Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012

Size: px
Start display at page:

Download "Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012"

Transcription

1 [Technical report] Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012 Mahito ITO * Osamu IJIMA * Tetsuya SHIMAMURA * Itaru UESATO * Yoshiyuki NOTO * Yuji ESAKI * Noriaki OSHIKI * Abstract Since December 2003, monitoring observations of spectral ultraviolet (UV) radiation reflected from the ground surface (RFuv) have been carried out at the Aerological Observatory in Tsukuba with a modified Brewer spectrophotometer, BR#059. Similar monitoring of diffuse spectral UV (DFuv) from the sky has been carried out with a Brewer spectrophotometer, BR#058, with an automated shadow unit, since August 2005 (Ito: 2004, 2006, 2007). In this paper, the results of these measurements are compared with global spectral UV (GLuv) and solar radiation data, GLsolar, DFsolar, and RFsolar, from 2004 to The results are summarized below. (1) The monthly means of daily totals of GLuv, DFuv, and RFuv showed seasonal patterns different from GLsolar, DFsolar, and RFsolar, respectively. (2) The annual means of the daily total of DFuv have been increasing by small amounts from year to year since 2006, in contrast to the almost constant DFsolar. (3) The annual and monthly means of the daily total of RFuv are affected by UV absorption by vegetation and reflection from snow, but vegetation and snow had little effect on the means of RFsolar. (4) The monthly mean of daily UV diffusibility, RDFuv (DFuv/GLuv), averaged about 0.84 (84%) and was almost constant throughout the year, but the diffusibility of solar radiation, RDFsolar (DFsolar/GLsolar), averaged about 0.61 (61%) and showed seasonal variations. (5) The annual means of monthly means of daily UV reflectivity, RRFuv (RFuv/GLuv), averaged only about 0.02 (2%), compared to the average of about 0.21 (21%) for daily solar reflectivity, RRFsolar (RFsolar/GLsolar). The spectrum of RRFuv exhibited a small linear wavelength dependence, with higher reflectivity at longer wavelengths. (6) The contributions (percentages) of the daily totals of direct UV radiation, DRuv (GLuv DFuv), DFuv, and RFuv relative to the daily total of GLuv, averaged about 20%, 80%, and 2%, respectively. In contrast, their contributions to the daily totals of DRsolar, DFsolar, and RFsolar relative to the daily total of GLsolar were different and averaged about 50%, 50%, and 20%, respectively. The differences between the seasonality of the components of UV radiation, GLuv, DFuv, and RFuv, and the components of solar radiation, GLsolar, DFsolar, and RFsolar, were elucidated. Continuous observations with Brewer spectrophotometers are very important for, inter alia, ground truth calibration of satellite observations, clarification of aerosol distributions, and studies of vegetation growth. 1. Introduction A spectral ultraviolet (UV) radiation monitoring network using Brewer spectrophotometers has been maintained by the Japan Meteorological Agency (JMA) at Tsukuba since 1990; at Sapporo, Kagoshima, and Naha since 1991; and at Syowa in Antarctica since 1991 (Ito et al.: 1991). Many characteristics of global UV at the surface of the earth have been clarified by these observations. However, the potential effects of UV radiation on the human body under cloudy conditions is also a concern, because the UV radiation is reflected from the ground surface and scattered by aerosols and cloud particles in the sky (MOE: 2004). The Aerological Observatory therefore started spectral UV observations at Tsukuba of diffuse UV radiation (DFuv) and reflected UV radiation (RFuv) in addition to global UV radiation (GLuv). Observations of RFuv were begun with a modified Brewer MKII * Ozone and Radiation Division, Aerological Observatory, JMA. spectrophotometer in December 2003 (Ito: 2004, 2005a). These observations clarified several different results: (1) the RFuv evidenced a seasonal pattern different from the GLuv. The RFuv intensity was high in March to April and low in December to January, with a period of relatively high intensity from July to August, and (2) the UV reflection ratio, RRFuv (RFuv/GLuv), evidenced a different seasonal pattern because the RFuv was high from January to April and low from June to September (Ito: 2007). Observations of DFuv were started by using an automated shadow unit in August 2005, after experimental observations using manually controlled shadow units (Ito: 2005b, 2006). These observation revealed several results: (1) the DFuv evidenced a different seasonal pattern of high intensity from May to August and low intensity from December to January, and (2) the ratio of UV diffusibility, RDFuv (DFuv/GLuv), was high from June to July and January to February and low from March to September (Ito: 2007). Observations of these three UV components, GLuv, DFuv, and

2 Journal of the Aerological Observatory No Photo 1. Observation site and instruments used. A: Brewer spectrophotometers for GLuv (global UV radiation) observations. B: BR#058 for DFuv (diffuse UV radiation) observations. C: BR#059 for RFuv (reflected UV radiation) observations. D: Pyranometers and pyrheliometers for DFsolar (diffuse solar radiation) and DRsolar (direct solar radiation) observations. E: Pyranometers for RFsolar (reflected solar radiation) observations at the BSRN network site. Table 1 Contents of observation and data. Radiation Symbol Contents GL uv Global UV radiation J/m 2 RF uv Reflected UV radiation J/m 2 DF uv Diffuse UV radiation J/m 2 DR uv Direct UV radiation on the horizontal surface J/m 2 UV RRF uv Reflectivity of UV radiation [RRFuv=RFuv/GLuv] Radiation RDF uv Diffusibility of UV radaition [RDFuv=DFuv/GLuv] UVB Total UV irradiance at the wavelength Fig. 1 Data records and instruments used in this report. RFuv, were continued. The DFuv data were collected for about 8 years, from 2005 to 2012, and the RFuv data were collected for about 9 years, from 2004 to The basic GLuv data were collected for about 23 years, from 1990 to All of these data were sent to the data centre of the WMO/WOUDC. In this paper, the seasonal patterns and inter-annual changes of DFuv, RFuv, and GLuv have been compared and analyzed with respect to three components of solar radiation: global solar radiation (GLsolar), diffuse solar radiation (DFsolar), and reflected solar radiation (RFsolar). The symbols used in this paper are defined in Table 1. Please refer to Ito (2007) for detailed descriptions of the instruments and the observational methods, and to McElroy et al. (2008) and Kipp & Zonen (1996, 2008a, b) for all of the technical terms used in this paper. 2. Instrumental and observational data 2.1 Instruments The GLuv was observed with a Brewer spectrophotometer BR#052, a BR#173, and a BR#200; DFuv, with a BR#058 with from to nm J/m 2 CIE CIE UV irradiance by Commission Internationale de I'Eclairage J/m 2 GL solar Global solar radiation kj/m 2 RF solar Reflected solar radiation kj/m 2 Solar DF solar Diffuse solar radiation kj/m 2 Radiation DR solar Direct solar radiation on the horizontal surface kj/m 2 RRF solar Reflectivity of solar radiation [RRFsolar=RFsolar/GLsolar] RDF solar Diffusibility of solar radiation [RDFsolar=DFsolar/GLsolar] (DRuv=GLuv-DFuv, GLsolar=DFsolar+DRsolar) automated shadow units; and RFuv, with a modified BR#059. The GLuv and the DFuv were observed on the rooftop of a building, and RFuv was observed above a field of grass at the observation site. The size of the shadow ball and the length of the shadow frame of the shadow units for the DFuv observations made with a BR#058 were based on a standard protocol (WMO: 1996, Ohmura: 2002, BSRN: 2002). The distance of 180 cm between the diffuser in the UV dome and the surface of the ground for the RFuv observations with a BR#059 was based on standard protocol (WMO: 1996). The instruments and field are shown in Photo 1 (A to C). For the observations of solar radiation, GLsolar was defined to be the value of DFsolar + DRsolar on a horizontal surface detected by the pyranometer CM22 (CM21) and the pyrheliometer CH1-52 -

3 Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012 (AOT/JMA: 1996). These observation sites were also on the rooftop. Pyranometer CM21 was also used for the observations of RFsolar on the observation field. The instruments and the field are shown in Photo 1 (D and E). Figure 1 provides a summary of the use of these instruments for data collection. 2.2 Observation and data The uv.rtn and the skc.rtn modified by time-control for the product of data every time were used for the observation schedules of GLuv, DFuv, and RFuv. The annual means, the monthly means, the daily totals of the integrated values of UVB and CIE in Table 1, and the spectral irradiances at wavelength intervals of 0.5 nm from 290 to 325 nm were produced by using those data. The spectrophotometer data were corrected to ensure a high degree of accuracy by using the results of regular external lamp tests. The errors associated with the process of narrowing the open sky area with the shadow units for BR#058, and the errors associated with changes in instrumental responsivity due to the reversal of BR#059, were included in the NIST lamp calibration errors (Ito: 2004, 2005b, 2007). The GLsolar, DFsolar, and RFsolar data were sampled every second and averaged every minute. The annual means, the monthly means, and the daily totals of these solar radiation data were generated by using those data as well as the above UV products. In the comparative analysis, the irradiance ratios of RDFuv (DFuv/GLuv), RRFuv (RFuv/GLuv), RDFsolar (DFsolar/GLsolar), and RRFsolar (RFsolar/GLsolar) were calculated with these data. In addition, monthly means of GLuv/GLsolar, DFuv/DFsolar, and RFuv/RFsolar were calculated from the daily means to investigate the ratio of UV to solar radiation. The results are consequently slightly different from the data generated by using the monthly means of the daily totals. In the comparison with the amount of solar radiation, as a matter of convenience we interpreted the amount of UV observed spectrophotometrically (290 to 325 nm) to be part of the solar radiation, although the measurable wavelength range of pyranometers CM22 and CM21 was stated to be 305 to 2800 nm, and that of the pyrheliometer was 200 to 4000 nm. Those monthly and annual means are shown in Fig. 2 (a-1) to (e-5). The dark blue lines in the figure indicate the annual means. The normal 9-year averages of the monthly means (DF: the 8-years average) are shown Fig. 3 (a-1) to (e-5). The dark black lines in the figure indicate the normal 9-year averages of monthly means, and the thin lines indicate the monthly means every year. In the graphs of RF and RRF, the monthly means for 2007 without snow cover are shown as the heavy dotted lines. 3. GLuv, DFuv, RFuv, RDFuv, and RRFuv 3.1 GLuv and GLsolar The seasonal pattern and the inter-annual changes of GLuv were similar to those of GLsolar in Fig. 2 (a-1), (b-1), and (c-1). But a small difference between GLsolar and GLuv is apparent. The maxima of GLsolar were scattered among the months from April to August, whereas the maximum of GLuv was concentrated in the months of July and August. The minima of GLsolar were scattered within the months from October to December, whereas the minimum of GLuv was concentrated in December, the month when the solar zenith angle is a maximum. As shown in Fig. 3 (a-1), (b-1), and (c-1), the normal averages of the 9-year monthly means, the annual time series of GLsolar followed a bimodal pattern with peaks in May and August. In contrast, the annual time series of GLuv followed a unimodal pattern with a single peak in August. We estimate that this difference of maximum month (peak) reflects the fact that (1) the rainy season comes in June, when the solar zenith angle is a minimum at Tsukuba, and (2) the maximum total ozone occurs in April during the spring season, and the total ozone becomes a minimum from September to October during the autumn at Tsukuba. In contrast, the GLsolar irradiance is a minimum in December, when the intensity is about 50% of the maximum value in May and August, but the GLuv irradiance is a minimum in December, when the intensity is only about 20% of the maximum value in August. The inter-annual change of GLsolar shown by the dark blue line in Fig. 2 indicates that there was a local minimum in 2006 and that there has been a pattern of small increases since The GLuv also evidences a similar trend. 3.2 DFuv and DFsolar As shown in Fig. 2 (a-2), (b-2), and (c-2), the seasonal pattern and inter-annual changes of DFuv were almost the same as those of DFsolar. Although DFsolar reached a maximum during the period from June to July, DFuv reached a maximum during the period from July to August. This difference could reflect the fact that DFuv is affected by total ozone. In contrast, the minima of DFsolar were slightly scattered from December to January. However, the minimum of DFuv was concentrated in December, because total ozone increased from January. The annual time series of DFsolar shown in Fig. 3 (a-2) followed a unimodal pattern with a peak in June, the month when the solar zenith angle is lowest, and no effects of the rainy season on the seasonal pattern were apparent. The annual time series of DFuv followed a unimodal pattern with a peak in August, similar to the GLuv time series

