Tropospheric aerosols in the Mediterranean: 1. Microphysical and optical properties

[1] Measurements of the aerosol properties were carried out at the island of Lampedusa, in the Mediterranean, in May 1999, as part of the Photochemical Activity and Ultraviolet Radiation modulating factors II campaign. Data from ground-based lidar and Sun photometer, and particle counters aboard an instrumented ultralight aircraft, are used in this study. Three different cases, when all the measurements were available in cloud-free conditions, were identified to derive the aerosol microphysical and optical properties. In one of these cases (18 May) the airmasses originated from Africa, and were loaded with a large amount of desert dust. In the other two cases (25 May and 27 May) the airmasses passed over Europe before reaching Lampedusa from North. The microphysical and optical properties of the aerosol strongly depend on the origin of the airmasses. The amount of particles in the 1–6 μm range of radii and the average aerosol surface area per unit volume are larger in the desert dust case than on 25 May and 27 May. The real part of the refractive index of the desert dust at 532 nm is between 1.52 and 1.58; its imaginary part is 5–7 × 10−3 and the single scattering albedo is about 0.7–0.75. The aerosol layer of 18 May closest to the surface, that probably contains a mixture of desert dust and marine aerosol, displays a smaller imaginary part (1.2 × 10−3) and a larger single scattering albedo (0.91). The aerosols originating from the North Atlantic and Europe have a real part of the refractive index between 1.35 and 1.49, and an imaginary part ranging from 8 × 10−4 to 1.8 × 10−2; the single scattering albedo at 532 nm (0.78–0.95) is larger than for desert dust values. The smallest value of the single scattering albedo (0.69) corresponds to an airmass originating from North, characterized by a large imaginary part of the refractive index. The asymmetry factor of the desert dust appears consistently larger for the desert dust (0.75–0.8) than for the other cases (0.61–0.72). The extinction-to-backscattering ratio, also derived from the measurements, is about 40 sr for the desert dust, and between 60 and 81 sr for the aerosol of northern origin. Simple estimates of the aerosol average direct shortwave radiative forcing at the top of the atmosphere indicate that all considered aerosol types induce a cooling. The radiative forcing per unit optical depth of the aerosol originating from North is about −37 Wm−2 over ocean and −(12–17) Wm−2 over land, while is −29 Wm−2 over ocean and −8 Wm−2 over land for desert dust. The largest forcing is however produced by the desert aerosols that generally display a considerably larger optical depth.

[1]  Irina N. Sokolik,et al.  Direct radiative forcing by anthropogenic airborne mineral aerosols , 1996, Nature.

[2]  E. M. Patterson,et al.  Commonalities in measured size distributions for aerosols having a soil-derived component , 1977 .

[3]  W. Junkermann,et al.  An Ultralight Aircraft as Platform for Research in the Lower Troposphere: System Performance and First Results from Radiation Transfer Studies in Stratiform Aerosol Layers and Broken Cloud Conditions , 2001 .

[4]  James E. Dye,et al.  Evaluation of the Forward Scattering Spectrometer Probe. Part I: Electronic and Optical Studies , 1984 .

[5]  D. Baumgardner,et al.  An Analysis and Comparison of Five Water Droplet Measuring Instruments. , 1983 .

[6]  M. Garstang,et al.  Temporal and spatial characteristics of Saharan dust outbreaks , 1996 .

[7]  R. G. Pinnick,et al.  Calibration of Knollenberg FSSP Light-Scattering Counters for Measurement of Cloud Droplets , 1981 .

[8]  B. Marticorena,et al.  Two-year simulations of seasonal and interannual changes of the Saharan dust emissions , 1996 .

[9]  P. Bhartia,et al.  Global distribution of UV-absorbing aerosols from Nimbus 7/TOMS data , 1997 .

[10]  J. Deluisi,et al.  Results of a Comprehensive Atmospheric Aerosol-Radiation Experiment in the Southwestern United States. Part II: Radiation Flux Measurements and Theoretical Interpretation , 1976 .

[11]  G. Fiocco,et al.  Saharan dust profiles measured by lidar at Lampedusa , 2001 .

[12]  M. Andreae,et al.  Uncertainty in Climate Change Caused by Aerosols , 1996, Science.

[13]  James E. Dye,et al.  Evaluation of the forward scattering spectrometer probe. Part II: Corrections for coincidence and dead-time losses , 1985 .

[14]  J. Michalsky,et al.  Automated multifilter rotating shadow-band radiometer: an instrument for optical depth and radiation measurements. , 1994, Applied optics.

[15]  François Dulac,et al.  Long‐term daily monitoring of Saharan dust load over ocean using Meteosat ISCCP‐B2 data: 1. Methodology and preliminary results for 1983–1994 in the Mediterranean , 1997 .

[16]  G. Fiocco,et al.  Lidar observations of the Pinatubo aerosol layer at Thule, Greenland , 1994 .

[17]  B. A. Bodhaine,et al.  Optical absorption by aerosol black carbon and dust in a desert region of Central Asia , 1993 .

[18]  J. Lelieveld,et al.  Role of mineral aerosol as a reactive surface in the global troposphere , 1996 .

