Japan Geoscience Union Meeting 2015

Presentation information

Poster

Symbol A (Atmospheric and Hydrospheric Sciences) » A-HW Hydrology & Water Environment

[A-HW24] Isotope Hydrology 2015

Mon. May 25, 2015 6:15 PM - 7:30 PM Convention Hall (2F)

Convener:*Masaya Yasuhara(Geological Survey of Japan, AIST), Kohei Kazahaya(Geological Survey of Japan, AIST), Shinji Ohsawa(Institute for Geothermal Sciences, Graduate School of Science, Kyoto University), Masaaki Takahashi(The National Institute of Advanced Industrial Science and Technology), 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)

6:15 PM - 7:30 PM

[AHW24-P01] Stable isotopic ratio of atmospheric vapor in Hiratsuka, Japan

*Kenta TAKAGI1, Takayuki INOUE2, Seigo OOKI2, Takeshi OHBA2 (1.Course of Chemistry, Graduate School of Science, Tokai University, 2.Course of Chemistry, School of Science, Tokai University)

Keywords:Precipitation, Atmospheric vapor, Stable isotope

The origin of water vapor in atmosphere could be variable, for example, the water vapor at a specific point is transported from a distance or the vapor is generated from surface water near the specific point. If there is equilibrium between precipitation and atmospheric vapor, the hydrogen and oxygen isotope ratios (δD and δ18O) of atmospheric vapor are plotted theoretically in meteoric water line. Recently, δD and δ18O of atmospheric vapor is used as a tracer for atmospheric water cycle, because the water vapor is much ubiquitous than precipitation (Tsunakawa and Yamanaka, 2005). However, Japan has various water resources. From this aspect, δD and δ18O of atmospheric vapor could be disturbed by several factors such as seasonal variation and difference vapor source of supply (Hiyama et al, 2008). In this study, we investigated the seasonal isotopic variation of atmospheric vapor and precipitation. Then, we also examined surface water on ground and transpiration from leaves of plants, as the candidates of atmospheric vapor sources.
Precipitation and atmospheric vapor were collected on the roof of a No.17 building at Shonan campus, Tokai University from May 2013 to Dec. 2014. Precipitation samples were collected based on the method described by Negrel et al. (2011) and Yoshimura (2002). The duration of collection varied from hours to days. Precipitation samples were percolated through 0.2 μm filter, and kept into a 100 ml low-density polyethylene bottle. Atmospheric vapor samples were collected by the cryogenic trap cooled with ethanol-dry ice mixture (Tsunakawa and Yamanaka, 2005). The total number of precipitation and atmospheric vapor samples were 142 and 90, respectively. The atmospheric vapor may be supplied by surface water on ground and transpiration from leaves of plants, therefore surface water samples were collected on 4 points (pond or river) near a No.17 building from Apr. to Dec. 2014. Transpiration samples were collected at 6 points near a No.17 building from Aug. to Dec. 2014 by polyethylene bag which covers leaves and twig over 1-4 days. Surface water and transpiration samples were percolated through 0.2 μm filter, and kept into a low-density polyethylene bottle. The total number of surface water samples was 6 in each points and the total number of transpiration samples were 16. 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 weighted average value.
Precipitation showed wide variations in δD and δ18O from -124.7 to +9.1 ‰ and -16.6 to -0.6 ‰, respectively. Atmospheric vapor also showed wide variations from -223.5 to -82.2 ‰ and -31.2 to -11.6 ‰, respectively. The δD-δ18O relationship of precipitation and atmospheric vapor were regressed by δD=8.5δ18O+17.4 (R2=0.95) and δD=6.6δ18O-2.6 (R2=0.92), respectively. The d-excess values (d=δD-8δ18O) of precipitation has a variation from -0.7 to 31.4 ‰. The d-excess of atmospheric vapor shows a definite seasonal trend within the range between 5.6 and 35.7 ‰. The isotopic compositions of atmospheric vapor almost agreed to the calculated value from precipitation assuming isotopic equilibrium with the exception in May 2014, where a significant difference between the observed and the calculated isotopic ratios. Such a composition seemed to be generated by the completely evaporated vapor originating in precipitation (= bulk vapor). In Jun. 2014, the d-excess of atmospheric vapor was deviated from the seasonal variation. Such a deviation can be caused by the addition of evaporated vapor from local surface water. The δD-δ18O plots of all sample suggested that atmospheric vapor was mainly composed by three kinds of vapor, namely, the vapor equilibrated with precipitation, the bulk vapor and the vapor evaporated from the local surface water near the observation point.