4 Journal of the Aerological Observatory No Notes Instruments GLsolar: shaded pyranometer CM21(CM22) and pyrheliometer CH1. DFsolar: shaded pyranometer CM21(CM22.) RFsolar: pyranometer CM21. GLuv: BR#052 (#173, #200). DFuv: shaded BR#058. RFuv: modified BR#059. Middle blue lines in every figure: Annual means. Fig. 2 Monthly and annual means of daily total irradiance, daily diffusibility, and daily reflectivity at Tsukuba from 2004 to (a-1) GLsolar: Global solar radiation (kj/m 2 ). (a-2) DFsolar: Diffuse solar radiation (kj/m 2 ). (a-3) RFsolar: Reflected solar radiation (kj/m 2 ). (a-4) RDFsolar: Diffusibility of solar radiation (DFsolar/GLsolar). (a-5) RRFsolar: Reflectivity of solar radiation (RFsolar/GLsolar). (b-1) GLuv: Global UV (UVB) radiation (J/m 2 ). (b-2) DFuv: Diffuse UV (UVB) radiation (J/m 2 ). (b-3) RFuv: Reflected UV (UVB) radiation (J/m 2 ). (b-4) RDFuv: Diffusibility of UV (UVB) radiation (DFuv/GLuv). (b-5) RRFuv: Reflectivity of UV (UVB) radiation (RFuv/GLuv). (c-1) to (c-5) The same variables as in (b-1) to (b-5), but for UV (CIE) radiation. (d-1) The contribution of global UV (UVB) radiation to global solar radiation (GLuv/GLsolar). (d-2) The contribution of diffuse UV (UVB) radiation to diffuse solar radiation (DFuv/DFsolar). (d-3) The contribution of reflected UV (UVB) radiation to reflected solar radiation (RFuv/RFsolar). (e-1) to (e-3): The same variables as in (d-1) to (d-3), but for UV (CIE) radiation

5 Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012 Notes Thin lines: Monthly means in every year. Heavy lines: Average of the monthly means for the observation periods. Heavy dotted lines of green color in (a-3), (a-5), (b-3), (b-5), (c-3) and (c-5), shows the monthly means in the year without snow cover day, Fig. 3 Seasonal change of monthly means of daily total irradiance, daily diffusibility, and daily reflectivity at Tsukuba from 2004 to Caption shared with Fig. 2. Figures (a-1) to (c-5) show seasonal changes every year and the average of the changes, as in Fig

6 Journal of the Aerological Observatory No The annual averages of DFsolar were almost constant from year to year, but the inter-annual change of DFuv evidenced a small increasing pattern. The reason for this small increase is unclear. 3.3 RFuv and RFsolar As indicated in Fig. 2 (a-3), (b-3), and (c-3), the seasonal pattern and the inter-annual changes of RFuv followed almost the same pattern as RFsolar. But a small difference between RFsolar and RFuv was apparent. The maxima of RFsolar were scattered among two periods during the months of April to May and July to August, whereas the maxima of RFuv were widely scattered in the months from January to August and were affected by the degrees of snow cover. Except for days of snow cover, the maxima of RFuv were scattered in the months from April to August, very similar to the maxima of RFsolar. The minima of RFsolar were scattered within the months from October to December, whereas the minimum of RFuv was concentrated in December. The annual time series of RFsolar shown in Fig. 3 (a-3) followed a bimodal pattern with peaks in April and August. This seasonal pattern is similar to the seasonal pattern of GLsolar. In contrast, the annual time series of RFuv in Fig. 3 (b-3) and (c-3) followed a bimodal pattern, but the local maximum irradiance in April was larger than the local maximum irradiance in August. The RFuv irradiance during the period from January to March was not reduced because of snow cover. In 2007, when there was no snow cover, the RFuv irradiance in January was slightly larger compared to the irradiance in December and increased till April (the time when there was a local maximum). The inter-annual changes of RFsolar evidenced a local minimum in 2006, similar to the inter-annual changes of GLsolar, and have increased by a small amount since In contrast, the RFuv evidenced a local minimum from 2007 to 2009 because of snow cover and has increased since RDFuv and RDFsolar The RDFsolar irradiance ratio shown in Fig. 2 (a-4) evidences a maximum intensity of about 0.8 and intensity minima of about 0.4 scattered from December to February. In contrast, the values of RDFuv in Fig. 2 (b-4) and (c-4) evidence an almost constant and high value of about 0.83 during the entire period of observations. The maxima of RDFuv were widely scattered during the months from June to December with a peak value of about 0.88, and the minima were very widely scattered during the months from December to August, the lowest values being 0.63 to The annual time series of RDFsolar shown in Fig. 3 (a-4) followed a bimodal pattern characterized by peaks in June (about 0.78) and October (about 0.64). The minimum occurred in January (about 0.42). The difference between the maximum and minimum ratios indicates an intensity of about 0.36 (36%). The seasonal pattern of RDFuv shown in Fig. 3 (b-4) and (c-4) shows very small variations, without any remarkable maximum or minimum. The RDFuv irradiance ratio remained at a high intensity of throughout year. Very small local maxima occurred in June (about 0.84) and October (about 0.88), and very small minima occurred in April (about 0.81) and August (about 0.82). The difference between the maximum and minimum ratios indicates an intensity of about 0.07 (7%). This difference was discernible every year. The inter-annual changes of RDFsolar evidence a local maximum in 2006 (about 0.64). From 2006, the RDFsolar decreased by a small amount to about In contrast, the RDFuv evidenced a small local minimum from 2007 to 2008 (about 0.82). The RDFuv at other times was almost constant, the intensity being about RRFuv and RRFsolar The RRFsolar irradiance ratio shown in Fig. 2 (a-5) evidenced a maximum intensity of and intensity minima of about 0.18 that were scattered during the month of May. In contrast, the RRFuv shown in Fig. 2 (b-5) and (c-5) evidenced a wide variation of intensities, from to 1.10, the maxima being scattered within the time interval from December to April. The maximum intensities were affected by the number of consecutive days with snow cover. In 2007, when there was no snow cover, the maximum irradiance ratio corresponded to an intensity of about in March. In contrast, the ratio associated with the scattered minima from June to October corresponded to an intensity of about The annual time series of RRFsolar shown in Fig. 3 (a-5) was unimodal with a maximum in January (about 0.24) and a minimum in May (about 0.18). The difference between the maximum and minimum ratios indicates a very small intensity of about 0.06 (6%). This difference was discernible every year. In contrast, the annual time series of RRFsolar shown in Fig. 3 (b-5) and (c-5) was unimodal with a maximum in January (about 0.042) and a minimum in July (about 0.012). This difference between the maximum and minimum ratios indicates a small intensity of about 0.03 (3%). In 2007, the year without a single day of snow cover, the RRFuv irradiance ratio increased to a maximum in May (about 0.019) and decreased to a minimum in July (about 0.012). The difference between the maximum and minimum ratios indicates a very small intensity of about (0.7%). In 2007, the seasonal pattern of RRFuv was affected by the growing conditions of the grass, because the length of grass is shortest in May and longest from July to August

