly values on cloudy and clear days. These results are helpful for understanding the climatic, agricultural, and ecological processes over China and useful for primary productivity estimation and ecosystem–atmosphere CO2 exchange study in China.

[1]  Xianzhou Zhang,et al.  Measuring and modelling photosynthetically active radiation in Tibet Plateau during April-October , 2000 .

[2]  J. Cañada,et al.  Influences of the clearness index for the whole spectrum and of the relative optical air mass on UV solar irradiance for two locations in the Mediterranean area, Valencia and Cordoba , 2000 .

[3]  C. P. Jacovides,et al.  Ratio of PAR to broadband solar radiation measured in Cyprus , 2004 .

[4]  L. Alados-Arboledas,et al.  Agricultural and Forest Meteorology Photosynthetically Active Radiation: Measurements and Modelling , 1994 .

[5]  Ellen J. Cooter,et al.  A solar radiation model for use in biological applications in the South and Southeastern USA , 1996 .

[6]  C. Gueymard The sun's total and spectral irradiance for solar energy applications and solar radiation models , 2004 .

[7]  Michael Geiger,et al.  A Web service for controlling the quality of measurements of global solar irradiation , 2002 .

[8]  R. Bird,et al.  Simple Solar Spectral Model for Direct and Diffuse Irradiance on Horizontal and Tilted Planes at the Earth's Surface for Cloudless Atmospheres , 1986 .

[9]  Terry A. Howell,et al.  Relationship of photosynthetically active radiation to shortwave radiation in the San Joaquin Valley , 1983 .

[10]  D. Dye Spectral composition and quanta‐to‐energy ratio of diffuse photosynthetically active radiation under diverse cloud conditions , 2004 .

[11]  T. O. Aro,et al.  Global PAR related to global solar radiation for central Nigeria , 1999 .

[12]  Francisco J. Batlles,et al.  Estimation of hourly global photosynthetically active radiation using artificial neural network models , 2001 .

[13]  Stephen D. Prince,et al.  Regional pattern and interannual variations in global terrestrial carbon uptake in response to changes in climate and atmospheric CO2 , 2005 .

[14]  G. Hoogenboom Contribution of agrometeorology to the simulation of crop production and its applications , 2000 .

[15]  Leszek Kuchar,et al.  Estimation of solar radiation for use in crop modelling , 1998 .

[16]  Ernest Hilsenrath,et al.  Observations of the solar irradiance in the 200-350 nm interval during the ATLAS-1 Mission: A comparison among three sets of measurements-SSBUV, SOLSPEC, and SUSIM , 1996 .

[17]  M. Sulev,et al.  Sources of errors in measurements of PAR , 2000 .

[18]  Patrick E. Van Laake,et al.  Mapping PAR using MODIS atmosphere products , 2005 .

[19]  Alexander Smirnov,et al.  Columnar aerosol optical properties at AERONET sites in central eastern Asia and aerosol transport to the tropical mid‐Pacific , 2005 .

[20]  Christian A. Gueymard,et al.  A two-band model for the calculation of clear sky solar irradiance, illuminance, and photosynthetically active radiation at the earth's surface , 1989 .

[21]  Estimation of Photosynthetic Photon Flux Density from 368-nm Spectral Irradiance* , 2004 .

[22]  K. Mccree Test of current definitions of photosynthetically active radiation against leaf photosynthesis data , 1972 .

[23]  Yang Sun,et al.  Aerosol optical depth (AOD) and Angstrom exponent of aerosols observed by the Chinese Sun Hazemeter Network from August 2004 to September 2005 , 2007 .

[24]  D. Retalis,et al.  Photosynthetically active radiation in Athens , 1996 .

[25]  B. Forgan A New Method for Calibrating Reference and Field Pyranometers , 1996 .

[26]  J. Proctor,et al.  Estimating photosynthetically active radiation from measured solar irradiance , 1983 .

[27]  T. Pohlert,et al.  Use of empirical global radiation models for maize growth simulation , 2004 .

[28]  D. M. Gottlieb,et al.  Solar flux and its variations , 1974 .

[29]  Steven S. Cliff,et al.  Asian continental aerosol persistence above the marine boundary layer over the eastern North Pacific: Continuous aerosol measurements from Intercontinental Transport and Chemical Transformation 2002 (ITCT 2K2) , 2005 .