[19]  D. Baumgardner,et al.  Evaluation of the Forward Scattering Spectrometer Probe. Part III: Time Response and Laser Inhomogeneity Limitations , 1990 .

[20]  J. Herman,et al.  Detection of mineral dust over the North Atlantic Ocean and Africa with the Nimbus 7 TOMS , 1999 .

[21]  Beat Schmid,et al.  Retrieving the vertical structure of the effective aerosol complex index of refraction from a combination of aerosol in situ and remote sensing measurements during TARFOX , 2000 .

[22]  E. M. Patterson,et al.  Complex Index of Refraction Between 300 and 700 nm for Saharan Aerosols , 1977 .

[23]  Stanley G. Benjamin,et al.  Radiative Heating Rates for Saharan Dust , 1980 .

[24]  Zev Levin,et al.  Size distribution, chemical composition, and optical properties of urban and desert aerosols in Israel , 1979 .

[25]  M. Mishchenko,et al.  APPLICATION OF THE T-MATRIX METHOD TO THE MEASUREMENT OF ASPHERICAL (ELLIPSOIDAL) PARTICLES WITH FORWARD SCATTERING OPTICAL PARTICLE COUNTERS , 2000 .

[26]  Y Sasano,et al.  Tropospheric aerosol optical properties derived from lidar, sun photometer, and optical particle counter measurements. , 1994, Applied optics.

[27]  J. Seinfeld,et al.  Radiative forcing by mineral dust aerosols : sensitivity to key variables , 1998 .

[28]  F. Prodi,et al.  A case of transport and deposition of Saharan dust over the Italian Peninsula and southern Europe , 1979 .

[29]  Toby N. Carlson,et al.  Vertical and areal distribution of Saharan dust over the western equatorial north Atlantic Ocean , 1972 .

[30]  Y. J. Kim,et al.  Corrections for the Effects of Particle Trajectory and Beam Intensity Profile on the Size Spectra of Atmospheric Aerosols Measured with a Forward Scattering Spectrometer Probe , 1990 .

[31]  H. Maring,et al.  Aerosol physical and optical properties and their relationship to aerosol composition in the free troposphere at Izaña, Tenerife, Canary Islands, during July 1995 , 2000 .

[32]  D. Tanré,et al.  Assessment of the African airborne dust mass over the western Mediterranean Sea using Meteosat data , 1992 .

[33]  Alexandros Papayannis,et al.  Characterization of the vertical structure of Saharan dust export to the Mediterranean basin , 1999 .

[34]  P. Russell,et al.  Complex Index of Refraction of Airborne Soil Particles , 1974 .

[35]  P. Disterhoft,et al.  Effects of desert dust and ozone on the ultraviolet irradiance at the Mediterranean island of Lampedusa during PAUR II , 2002 .

[36]  Y. J. Kim,et al.  Size Calibration Corrections for the Forward Scattering Spectrometer Probe (FSSP) for Measurement of Atmospheric Aerosols of Different Refractive Indices , 1990 .

[37]  Mian Chin,et al.  Contribution of different aerosol species to the global aerosol extinction optical thickness: Estimates from model results , 1997 .

[38]  G. d’Almeida,et al.  A model for Saharan dust transport , 1986 .

[39]  Giorgio Fiocco,et al.  Tropospheric aerosols in the Mediterranean: 2. Radiative effects through model simulations and measurements , 2003 .

[40]  Mark R. Schoeberl,et al.  The structure of the polar vortex , 1992 .

[41]  Larry L. Stowe,et al.  Characterization of tropospheric aerosols over the oceans with the NOAA advanced very high resolution radiometer optical thickness operational product , 1997 .

[42]  J. Rosen,et al.  Measurement of extinction‐to‐backscatter ratio for near‐surface aerosols , 1997 .

[43]  S. K. Satheesh,et al.  Large differences in tropical aerosol forcing at the top of the atmosphere and Earth's surface , 2000, Nature.

[44]  E. Patterson Optical properties of the crustal aerosol - Relation to chemical and physical characteristics , 1981 .

[45]  J. Joseph,et al.  Properties of Sharav (Khamsin) Dust–Comparison of Optical and Direct Sampling Data , 1980 .

[46]  Jonathan P. Taylor,et al.  Optical properties and direct radiative effect of Saharan dust: A case study of two Saharan dust outbreaks using aircraft data , 2001 .

[47]  P. Disterhoft,et al.  Radiation, ozone and aerosol measurements at Lampedusa during the PAUR-II campaign , 2001 .

[48]  J. P. Díaz,et al.  Radiative properties of aerosols in Saharan dust outbreaks using ground‐based and satellite data: Applications to radiative forcing , 2001 .

[49]  Eric P. Shettle,et al.  Atmospheric Aerosols: Global Climatology and Radiative Characteristics , 1991 .

[50]  J. Coakley,et al.  Climate Forcing by Anthropogenic Aerosols , 1992, Science.

[51]  Z. Levin,et al.  The Effects of Desert Particles Coated with Sulfate on Rain Formation in the Eastern Mediterranean , 1996 .

[52]  P. Pilewskie,et al.  Pinatubo and pre‐Pinatubo optical‐depth spectra: Mauna Loa measurements, comparisons, inferred particle size distributions, radiative effects, and relationship to lidar data , 1993 .