7 Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012 The inter-annual changes of the RRFsolar irradiance ratio evidenced a pattern of very small increases from 2004 (about 0.18) to 2012 (about 0.21). In contrast, the RRFuv evidenced a small local maximum in 2006 (about 0.03), a small local minimum in 2007 (about 0.015), and a pattern of small increases since 2007, the intensity in 2012 being about GLuv/GLsolar, DFuv/DFsolar, and RFuv/RFsolar 4.1 GLuv/GLsolar As indicated in Fig. 2 (d-1) and (e-1), the maxima of the GLuv/GLsolar irradiance ratios were concentrated in the period from July to August, and the minima were concentrated in the period from December to January. In Fig. 3 (d-1) and (e-1), the annual time series of GLuv/GLsolar was unimodal, with a maximum in July (UVB: , CIE: ) and a minimum in January (UVB: , CIE: ). The differences between the maximum and minimum ratios indicates that the intensities were about (0.09%) for UVB and about (0.01%) for CIE. These differences were discernible every year. The inter-annual changes of the GLuv/GLsolar irradiance ratio evidenced a small minimum in 2005, but the ratio has been almost constant since DFuv/DFsolar As indicated in Fig. 2 (d-2) and (e-2), the DFuv/DFsolar irradiance ratios have been remarkably different in each year. The maximum has occurred in August, and the minima have been scattered from December to February. As indicated in Fig. 3 (d-2) and (e-2), the annual times series of DFuv/DFsolar has been triangular, with a maximum in August (UVB: , CIE: ) and a minimum in December (UVB: , CIE: ). The difference between the maximum and minimum ratios indicates intensities of about (0.07%) for UVB and about (0.01%) for CIE. A small local maximum occurs in May. However, the seasonal changes in every year evidence patterns different from the above average pattern for observations during the 8-year study period. The inter-annual changes of the DFuv/DFsolar irradiance ratio evidence very small minima in 2006 and 2008, and a small increase in intensities since The reason for the increasing intensities is the almost constant intensity of DFsolar and the small increase of DFuv discussed in section 3.2. occurred from December to January. The annual time series of RFuv/RFsolar was trapezoidal, as shown in Fig. 3 (d-3) and (e-3), with a maximum in April (UVB: , CIE: ) and a minimum in December (UVB: , CIE: ). The difference between the maximum and minimum ratios indicates that the intensities were about (0.006%) for UVB and about (0.0006%) for CIE. Small local maxima occurred in July. Inter-annual changes in the RFuv/RFsolar irradiance ratio evidenced local maxima in 2005, 2008, and Those local maxima were due to the small increase of RFuv caused by snow cover, as discussed in section Spectral irradiances and spectral ratios 5.1 Monthly spectral irradiances and monthly spectral ratios The GLuv, DFuv, and RFuv monthly spectral irradiances and the RDFuv and RRFuv monthly spectral ratios from 2004 to 2012 at Tsukuba are shown in Fig. 4 (1) to (3) and in Fig. 4. (4) and (5), respectively. Heavy lines in the figures show the averages for the observation period in 9 (DF: 8) years. The GLuv and DFuv monthly spectral irradiances in Fig. 4 (1) and Fig. 4 (2), respectively, were characterized by a maximum from June to August and a minimum in December. The DFuv irradiance intensity was about 80% of the GLuv irradiance intensity. In contrast, the RFuv monthly spectral irradiance in Fig. 4 (3) was characterized by a maximum from January to April and a minimum from October to December. The RFuv irradiance intensity was about 2% of the GLuv irradiance intensity. The monthly RDFuv spectral ratios shown in Fig. 4 (4) all fell within the range The wave-like lines in the figure may reflect small wavelength shifts in the BR#058 spectrophotometer used to make the DFuv observation. The monthly RRFuv spectral ratios shown in Fig. 4 (5) fell within the range , but the intensities changed in every month. In the figure, the maximum occurred during the snow cover season and the period when vegetation was depleted from January to March. The minimum occurred during the season when vegetation was mature from July to August. The long-wavelength spectral ratios were slightly higher than the short-wavelength spectral ratios. Extrapolation of the RRFuv spectral ratios produced estimates that agreed with the RRFsolar spectral ratios. This extrapolation is confirmed by the high value of RRFsolar (0.205) shown in following Table RFuv/RFsolar As indicated in Fig. 2 (d-3) and (e-3), the RFuv/RFsolar irradiance ratios were remarkably different in each year. The maxima were scattered from January to August, and the minimum 5.2 Spectral irradiances and spectral ratios at wavelengths of 305, 310, 315, 320, and 325 nm The seasonal changes of monthly spectral irradiances at wavelengths of 305, 310, 315, 320, and 325 nm in Figs. 5 (1) to (5)

8 Journal of the Aerological Observatory No Fig. 4 Seasonal change of monthly GLuv, DFuv, and RFuv spectral irradiance, and their spectral ratios from 2004 to 2012 at Tsukuba. Heavy lines show the averages for the observation periods. (1) GLuv, (2) DFuv, and (3) RFuv: Global, diffuse, and reflected spectral UV per 5 nm from 290 to 325 nm in every year. (4) RDFuv and (5) RRFuv: Diffusibility and reflectivity relative to global spectral UV per 5 nm from 300 to 325 nm in every year. Fig. 5 Seasonal changes of GLuv, DFuv, and RFuv monthly irradiance and monthly RDFuv and RRFuv irradiance ratios, at wavelengths of 305, 310, 315, 320, and 325 nm, for the observation period from 2004 to 2012 at Tsukuba. (1) GLuv, (2) DFuv, and (3) RFuv: Global, diffuse, and reflected spectral irradiance. (4) RDFuv and (5) RRFuv: Diffusibility and reflectivity to global spectral irradiance. Dotted lines in Figs. (3) and (5) show the irradiances and irradiance ratios in 2007, the year without snow cover. Fig. 6 Relationships between UV (CIE) radiation and solar radiation, using averages of the monthly means for 9 (8) years from 2004 (2005) to 2012 at Tsukuba. (1): GLsolar versus GLuv, (2): DFsolar versus DFuv, (3): RFsolar versus RFuv, (4): RDFsolar versus RDFuv, and (5) RRFsolar versus RRFuv

9 Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012 Fig. 7 Annual changes of direct, diffuse, and reflected irradiances, and their percentage contributions to global irradiance based on calculated results with averages of monthly means of daily total irradiances, for 9 (8) years from 2004 (2005) to 2012 at Tsukuba. (a-1), (b-1), (c-1), and (d-1): DR, DF, and RF irradiances. (a-2), (b-2), (c-2), and (d-2): DR, DF, and RF irradiance percentages. were calculated from the averaged monthly means of daily totals during the observation period of 9 (DF: 8) years. In Figs. (3) and (5), the seasonal changes in 2007, the year without snow cover, are shown by the dotted lines. The GLuv annual time series at 5 wavelengths shown in Fig. 5 (1) have triangular shapes with maxima in August. In contrast, the DFuvs at the same wavelengths in Fig. 5 (2) have trapezoidal shapes characterized by maxima from June to August. The RFuvs at the long-wavelengths (315, 320 and 325 nm) in Fig. 5 (3) have trapezoidal shapes characterized by maxima from January to April and minima from November to December. However in 2007, the year without snow cover, the RFuv pattern was bimodal with a main peak from May to April and a local maximum in August. The RDFuv in Fig. 5 (4) evidenced higher intensities at wavelengths of 320 and 325 nm. The reason is not clarified, because the characteristics are not agreed within the low value of RDFsolar (0.605) shown in following Table 2. The difference of the RRFuv between snow cover and no snow cover is clear in Fig. 5 (5). The ratios at long wavelengths are higher than the ratios at short wavelengths, especially from January to April. 6. The relationships between UV and solar radiation The relationships between the GLuv, DFuv, and RFuv UV (CIE) radiation and the GLsolar, DFsolar, and RFsolar solar radiation are revealed by examining the monthly means for the observation period in Figs. 6 (1) to (5). In these figures, the symbols for each month are color coded. The black thin line and the magnitude of R 2 indicate the approximate trend and the fraction of the variance accounted for by the regression line, respectively. The relationship between GLsolar and GLuv shown in Fig. 6 (1) is almost elliptical in shape, the associated R 2 being The relationship between DFsolar and DFuv shown in Fig. 6 (2) reveals more scatter at high irradiances, the associated R 2 being The relationship between RFsolar and RFuv shown in Fig. 6 (3) has been highly affected by snow cover, the associated R 2 being There is little recognizable relationship between RDFsolar and RDFuv apparent in Fig. 6 (4), the associated R 2 being The relationship between RRFsolar and RRFuv shown in Fig. 6 (5) has also been much affected by snow cover, the associated R 2 being As mentioned, DFsolar and DFuv are more highly correlated than GLsolar and GLuv. The higher correlation in the former case

10 Journal of the Aerological Observatory No is due to the fact that DFsolar and DFuv have not been affected by the rainy season at Tsukuba. There is almost no correlation between RDF and RRF. 7. UV (CIE): contributions of DRuv, DFuv, and RFuv to GLuv. The irradiance of direct UV radiation, DRuv on a horizontal surface, can be calculated from the difference between GLuv and DFuv. The seasonal changes of monthly means of daily total DRuv, DFuv, and RFuv are shown in Fig. 7. In panels (a-1), (b-1), (c-1), (d-1), and (e-1) are the solar radiation, the UV (UVB) radiation, the UV (CIE) radiation, the irradiance at a wavelength of 310 nm, and the irradiance at a wavelength of 320 nm, respectively. In the right-hand panel of each pair of figures, (a-2), (b-2), (c-2), (d-2), and (e-2), are shown the contributions (percentages) of DRuv, DFuv, and RFuv, respectively. The difference between the seasonal change of solar radiation and UV radiation are clearly apparent. The contribution of DRsolar to GLsolar was about 50%, except during the summer season. In contrast, the contribution of DRuv to GLuv was about 20% during all seasons. In contrast, the contribution of RFuv to GLuv evidences much smaller intensities than the contribution of RFsolar to GLsolar. 8. Conclusions Monitoring observations of spectral UV (RFuv) reflected from the ground surface have been carried out by using a modified Brewer spectrophotometer, BR#059, since December of 2003; similar monitoring of diffuse spectral UV (DFuv) in the sky has been carried out with a Brewer spectrophotometer, BR#058, with an automated shadow unit, since August of 2005, at Tsukuba. In this paper, the results of these measurements are compared with global spectral UV, GLuv, and solar radiation, GLsolar, DFsolar, and RFsolar, during the observation period of 9 (DF: 8) years from 2004 (2005) to These data are summarized in Table 2, and conclusions about seasonal changes in the data are summarized as follows. (1) GLuv, DFuv, and RFuv The annual time series of GLuv was unimodal, with a peak in August. In contrast, the time series of GLsolar was bimodal, with peaks in May and August. The inter-annual changes of GLuv evidenced a local minimum in 2006 and a pattern of small increases since GLsolar evidenced similar patterns. The annual time series of DFuv was unimodal, with a peak in August. In contrast, the annual time series of GLsolar was unimodal, with a peak in June. The inter-annual change of DFuv evidenced a pattern of small increases since 2006, but DFsolar Table 2 The averages of annual means of daily total irradiances and daily irradiance ratios from 2005 to 2012 at Tsukuba. (a): GLsolar, GLuv, DFsolar, DFuv, RFsolar and RFuv. (b): RDFsolar, RDFuv, RRFsolar, and RRFuv. (c): Irradiance ratios of "GLuv/GLsolar", "DFuv/DFsolar" and "RFuv/RFsolar". (a) GL DF RF Solar (KJ/m 2 ) UV (UVB) (J/m 2 ) UV (CIE) (J/m 2 ) (b) RDF: DF/GL RRF: RF/GL Ratio (Percent) Ratio (Percent) Solar (60.5) (20.5) UV (UVB) (84.3) (2.0) UV (CIE) (84.3) (2.0) (c) GLuv/GLsolar DFuv/DFsolar RFuv/RFsolar Ratio (Percent) Ratio (Percent) Ratio (Percent) UV (UVB) (0.1087) (0.1749) (0.0087) UV (CIE) (0.0115) (0.0184) (0.0009) was nearly constant from year to year. The annual time series of RFuv displayed a bimodal pattern, with peaks in April and August. This seasonal pattern was similar to the seasonal pattern of RFsolar, but the pattern was strongly affected by snow cover and vegetation. The RFuv has been increasing by small amounts from year to year since a local minimum in (2) RDFuv and RRFuv The average RDFuv ratio was high, about 0.84 (84%), during the observation period. In contrast, the average RDFsolar was about 0.61 (61%). The RDFuv showed little seasonality and no remarkable maximum or minimum periods. On the contrary, the annual time series of RDFsolar was bimodal, with peaks in June and October. The average of the RRFuv ratio was low, about 0.02 (2%), during the observation period. On the contrary, the average RRFsolar ratio was about 0.21 (21%). The RRFuv ratio was only about 1/10 of the RRFsolar ratio. The seasonal pattern of RRFuv was much affected by snow cover, but snow cover had little effect on the seasonal pattern of RRFsolar. The RRFuv has been increasing by small amounts from year to year since 2007 because of snow cover effects (snow cover days has been increasing). (3) GLuv/GLsolar, DFuv/DFsolar, and RFuv/RFsolar The GLuv (CIE) / GLsolar irradiance ratio indicates an intensity of about (0.0115%). The annual time series of the ratio is characterized by a unimodal pattern with a broad peak. The ratio has been nearly constant from year to year since

