Japan Geoscience Union Meeting 2014

Presentation information

Poster

Symbol A (Atmospheric, Ocean, and Environmental Sciences) » A-HW Hydrology & Water Environment

[A-HW25_2PO1] Isotope Hydrology 2014

Fri. May 2, 2014 4:15 PM - 5:30 PM Poster (3F)

Convener:*Yasuhara Masaya(Geological Survey of Japan, AIST), Kohei Kazahaya(Geological Survey of Japan, AIST), Shinji Ohsawa Shinji(Institute for Geothermal Sciences, Graduate School of Science, Kyoto University), Masaaki Takahashi(Geological Survey of Japan (GSJ), National Institute of Advanced Industrial Science and Technology (AIST)), YUICHI SUZUKI(Faculty of Geo-Environmental Sience,Rissho University), Futaba Kazama(Social Cystem Engineering, Division of Engineering, Interdiciplinary Graduate School of Medical and Engineering, University of Yamanashi), Kazuyoshi Asai(Geo Science Laboratory)

4:15 PM - 5:30 PM

[AHW25-P02] Isotope characteristic of rain water and atmospheric vapor in Hiratsuka, Japan

*Kenta TAKAGI1, Seigo OOKI2, Takeshi OHBA2 (1.Course of Chemistry, Graduate School of Science, Tokai University, 2.Course of Chemistry, School of Science, Tokai University)

Keywords:rain water, isotope

IntroductionThe stable isotope ratios of hydrogen and oxygen in meteoric water (δD and δ18O) are affected by geological and climatic conditions. Global meteoric water line (GMWL) describes the average isotopic compositions in the world. According to Craig (1961), the relationship between δD and δ18O was expressed asδD=8δ18O+10 (1)However those intercept are not always 10 in each area. In Japan, the meteoric water originates in both Pacific Ocean and Japan Sea. The effects of two seas vary due seasonally. The isotope ratio of atmospheric vapor is important for study of atmospheric circulation, however, the number of published paper is not so much. In this study, we investigate the d-excess (d=δD -8δ18O) of rain water and atmospheric vapor in Hiratsuka, Japan.Sampling methodsSamples were collected on the roof of a No.17 building at Shonan campus, Tokai University from May to December 2013. Rain water samples were collected based on a method described by Negrel et al. (2011) and Yoshimura (2002). The collection duration was days or hours in scale. Rain water samples were percolated through 0.2 μm filter, and kept into a 100 ml low-density polyethylene bottle. Atmospheric vapor samples were collected through a trap cooled with ethanol and dry ice mixture. Samples were 42 of rain water and 11 of atmospheric vapor. δD and δ18O of samples were measured by a Cavity Ring-Down Spectrometer analyzer (model L2120-I from PICARRO). Some data of rain water, which were sampled several times in a day, were processed to be the average value.Results and discussionRain water shows a wide variation in δD and δ18O from -86.4 to +6.2 ‰ and -12.6 to -2.6 ‰, respectively. Atmospheric vapor shows a variation from -223.5 to -98.6 ‰ and -31.2 to -14.7 ‰, respectively. The δD-δ18O relationship of rain water gives a regression line: δD=9.2δ18O+24.0 (R2=0.95) and that of atmospheric vapor gives a regression line: δD=7.3δ18O+7.9 (R2=0.96). The d-excess values show a variation from 4.4 ‰ to 33.2 ‰. In Japan, origin of meteoric water affects to d-excess (Waseda and Nakai, 1983). In case of Pacific Ocean, d-excess is low (10≥d). In case of Japan Sea, d-excess is high (20≤d). In this study, the d-excess was low in summer when southern winds were blown from Pacific Ocean as the seasonal wind, and that value was high in winter when northern winds were blown from Japan Sea. Samples of atmospheric vapor show also this trend. Suggesting that atmospheric vapor is influenced by the same effect of meteoric water. The meteoric water line of rain samples was affected by d-excess which reflects variations of moisture sources, which is the reason why the slope of this line would be bigger than GMWL.