11 Seasonal Variations of Global, Reflected, and Diffuse Spectral UV Observations based on Brewer Spectrophotometers at Tsukuba, 2004 to 2012 Table 3 Annual means of monthly means of DF, DR, and RF irradiance percentage against to GL (100%) from 2005 to 2012 at Tsukuba. GL DF DR RF Solar Radiation UV (UVB) UV (CIE) nm nm nm (percent) The DFuv (CIE) / DFsolar irradiance ratio indicates an intensity of about (0.0184%). The annual time series of the ratio is triangular in shape. The ratio has been increasing by small amounts from year to year since The RFuv (CIE) / RFsolar irradiance ratio indicates a low intensity of about (0.0009%). The annual time series of the ratio is trapezoidal in shape. The ratio has been changing by small amounts from year to year since (4) The relations between UV radiation and solar radiation The DFsolar is more highly correlated with DFuv than is GLsolar with GLuv. The reason for the higher correlation in the former case reflects the fact that DFsolar and DFuv are not affected by the rainy season at Tsukuba. (5) The UV (CIE) contributions of three components, DRuv, DFuv, and RFuv to GLuv. The average contributions (percentages) of the daily totals of three components, DRuv (i.e., GLuv DFuv), DFuv, and RFuv to GLuv are shown in Table 3. The contributions of DRuv, DFuv, and RFuv compared to GLuv were calculated to be about 20%, 80%, and 2%, respectively. For comparison, the contributions of DRsolar, DFsolar, and RFsolar compared to GLsolar were about 50%, 50%, and 20%, respectively. We were able to elucidate the differences of seasonal variations between the UV radiation, GLuv, DFuv, and RFuv, and solar radiation, GLsolar, DFsolar, and RFsolar. In particular, RFuv is affected by the reflective effect of snow cover and the absorptive effects of vegetation. Continuous observations with Brewer spectrophotometers are very important for, inter alia, ground truth calibration of satellite observations, clarification of aerosol distribution, and studies of vegetation growth. Acknowledgments We would like to thank Dr. D. I. Wardle, Dr. V. Savastiouk, Mr. T. Grajnar, and Mr. M. Brohart of the Experimental Studies Division of the Meteorological Service of Canada; Mr. I. B.A.H. Dieterrink of Kipp & Zonen Inc. in the Netherlands; and the members of the Brewer Workshop. We also thank the staff members of the Aerological Observatory and Ozone Layer Monitoring Office, JMA. References AOT/JMA(1996) : "Radiation Data in Tsukuba", Aerological Observatory, JMA, 196pp. BSRN (2002) : BSRN 7th Report. WCRP/BSRN, 53pp. Ito, M (2004) : Reflected spectral UVB observation on the ground surface using modified Brewer spectrophotometer. Jour. of Aerological Observatory, 64, Ito, M (2005a) : Diffuse spectral UVB routine observation using Brewer spectrophotometer and simple shadow unit. Jour. of Aerological Observatory, 65, Ito, M (2005b) : Reflected spectral UVB routine observation on the ground surface using modified Brewer spectrophotometer at Tsukuba in Jour. of Aerological Observatory, 65, Ito, M. (2006) : Diffuse spectral UVB observation using Brewer spectrophotometer and new automated shadow unit. Jour. of the Aerological Observatory, 66, Ito, M. (2007) : Reflected and diffuse spectral UV observations using Brewer spectrophotometers at Tsukuba. Jour. of Aerological Observatory, 67, Ito, T., Ueno, T., Kajihara, R., Shitamichi, M., Uekubo, T., Ito, M. and M. Kobayashi (1991) : Development of monitoring technique of ultraviolet irradiance on the ground - an assessment of UV-B increase due to ozone depletion based on spectral observations -. Jour. of Meteorological Research, 43, Kipp & Zonen (1996) : Brewer MKIII Spectrophotometer Final Test Record, BR#174. Kipp & Zonen Inc., 75pp. Kipp & Zonen (2008a) : Brewer MKIII Spectrophotometer Operators Manual. Kipp & Zonen Inc., 132pp. Kipp & Zonen (2008b) : Brewer MKIII Spectrophotometer Service Manual. Kipp & Zonen Inc., 125pp. McElroy, C.T., V. Savastiouk and T. Grajnar (2008) : Standard operating procedures manual for the Brewer Spectrophotometer, Ver. D.01. Environment Canada, 138pp. MOE (2004) : "Shigaisen-Hoken-Shido-Manual". Ministry of the Environment, 38pp. Ohmura, A. (2002):Examination of shadow mechanism for diffuse sky irradiance measurement for the BSRN use. Report for the seventh BSRN science and review workshop, WCRP Informal Report No.18/2002, Annex 3 to Diffuse Geometry WG Report, 4pp. WMO (1996):Guide to meteorological instruments and methods of observation. WMO, No.188, I I

12 Journal of the Aerological Observatory No つくばにおけるブリューワー分光光度計を使用した波長別全天 散乱 地面反射紫外線量の季節変化 2004~2012 年 伊藤真人 * 居島修 * 島村哲也 * 上里至 * 能登美之 * 江崎雄治 * * 押木徳明要旨ブリューワー分光光度計を改造して地面反射波長別紫外線量 (RFuv) の観測を 2003 年 12 月に, またブリューワー分光光度計用自動遮蔽装置を開発し散乱波長別紫外線量 (DFuv) の観測を 2005 年 8 月より開始した. 本稿では, 現在までに蓄積された約 9 年間 (DFuv は約 8 年間 ) のデータにより, 両成分の年変化の特性について全天波長別紫外線量 (GLuv) や全天 散乱 地面反射日射量 (GLsolar,DFsolar,RFsolar) との比較を行った. これらは, 以下のようにまとめられる. (1) GLuv,DFuv,RFuv の年変化は,GLsolar,DFsolar,RFsolar とはそれぞれ異なった特徴を持つ.(2) DFuv の経年変化は,DFsolar がほぼ一定で変化が認められないのに対し,2006 年以降, 若干の増加傾向を示す.(3) RFuv の年変化や経年変化は, 積雪や植物の生育状況に大きく左右される.RFsolar では, これらの影響は少ない.(4) RDFuv は, 年変化を持たず約 0.84 (84%) の年間を通してほぼ一定で推移する. これに対し,RDFsolar は年変化を有し, 年平均約 0.61(61%) を示す.(5) RRFuv は 0.02(2%) を示し,RRFsolar が 0.21 (21%) を示すのに対し低い値をとる. また,RRFuv は微弱な波長依存性を持ち, 長波長側で若干大きくなる.(6) 紫外線量の各成分の割合は,GLuv を 100% とすると DRuv が約 20%,DFuv が約 80%,RFuv が約 2% となり, 日射 Solar の場合の約 50%, 約 50%, 約 20% と大きく異なる. 以上にように,GLuv,DFuv,RFuv の年変化と経年変化の特徴を把握することができた. 今後, これらのデータが, 衛星観測の地上較生, エアロゾル挙動の研究, 植物生育の研究等々の分野において利用されることを期待したい. * 気象庁高層気象台観測第三課

Altitudinal Increasing Rate of UV radiation by the Observations with Brewer Spectrophotometers at Norikura, Suzuran and Tsukuba

Altitudinal Increasing Rate of UV radiation by the Observations with Brewer Spectrophotometers at Norikura, Suzuran and Tsukuba [Technical report] Altitudinal Increasing Rate of UV radiation by the Observations with Brewer Spectrophotometers at Norikura, Suzuran and Tsukuba Mahito ITO *, Itaru UESATO *, Yoshiyuki NOTO **, Osamu

More information

Absolute Calibration for Brewer Spectrophotometers and Total Ozone/UV Radiation at Norikura on the Northern Japanese Alps

Absolute Calibration for Brewer Spectrophotometers and Total Ozone/UV Radiation at Norikura on the Northern Japanese Alps [Technical report] Absolute Calibration for Brewer Spectrophotometers and Total Ozone/UV Radiation at Norikura on the Northern Japanese Alps Mahito ITO *, Itaru UESATO *, Yoshiyuki NOTO *, Osamu IJIMA

More information

Global Spectral UV in Recent 6 Years and Test Observation of Diffuse Spectral UV with Brewer Spectrophotometer at Rikubetsu, Central Hokkaido

Global Spectral UV in Recent 6 Years and Test Observation of Diffuse Spectral UV with Brewer Spectrophotometer at Rikubetsu, Central Hokkaido [Technical report] Global Spectral UV in Recent 6 s and Test Observation of Diffuse Spectral UV with Brewer Spectrophotometer at Rikubetsu, Central Hokkaido Mahito ITO *, Masaji ONO **, Noritsugu TSUDA

More information

28 th Conference on Severe Local Storms 11 Nov Eigo Tochimoto and Hiroshi Niino (AORI, The Univ. of Tokyo)

28 th Conference on Severe Local Storms 11 Nov Eigo Tochimoto and Hiroshi Niino (AORI, The Univ. of Tokyo) L 28 th Conference on Severe Local Storms 11 Nov. 2016 Eigo Tochimoto and Hiroshi Niino (AORI, The Univ. of Tokyo) Introduction In the warm sector of extratropical cyclones (ECs), there are strong upper-level

More information

Reactive Fluid Dynamics 1 G-COE 科目 複雑システムのデザイン体系 第 1 回 植田利久 慶應義塾大学大学院理工学研究科開放環境科学専攻 2009 年 4 月 14 日. Keio University

Reactive Fluid Dynamics 1 G-COE 科目 複雑システムのデザイン体系 第 1 回 植田利久 慶應義塾大学大学院理工学研究科開放環境科学専攻 2009 年 4 月 14 日. Keio University Reactive Fluid Dynamics 1 G-COE 科目 複雑システムのデザイン体系 第 1 回 植田利久 慶應義塾大学大学院理工学研究科開放環境科学専攻 2009 年 4 月 14 日 Reactive Fluid Dynamics 2 1 目的 本 G-COE で対象とする大規模複雑力学系システムを取り扱うにあたって, 非線形力学の基本的な知識と応用展開力は不可欠である. そこで,

More information

Taking an advantage of innovations in science and technology to develop MHEWS

Taking an advantage of innovations in science and technology to develop MHEWS Taking an advantage of innovations in science and technology to develop MHEWS Masashi Nagata Meteorological Research Institute, Tsukuba, Ibaraki, Japan Japan Meteorological Agency 1 Why heavy rainfalls

More information

CMB の温度 偏光揺らぎにおける弱い重力レンズ効果 並河俊弥 ( 東京大学 )

CMB の温度 偏光揺らぎにおける弱い重力レンズ効果 並河俊弥 ( 東京大学 ) CMB の温度 偏光揺らぎにおける弱い重力レンズ効果 再構築法の開発 並河俊弥 ( 東京大学 ) 201 1 第 41 回天文 天体物理若手夏の学校 2011/08/01-04 CMB lensing の宇宙論への応用 暗黒エネルギー ニュートリノ質量など 比較的高赤方偏移の揺らぎに感度をもつ 光源の性質がよく分かっている 他の観測と相補的 原始重力波 TN+ 10 重力レンズ由来の B-mode

More information

Agilent 4263B LCR Meter Operation Manual. Manual Change. Change 1 Add TAR in Test Signal Frequency Accuracy Test (Page 9-38) as follows.

Agilent 4263B LCR Meter Operation Manual. Manual Change. Change 1 Add TAR in Test Signal Frequency Accuracy Test (Page 9-38) as follows. Agilent 4263B LCR Meter Operation Manual Manual Change Agilent Part No. N/A Jun 2009 Change 1 Add TAR in Test Signal Frequency Accuracy Test (Page 9-38) as follows. Test Signal Frequency Accuracy Frequency

More information

京都 ATLAS meeting 田代. Friday, June 28, 13

京都 ATLAS meeting 田代. Friday, June 28, 13 京都 ATLAS meeting 0.06.8 田代 Exotic search GUT heavy gauge boson (W, Z ) Extra dimensions KK particles Black hole Black hole search (A 模型による )Extra dimension が存在する場合 parton 衝突で black hole が生成される Hawking

More information

C-H Activation in Total Synthesis Masayuki Tashiro (M1)

C-H Activation in Total Synthesis Masayuki Tashiro (M1) 1 C-H Activation in Total Synthesis Masayuki Tashiro (M1) 21 st Jun. 2014 Does a late-stage activation of unactivated C-H bond shorten a total synthesis?? 2 3 Contents 1. Comparison of Two Classical Strategies

More information

一体型地上気象観測機器 ( ) の風計測性能評価 EVALUATION OF WIND MEASUREMENT PERFORMANCE OF COMPACT WEATHER SENSORS

一体型地上気象観測機器 ( ) の風計測性能評価 EVALUATION OF WIND MEASUREMENT PERFORMANCE OF COMPACT WEATHER SENSORS 第 23 回風工学シンポジウム (2014) 一体型地上気象観測機器 ( ) の風計測性能評価 EVALUATION OF WIND MEASUREMENT PERFORMANCE OF COMPACT WEATHER SENSORS 1) 2) 3) 4) 5) 吉田大紀 林 泰一 伊藤芳樹 林 夕路 小松亮介 1) 4) 4) 1) 1) 寺地雄輔 太田行俊 田村直美 橋波伸治 渡邉好弘 Daiki

More information

Development of a High-Resolution Climate Model for Model-Observation Integrating Studies from the Earth s Surface to the Lower Thermosphere

Development of a High-Resolution Climate Model for Model-Observation Integrating Studies from the Earth s Surface to the Lower Thermosphere Chapter 1 Earth Science Development of a High-Resolution Climate Model for Model-Observation Integrating Studies from the Earth s Surface to the Lower Thermosphere Project Representative Shingo Watanabe

More information

一般化川渡り問題について. 伊藤大雄 ( 京都大学 ) Joint work with Stefan Langerman (Univ. Libre de Bruxelles) 吉田悠一 ( 京都大学 ) 組合せゲーム パズルミニ研究集会

一般化川渡り問題について. 伊藤大雄 ( 京都大学 ) Joint work with Stefan Langerman (Univ. Libre de Bruxelles) 吉田悠一 ( 京都大学 ) 組合せゲーム パズルミニ研究集会 一般化川渡り問題について 伊藤大雄 ( 京都大学 ) Joint work with Stefan Langerman (Univ. Libre de Bruxelles) 吉田悠一 ( 京都大学 ) 12.3.8 組合せゲーム パズルミニ研究集会 1 3 人の嫉妬深い男とその妹の問題 [Alcuin of York, 青年達を鍛えるための諸問題 より ] 3 人の男がそれぞれ一人ずつ未婚の妹を連れて川にさしかかった

More information

D j a n g o と P H P の仲間たち ( 改変済 ) サイボウズ ラボ株式会社 TSURUOKA Naoya

D j a n g o と P H P の仲間たち ( 改変済 ) サイボウズ ラボ株式会社 TSURUOKA Naoya D j a n g o と P H P の仲間たち ( 改変済 ) サイボウズ ラボ株式会社 TSURUOKA Naoya D j a n g o と P H P の仲間たち What's Django? W h a t ' s D j a n g o Pythonのフレームワーク インストール簡単 コマンドを実行するだけで自動生成しまくり

More information

Introduction to Multi-hazard Risk-based Early Warning System in Japan

Introduction to Multi-hazard Risk-based Early Warning System in Japan Introduction to Multi-hazard Risk-based Early Warning System in Japan Yasuo SEKITA (Mr) Director-General, Forecast Department Japan Meteorological Agency (JMA) Natural Disasters in Asia Source: Disasters

More information

シミュレーション物理 6 運動方程式の方法 : 惑星の軌道 出席のメール ( 件名に学生番号と氏名 ) に, 中点法をサブルーチンを使って書いたプログラムを添付

シミュレーション物理 6 運動方程式の方法 : 惑星の軌道 出席のメール ( 件名に学生番号と氏名 ) に, 中点法をサブルーチンを使って書いたプログラムを添付 シミュレーション物理 6 運動方程式の方法 : 惑星の軌道 出席のメール ( 件名に学生番号と氏名 ) に, 中点法をサブルーチンを使って書いたプログラムを添付 今回の授業の目的 4 次のRunge-Kutta 法を用いて, 惑星の軌道のシミュレーションを行う 2 d r GMm m = r 2 3 dt r 2 d r GM = 2 (using angular momentum cons.) 2

More information

October 7, Shinichiro Mori, Associate Professor

October 7, Shinichiro Mori, Associate Professor The areas of landslides and affected buildings and houses within those areas, in and around Palu City during Sulawesi Earthquake on September 28, 2018 specified by an analysis based on satellite imagery

More information

谷本俊郎博士の研究業績概要 谷本俊郎博士は これまで地球内部の大規模なマントルの対流運動を解明するための研究 および 大気 - 海洋 - 固体地球の相互作用に関する研究を様々な角度から進めてきた これらのうち主要な研究成果は 以下の様にまとめることができる

谷本俊郎博士の研究業績概要 谷本俊郎博士は これまで地球内部の大規模なマントルの対流運動を解明するための研究 および 大気 - 海洋 - 固体地球の相互作用に関する研究を様々な角度から進めてきた これらのうち主要な研究成果は 以下の様にまとめることができる 谷本俊郎博士の研究業績概要 谷本俊郎博士は これまで地球内部の大規模なマントルの対流運動を解明するための研究 および 大気 - 海洋 - 固体地球の相互作用に関する研究を様々な角度から進めてきた これらのうち主要な研究成果は 以下の様にまとめることができる 1. 地球内部の全球的 3 次元構造とマントル対流プレートテクトニクスによる地球表面の運動が GPS 等の測地観測によってリアルタイムでわかるようになってきた現在

More information

Evaluation of IGS Reprocessed Precise Ephemeris Applying the Analysis of the Japanese Domestic GPS Network Data

Evaluation of IGS Reprocessed Precise Ephemeris Applying the Analysis of the Japanese Domestic GPS Network Data Evaluation of IGS Reprocessed Precise Ephemeris Applying the Analysis of the Japanese Domestic GPS Network Data Seiichi SHIMADA * Abstract The IGS reprocessed GPS precise ephemeris (repro1) is evaluated

More information

Day 5. A Gem of Combinatorics 組合わせ論の宝石. Proof of Dilworth s theorem Some Young diagram combinatorics ヤング図形の組合せ論

Day 5. A Gem of Combinatorics 組合わせ論の宝石. Proof of Dilworth s theorem Some Young diagram combinatorics ヤング図形の組合せ論 Day 5 A Gem of Combinatorics 組合わせ論の宝石 Proof of Dilworth s theorem Some Young diagram combinatorics ヤング図形の組合せ論 Recall the last lecture and try the homework solution 復習と宿題確認 Partially Ordered Set (poset)

More information

Crustal Deformation Associated with the 2005 West Off Fukuoka Prefecture Earthquake Derived from ENVISAT/InSAR and Fault- slip Modeling

Crustal Deformation Associated with the 2005 West Off Fukuoka Prefecture Earthquake Derived from ENVISAT/InSAR and Fault- slip Modeling Crustal Deformation Associated with the 2005 West Off Fukuoka Prefecture Earthquake Derived from ENVISAT/InSAR and Fault- slip Modeling Taku OZAWA, Sou NISHIMURA, and Hiroshi OHKURA Volcano Research Department,

More information

むらの定量化について IEC-TC110 HHG2 への提案をベースに ソニー株式会社冨岡聡 フラットパネルディスプレイの人間工学シンポジウム

むらの定量化について IEC-TC110 HHG2 への提案をベースに ソニー株式会社冨岡聡 フラットパネルディスプレイの人間工学シンポジウム むらの定量化について IEC-TC110 HHG2 への提案をベースに ソニー株式会社冨岡聡 むら を 定量化する とは? どちらも輝度分布の最大最小の差は 22% 画面の 4 隅に向かって暗くなる状態は 気にならない 気になるもの むら むら とは人の主観である 気になる要素 を見出し 計測可能にする SEMU: 既存の定量評価方法 SEMI: 半導体 FPD ナノテクノロジー MEMS 太陽光発電

More information

Influence of MJO on Asian Climate and its Performance of JMA Monthly Forecast Model

Influence of MJO on Asian Climate and its Performance of JMA Monthly Forecast Model Influence of MJO on Asian Climate and its Performance of JMA Monthly Forecast Model Satoko Matsueda, Yuhei Takaya and Kengo Miyaoka Climate Prediction Division, Japan Meteorological Agency Madden-Julian

More information

The unification of gravity and electromagnetism.

The unification of gravity and electromagnetism. The unification of gravity and electromagnetism. (The physics of dark energy.) Terubumi Honjou The 9 chapter. The unification of gravity and electromagnetism. [1]... to the goal of modern physics and the

More information

超新星残骸からの陽子起源ガンマ線 放射スペクトルの変調機構

超新星残骸からの陽子起源ガンマ線 放射スペクトルの変調機構 超新星残骸からの陽子起源ガンマ線 放射スペクトルの変調機構 名古屋大学理学研究科 井上剛志 今日の話とは別の成果 : Inoue, Hennebelle, Fukui, Matsumoto, Iwasaki, Inutsuka 2018, PASJ Special issue, arxiv: 1707.02035 IntroducGon to RX J1713.7-3946 p SNR: RX J1713.7-3946:

More information

車載用高効率燃焼圧センサー基板に最適なランガサイト型結晶の開発 結晶材料化学研究部門 シチズンホールディングス ( 株 )* 宇田聡 八百川律子 * Zhao Hengyu 前田健作 野澤純 藤原航三

車載用高効率燃焼圧センサー基板に最適なランガサイト型結晶の開発 結晶材料化学研究部門 シチズンホールディングス ( 株 )* 宇田聡 八百川律子 * Zhao Hengyu 前田健作 野澤純 藤原航三 車載用高効率燃焼圧センサー基板に最適なランガサイト型結晶の開発 結晶材料化学研究部門 シチズンホールディングス ( 株 )* 宇田聡 八百川律子 * Zhao Hengyu 前田健作 野澤純 藤原航三 概要車載用燃焼圧センサー用として高抵抗を示すランガサイト型圧電結晶をデザインした すなわち4 元系のランガサイト型結晶 CNGS の適正組成をイオン半径 結晶構成要素の結晶サイト存在に関する自由度 および

More information

69 地盤の水分変化モニタリング技術 比抵抗モニタリングシステムの概要 * 小林剛 Monitoring Technology for a Moisture Change of Subsurface Outline of the Resistivity Monitoring System Tsuyo

69 地盤の水分変化モニタリング技術 比抵抗モニタリングシステムの概要 * 小林剛 Monitoring Technology for a Moisture Change of Subsurface Outline of the Resistivity Monitoring System Tsuyo 69 比抵抗モニタリングシステムの概要 * 小林剛 Monitoring Technology for a Moisture Change of Subsurface Outline of the Resistivity Monitoring System Tsuyoshi KOBAYASHI * Abstract Resistivity monitoring system is a visualization

More information

Youhei Uchida 1, Kasumi Yasukawa 1, Norio Tenma 1, Yusaku Taguchi 1, Jittrakorn Suwanlert 2 and Somkid Buapeng 2

Youhei Uchida 1, Kasumi Yasukawa 1, Norio Tenma 1, Yusaku Taguchi 1, Jittrakorn Suwanlert 2 and Somkid Buapeng 2 Bulletin of the Geological Subsurface Survey of Japan, Thermal vol.60 Regime (9/10), in the p.469-489, Chao-Phraya 2009 Plain, Thailand (Uchida et al.) Subsurface Thermal Regime in the Chao-Phraya Plain,

More information

GRASS 入門 Introduction to GRASS GIS

GRASS 入門 Introduction to GRASS GIS 40 th GIS seminar GRASS 入門 Introduction to GRASS GIS 筑波大学生命環境科学研究科地球環境科学専攻空間情報科学分野 花島裕樹 email:hanashima@geoenv.tsukuba.ac.jp http://grass.osgeo.org/ 18 th December, 2008 Geographic Resource Analysis Support

More information

Photoacclimation Strategy in Photosystem II of Prymnesiophyceae Isochrysis galbana

Photoacclimation Strategy in Photosystem II of Prymnesiophyceae Isochrysis galbana Photoacclimation Strategy in Photosystem II of Prymnesiophyceae Isochrysis galbana プリムネシウム藻綱 Isochrysis galbana の光化学系 II における光適応戦略 6D551 小幡光子 指導教員山本修一 SYNOPSIS 海洋に生息する藻類は 海水の鉛直混合や昼夜により 弱光から強光までの様々な光強度

More information

英語問題 (60 分 ) 受験についての注意 3. 時計に組み込まれたアラーム機能 計算機能 辞書機能などを使用してはならない 4. 試験開始前に 監督から指示があったら 解答用紙の受験番号欄の番号が自身の受験番号かどうかを確認し 氏名を記入すること

英語問題 (60 分 ) 受験についての注意 3. 時計に組み込まれたアラーム機能 計算機能 辞書機能などを使用してはならない 4. 試験開始前に 監督から指示があったら 解答用紙の受験番号欄の番号が自身の受験番号かどうかを確認し 氏名を記入すること (2018 年度一般入試 A) 英語問題 (60 分 ) ( この問題冊子は 8 ページである ) 受験についての注意 1. 監督の指示があるまで 問題を開いてはならない 2. 携帯電話 PHS の電源は切ること 3. 時計に組み込まれたアラーム機能 計算機能 辞書機能などを使用してはならない 4. 試験開始前に 監督から指示があったら 解答用紙の受験番号欄の番号が自身の受験番号かどうかを確認し 氏名を記入すること

More information

高分解能原子核乾板を用いた暗黒物質探索 中竜大 名古屋大学基本粒子研究室 (F 研 ) ICEPP 白馬

高分解能原子核乾板を用いた暗黒物質探索 中竜大 名古屋大学基本粒子研究室 (F 研 ) ICEPP 白馬 高分解能原子核乾板を用いた暗黒物質探索 中竜大 名古屋大学基本粒子研究室 (F 研 ) ICEPP シンポジウム @ 白馬 2010.2.14-17 χ Direct Detection χ q q Indirect Detection χ γ, ν, lepton Accelerator Detection q χ χ γ, ν, lepton q χ Target : Xe, Ge, Si, NaI,

More information

Yutaka Shikano. Visualizing a Quantum State

Yutaka Shikano. Visualizing a Quantum State Yutaka Shikano Visualizing a Quantum State Self Introduction http://qm.ims.ac.jp 東京工業大学 ( 大岡山キャンパス ) 学部 4 年間 修士課程 博士課程と通ったところです 宇宙物理学理論研究室というところにいました マサチューセッツ工科大学 博士課程の際に 機械工学科に留学していました (1 年半 ) チャップマン大学

More information

Report on the experiment of vibration measurement of Wire Brushes. mounted on hand held power tools ワイヤ ブラシ取付け時の手持動力工具振動測定調査の実施について

Report on the experiment of vibration measurement of Wire Brushes. mounted on hand held power tools ワイヤ ブラシ取付け時の手持動力工具振動測定調査の実施について Report on the experiment of vibration measurement of Wire Brushes mounted on hand held power tools ワイヤ ブラシ取付け時の手持動力工具振動測定調査の実施について In this report, the purpose of the experiment is to clarify the vibration

More information

Fusion neutron production with deuterium neutral beam injection and enhancement of energetic-particle physics study in the Large Helical Device

Fusion neutron production with deuterium neutral beam injection and enhancement of energetic-particle physics study in the Large Helical Device 15 th IAEA Technical Meeting on Energetic Particles in Magnetic Confinement Systems, 5-8 September, PPPL Session 8 : Diagnostic Development : O-14 Fusion neutron production with deuterium neutral beam

More information

Deep moist atmospheric convection in a subkilometer

Deep moist atmospheric convection in a subkilometer Deep moist atmospheric convection in a subkilometer global simulation Yoshiaki Miyamoto, Yoshiyuki Kajikawa, Ryuji Yoshida, Tsuyoshi Yamaura, Hisashi Yashiro, Hirofumi Tomita (RIKEN AICS) I. Background

More information

第 6 回 スペースデブリワークショップ 講演資料集 291 E3 デオービット用膜面展開機構の開発 Development of Membran Deployment mechanism for Deorbiting 高井元 ( 宇宙航空研究開発機構 ), 古谷寛, 坂本啓 ( 東京工業大学 ),

第 6 回 スペースデブリワークショップ 講演資料集 291 E3 デオービット用膜面展開機構の開発 Development of Membran Deployment mechanism for Deorbiting 高井元 ( 宇宙航空研究開発機構 ), 古谷寛, 坂本啓 ( 東京工業大学 ), 第 6 回 スペースデブリワークショップ 講演資料集 291 E3 デオービット用膜面展開機構の開発 Development of Membran Deployment mechanism for Deorbiting 高井元 ( 宇宙航空研究開発機構 ), 古谷寛, 坂本啓 ( 東京工業大学 ), 奥泉信克, 宮崎英治, 井上浩一 ( 宇宙航空研究開発機構 ) Moto Takai(JAXA),

More information

Ground based monitoring of aerosol optical properties and surface radiation budget

Ground based monitoring of aerosol optical properties and surface radiation budget Ground based monitoring of aerosol optical properties and surface radiation budget International Workshop on Land Use/Cover Changes and Air Pollution in Asia Bogor, Indonesia, 6 August 2015 Akihiro UCHIYAMA

More information

日本政府 ( 文部科学省 ) 奨学金留学生申請書

日本政府 ( 文部科学省 ) 奨学金留学生申請書 A PP L IC AT IO N J AP A N ESE G O VE R NMENT ( M ONB UK AG AK US HO :M EXT)SC H OL A RS H IP F O R 2 0 1 6 日本政府 ( 文部科学省 ) 奨学金留学生申請書 Undergraduate Students ( 学部留学生 ) INSTRUCTIONS( 記入上の注意 ) 1.Type application,

More information

Effects of pairing correlation on the low-lying quasiparticle resonance in neutron drip-line nuclei

Effects of pairing correlation on the low-lying quasiparticle resonance in neutron drip-line nuclei 2016/09/13 INPC2016 @ Adelaide 1 Effects of pairing correlation on the low-lying quasiparticle resonance in neutron drip-line nuclei Back ground Prog. Theor. Exp. Phys. 2016, 013D01 Yoshihiko Kobayashi

More information

Numerical Simulation of Seismic Wave Propagation and Strong Motions in 3D Heterogeneous Structure

Numerical Simulation of Seismic Wave Propagation and Strong Motions in 3D Heterogeneous Structure Numerical Simulation of Seismic Wave Propagation and Strong Motions in 3D Heterogeneous Structure Project Representative Takashi Furumura Author Takashi Furumura Center for Integrated Disaster Information

More information

Hetty Triastuty, Masato IGUCHI, Takeshi TAMEGURI, Tomoya Yamazaki. Sakurajima Volcano Research Center, DPRI, Kyoto University

Hetty Triastuty, Masato IGUCHI, Takeshi TAMEGURI, Tomoya Yamazaki. Sakurajima Volcano Research Center, DPRI, Kyoto University Hypocenters, Spectral Analysis and Source Mechanism of Volcanic Earthquakes at Kuchinoerabujima: High-frequency, Low-frequency and Monochromatic Events Hetty Triastuty, Masato IGUCHI, Takeshi TAMEGURI,

More information

Kyoko Kagohara 1, Tomio Inazaki 2, Atsushi Urabe 3 and Yoshinori Miyachi 4 楮原京子

Kyoko Kagohara 1, Tomio Inazaki 2, Atsushi Urabe 3 and Yoshinori Miyachi 4 楮原京子 地質調査総合センター速報 No.54, 平成 21 年度沿岸域の地質 活断層調査研究報告,p.61-67,2010 長岡平野西縁断層帯における浅層反射法地震探査 - 新潟市松野尾地区の地下構造 Subsurface structure of the Western boundary fault zone of Nagaoka Plain, based on high-resolution seismic

More information

Analysis of shale gas production performance by SGPE

Analysis of shale gas production performance by SGPE 447 77 6 24 11 447 453 Journal of the Japanese Association for Petroleum Technology Vol. 77, No. 6 Nov., 2012 pp. 447 453 Lecture Analysis of shale gas production performance by SGPE Kanji Kato **, Mahmood

More information

A method for estimating the sea-air CO 2 flux in the Pacific Ocean

A method for estimating the sea-air CO 2 flux in the Pacific Ocean 太平洋における大気 - 海洋間二酸化炭素フラックス推定手法 A method for estimating the sea-air CO 2 flux in the Pacific Ocean 杉本裕之 気象庁地球環境 海洋部 / 気象研究所海洋研究部 平石直孝 気象庁地球環境 海洋部 ( 現 : 気象庁観測部 ) 石井雅男, 緑川貴 気象研究所地球化学研究部 Hiroyuki Sugimoto Global

More information

Safer Building and Urban Development ( 安全な建物づくり まちづくりづ ) Contents ( 内容 ) 1)Lessons from building damage by earthquake motions and/or tsunami ( 振動被害または

Safer Building and Urban Development ( 安全な建物づくり まちづくりづ ) Contents ( 内容 ) 1)Lessons from building damage by earthquake motions and/or tsunami ( 振動被害または Safer Building and Urban Development ( 安全な建物づくり まちづくりづ ) Contents ( 内容 ) 1)Lessons from building damage by earthquake motions and/or tsunami ( 振動被害または津波被害からの教訓 ) 2)Way of thinking for reconstruction (

More information

井出哲博士の研究業績概要 井出哲博士はこれまで データ解析や数値シミュレーションの手法を用いることによって 地震の震源で起きている現象を様々な角度から研究してきた その主な研究成果は 以下の 3 つに大別される

井出哲博士の研究業績概要 井出哲博士はこれまで データ解析や数値シミュレーションの手法を用いることによって 地震の震源で起きている現象を様々な角度から研究してきた その主な研究成果は 以下の 3 つに大別される 井出哲博士の研究業績概要 井出哲博士はこれまで データ解析や数値シミュレーションの手法を用いることによって 地震の震源で起きている現象を様々な角度から研究してきた その主な研究成果は 以下の 3 つに大別される 1. 地震の動的破壊プロセスの解明地下の岩盤の破壊を伴う摩擦すべりである地震を理解するには 地下で何が起きたかを正確に知る必要がある 井出博士は そのための手法である 断層すべりインバージョン法

More information

On Attitude Control of Microsatellite Using Shape Variable Elements 形状可変機能を用いた超小型衛星の姿勢制御について

On Attitude Control of Microsatellite Using Shape Variable Elements 形状可変機能を用いた超小型衛星の姿勢制御について The 4th Workshop on JAXA: Astrodynamics and Flight Mechanics, Sagamihara, July 015. On Attitude Control of Microsatellite Using Shape Variable Elements By Kyosuke Tawara 1) and Saburo Matunaga ) 1) Department

More information

Study of Cloud and Precipitation Processes Using a Global Cloud-system Resolving Model

Study of Cloud and Precipitation Processes Using a Global Cloud-system Resolving Model Study of Cloud and Precipitation Processes Using a Global Cloud-system Resolving Model Project Representative Masaki Satoh Atmosphere and Ocean Research Institute, University of Tokyo / Research Institute

More information

WHO 飲料水水質ガイドライン第 4 版 ( 一部暫定仮訳 ) 第 9 章放射線学的観点 9.4 飲料水中で一般的に検出される放射性核種のガイダンスレベル 過去の原子力緊急事態に起因する長期被ばく状況に関連する可能性のある人工の放射性核種のみならず 飲料水供給で最も一般的に検出される自然由来及び人工

WHO 飲料水水質ガイドライン第 4 版 ( 一部暫定仮訳 ) 第 9 章放射線学的観点 9.4 飲料水中で一般的に検出される放射性核種のガイダンスレベル 過去の原子力緊急事態に起因する長期被ばく状況に関連する可能性のある人工の放射性核種のみならず 飲料水供給で最も一般的に検出される自然由来及び人工 WHO 飲料水水質ガイドライン第 4 版 ( 一部暫定仮訳 ) 第 9 章放射線学的観点 9.4 飲料水中で一般的に検出される放射性核種のガイダンスレベル 過去の原子力緊急事態に起因する長期被ばく状況に関連する可能性のある人工の放射性核種のみならず 飲料水供給で最も一般的に検出される自然由来及び人工の放射性核種について定められたガイダンスレベルを表 9.2 に示す それぞれの成人の線量換算係数もまた示されている

More information

重力波天体の多様な観測による 宇宙物理学の新展開 勉強会 熱海 銀河における元素量の観測. 青木和光 Wako Aoki. 国立天文台 National Astronomical Observatory of Japan

重力波天体の多様な観測による 宇宙物理学の新展開 勉強会 熱海 銀河における元素量の観測. 青木和光 Wako Aoki. 国立天文台 National Astronomical Observatory of Japan 重力波天体の多様な観測による 宇宙物理学の新展開 勉強会 2013.1.8. 熱海 銀河における元素量の観測 青木和光 Wako Aoki 国立天文台 National Astronomical Observatory of Japan 銀河における元素量の観測 中性子星合体によってどのような元素合成が起こ るか とくにr-processのサイトか 化学進化への影響は 化学組成と金属量 化学組成 元素量

More information

2018 年 ( 平成 30 年 ) 7 月 13 日 ( 金曜日 ) Fri July 13, 2018

2018 年 ( 平成 30 年 ) 7 月 13 日 ( 金曜日 ) Fri July 13, 2018 2018 年 ( 平成 30 年 ) 13 日 ( 金曜日 ) Fri July 13, 2018 発行所 (Name) : 株式会社東京証券取引所 所在地 (Address) : 103-8220 東京都中央日本橋兜町 2-1 ホームヘ ーシ (URL) : https://www.jpx.co.jp/ 電話 (Phone) : 03-3666-0141 2-1 Nihombashi Kabutocho,

More information

PROTEUS, AND THE NAME OF THE TYPE SPECIES OP THE GENUS HUENIA

PROTEUS, AND THE NAME OF THE TYPE SPECIES OP THE GENUS HUENIA H HUENIA {^ERALDICA,THE CORRECT NAME FOR HUENIA PROTEUS, AND THE NAME OF THE TYPE SPECIES OP THE GENUS HUENIA しノ. by L. B, HOLTHUIS CRUSTACEA SMITH^IB^^ISf RETURN fo W-l 妙. V, i コノハガニの学名について L. B. ホノレトイス.

More information

結合および相互作用エネルギーの定量的 評価法の開発と新規典型元素化合物の構築

結合および相互作用エネルギーの定量的 評価法の開発と新規典型元素化合物の構築 結合および相互作用エネルギーの定量的 評価法の開発と新規典型元素化合物の構築 ( 課題番号 :17350021) 平成 17 年度 ~ 平成 18 年度科学研究費補助金 ( 基盤研究 (B) ) 研究成果報告書 平成 19 年 5 月 研究代表者山本陽介 広島大学大学院理学研究科教授 目次 1. 課題番号 2. 研究課題 3. 研究組織 4. 研究経費 5. 研究発表 原著論文 総説類 国内学会における特別講演

More information

近距離重力実験実験室における逆二乗則の法則の検証. Jiro Murata

近距離重力実験実験室における逆二乗則の法則の検証. Jiro Murata 近距離重力実験実験室における逆二乗則の法則の検証? Jiro Murata Rikkyo University / TRIUMF 第 29 回理論懇シンポジウム 重力が織りなす宇宙の諸階層 2016/12/20-22 東北大学天文学教室 1. 重力実験概観 Newton 実験の紹介 2. 加速器実験の解釈 比較 1 ATLAS よくある質問 Q 重力実験はどのくらいの距離までいってるんですか? A

More information

-the 1st lecture- Yoshitaka Fujita Osaka University. Snake of March 16-20, 2015

-the 1st lecture- Yoshitaka Fujita Osaka University. Snake of March 16-20, 2015 -the 1st lecture- @Milano March 16-20, 2015 Yoshitaka Fujita Osaka University Snake of Sizes 1 1.4 billion light years 1 fm 量子力学 Quantum Mechanics Molecule ミクロの世界 Micro World ニュートン力学 Newton Mechanics マクロの世界

More information

Neutron-Insensitive Gamma-Ray Detector with Aerogel for Rare Neutral-Kaon Decay Experiment

Neutron-Insensitive Gamma-Ray Detector with Aerogel for Rare Neutral-Kaon Decay Experiment Neutron-Insensitive Gamma-Ray Detector with Aerogel for Rare Neutral-Kaon Decay Experiment Kyoto University E-mail: maeda_y@scphys.kyoto-u.ac.jp A novel γ-ray detector insensitive to neutrons is developed

More information

Predictabilities of a Blocking Anticyclone and a Explosive Cyclone

Predictabilities of a Blocking Anticyclone and a Explosive Cyclone Chapter 1 Earth Science Predictabilities of a Blocking Anticyclone and a Explosive Cyclone Project Representative Takeshi Enomoto Authors Takeshi Enomoto Akira Yamazaki Akira Kuwano-Yoshida Mio Matsueda

More information

Product Specification

Product Specification This information may be changed without a previous notice. Specification No. JECXDE-9004E Product Specification Issued Date: 17 / Dec. / 2014 Part Description: Supercapacitor (EDLC) Customer Part No.:

More information

11/13 Diagonalization. Theorem: The set R of all real numbers is not enumerable. 12/13. 0.a k1 a k2 a k3... where a ij {0, 1,...

11/13 Diagonalization. Theorem: The set R of all real numbers is not enumerable. 12/13. 0.a k1 a k2 a k3... where a ij {0, 1,... 対角線論法 可算無限集合 : 自然数全体の集合との間に 対 対応がある集合のこと. 可算集合 : 有限または可算無限である集合のこと. つまり, つずつ要素を取り出してきて, もれなく書き並べられるもの 例. 正の偶数全体の集合 E は可算無限である. 自然数全体の集合 N の要素 と,E の要素 2 を対とする 対 対応がある. 例 2. 整数全体の集合 Z は可算無限である. 対 対応がある.

More information

Development of Advanced Simulation Methods for Solid Earth Simulations

Development of Advanced Simulation Methods for Solid Earth Simulations Chapter 1 Earth Science Development of Advanced Simulation Methods for Solid Earth Simulations Project Representative Mikito Furuichi Department of Mathematical Science and Advanced Technology, Japan Agency

More information

( 主査 ) 教授髙橋秀幸教授山口信次郎准教授佐藤修正

( 主査 ) 教授髙橋秀幸教授山口信次郎准教授佐藤修正 氏名 ( 本籍地 ) 学 位 の 種 類 学 位 記 番 号 学位授与年月日 学位授与の要件 研究科, 専攻 論 文 題 目 ぱんれい 庞磊博士 ( 生命科学 ) 生博第 337 号平成 29 年 3 月 24 日学位規則第 4 条第 1 項該当東北大学大学院生命科学研究科 ( 博士課程 ) 生態システム生命科学専攻 Analyses of Functional Tissues and Hormonal

More information

観光の視点から見た民泊の現状 課題 展望

観光の視点から見た民泊の現状 課題 展望 38 特集 シェアリングエコノミーと交通 / 論説 観光の視点から見た民泊の現状 課題 展望 193 ( ) Current State of Affairs, Challenges, and Outlook for Minpaku from the Perspective of Tourism Noriko YAGASAKI Minpaku, translated as lodging at private

More information

Spontaneous magnetization of quark matter in the inhomogeneous chiral phase

Spontaneous magnetization of quark matter in the inhomogeneous chiral phase Spontaneous agnetization of uar atter in the inhoogeneous chiral phase arxiv:7. [hep-ph] Ryo Yoshiie (Kyoto University) collaborator:kazuya Nishiyaa oshitaa atsui XQCD 9/@CCNU QCD phase diagra and chiral

More information

Estimation of Gravel Size Distribution using Contact Time

Estimation of Gravel Size Distribution using Contact Time ISSN 386-1678 Report of the Research Institute of Industrial Technology, Nihon University Number 97, 212 Estimation of Gravel Size Distribution using Contact Time Akira ODA*, Yuya HIRANO**, Masanori WATANABE***

More information

Y. Okayasu for the Jlab E collaboration Department of Physics. Tohoku University

Y. Okayasu for the Jlab E collaboration Department of Physics. Tohoku University Analysis status of the Λ hyernuclear sectroscoic exeriment @ Jlab Hall C (E01-011) Contents 1: Characteristics of the (e,e K ) reaction 2: Physics goals of Jlab E01-011 3: Thomas Jefferson National Accelerator

More information

Algorithm Theoretical Basis Document for Cloud Top Height Product

Algorithm Theoretical Basis Document for Cloud Top Height Product Algorithm Theoretical Basis Document for Cloud Top Height Product MOURI Kouki*, SUZUE Hiroshi*, YOSHIDA Ryo* and IZUMI Toshiharu** Abstract The cloud top height product is an element of the fundamental

More information

質量起源 暗黒物質 暗黒エネルギー 宇宙線 陽子崩壊 ニュートリノ質量 米国 P5 ニュートリノ CPV 宇宙背景ニュートリノクォーク レプトンマヨラナ粒子 ニュートリノ測定器 陽子崩壊探索. Diagram courtesy of P5. Origin of Mass.

質量起源 暗黒物質 暗黒エネルギー 宇宙線 陽子崩壊 ニュートリノ質量 米国 P5 ニュートリノ CPV 宇宙背景ニュートリノクォーク レプトンマヨラナ粒子 ニュートリノ測定器 陽子崩壊探索. Diagram courtesy of P5. Origin of Mass. Diagram courtesy of P5 The Energy Frontier Origin of Mass Matter/Antimatter Asymmetry Dark Matter Origin of Universe Unification of Forces New Physics Beyond the Standard Model ニュートリノ質量 質量起源 The Intensity

More information

Thermal Safety Software (TSS) series

Thermal Safety Software (TSS) series Ready-solutions Thermal Safety Software (TSS) series 各種の反応危険性評価ソフト The subset for adiabatic calorimetry ( 断熱測定データ解析ソリューション ) 断熱熱量計 (ARC VSP DEWAR) 等は 化学反応の熱的危険性評価に有効であることが知られています このソリューションは 断熱下で測定した熱量データを多目的に解析するために

More information

Advance Publication by J-STAGE. 日本機械学会論文集 Transactions of the JSME (in Japanese)

Advance Publication by J-STAGE. 日本機械学会論文集 Transactions of the JSME (in Japanese) Advance Publication by J-STAGE 日本機械学会論文集 Transactions of the JSME (in Japanese) DOI:10.1299/transjsme.16-00058 Received date : 24 February, 2016 Accepted date : 6 September, 2016 J-STAGE Advance Publication

More information

Multi-Scale Simulations for Adaptation to Global Warming and Mitigation of Urban Heat Islands

Multi-Scale Simulations for Adaptation to Global Warming and Mitigation of Urban Heat Islands Chapter 1 Earth Science Multi-Scale Simulations for Adaptation to Global Warming and Mitigation of Urban Heat Islands Project Representative Ryo Onishi Center for Earth Information Science and Technology,

More information

ATLAS 実験における荷電ヒッグス粒子の探索

ATLAS 実験における荷電ヒッグス粒子の探索 1 ATLAS 実験における荷電ヒッグス粒子の探索 筑波大学大学院数理物質科学研究科物理学専攻博士後期課程 3 年永田和樹 2016 年 1 月 19 日 CiRfSE workshop 重い荷電ヒッグス粒子探索 2 もし 荷電ヒッグス粒子の発見できたら 標準理論を超える物理の存在の証明 例 :Minimal Supersymmetric Standard Model (MSSM) 重い荷電ヒッグス粒子探索

More information

JAXA Status Report. JAXA Status Report. 4-6 April 2017 WMO ET-SAT

JAXA Status Report. JAXA Status Report. 4-6 April 2017 WMO ET-SAT JAXA Status Report JAXA Status Report 4-6 April 2017 WMO ET-SAT JAXA s Past, Current and Future Satellite/Sensor Activities ALOS-2 (CY 2014) GCOM-C (JFY 2017) GOSAT-2 (JFY 2018) Earth CARE/CPR (JFY 2019(TBC))

More information

電離によるエネルギー損失. β δ. Mean ioniza9on energy. 物質のZ/Aに比例 Z/A~1/2, β~1 1.5MeV/(g cm 2 ) 入射粒子の速度 (β) に依存粒子識別が可能低速では1/β 2. 高速ではβ 2 /(1- β 2 ) で上昇 1.

電離によるエネルギー損失. β δ. Mean ioniza9on energy. 物質のZ/Aに比例 Z/A~1/2, β~1 1.5MeV/(g cm 2 ) 入射粒子の速度 (β) に依存粒子識別が可能低速では1/β 2. 高速ではβ 2 /(1- β 2 ) で上昇 1. 放射線検出器の基礎 - 2 飯嶋徹 電離によるエネルギー損失 2 2 de 2 Z 1 2mc 2 2 ln e β δ = Kz β (1 2 dx A β I β ) 2 K = 4π N r m c = 0.3071 MeV cm / gr 2 2 2 0 0 e I Mean ioniza9on energy I 7 = 12 + ev Z Z Z < 13 I 1.19 = 9.76 +

More information

2015 年度研究活動報告理工学術院 先進理工 応用物理学科小澤徹 Department of Applied Physics, Waseda University

2015 年度研究活動報告理工学術院 先進理工 応用物理学科小澤徹 Department of Applied Physics, Waseda University 2015 年度研究活動報告理工学術院 先進理工 応用物理学科小澤徹 Tohru OZAWA Department of Applied Physics, Waseda University 出版された論文 R. Carles, T. Ozawa Finite time extinction for nonlinear Schrödinger equation in 1D and 2D, Commun.

More information

統合シミュレーションコードによる高速点火実験解析大阪大学レーザーエネルギー学研究センター中村龍史

統合シミュレーションコードによる高速点火実験解析大阪大学レーザーエネルギー学研究センター中村龍史 統合シミュレーションコードによる高速点火実験解析大阪大学レーザーエネルギー学研究センター中村龍史 概要 高速点火核融合ではターゲット爆縮から追加熱用レーザーによる高速電子発生まで時間 空間スケールにおいて非常に広範な領域の現象を理解する必要がある そこで本プロジェクトでは輻射流体コード 粒子コード Fokker-Planck コード の開発が進められており これらのコードをネットワークを介して結合することで統合コードの構築を目指している

More information

二国間交流事業共同研究報告書 共同研究代表者所属 部局独立行政法人理化学研究所 創発物性科学研究センター

二国間交流事業共同研究報告書 共同研究代表者所属 部局独立行政法人理化学研究所 創発物性科学研究センター ( 様式 4-1) 二国間交流事業共同研究報告書 平成 26 年 3 月 20 日 独立行政法人日本学術振興会理事長殿 共同研究代表者所属 部局独立行政法人理化学研究所 創発物性科学研究センター 量子情報エレクトロニクス部門 量子凝縮物性研究ク ルーフ ( ふりがな ) ノリフランコ職 氏名ク ルーフ テ ィレクター NORI FRANCO 1. 事業名相手国 ( ロシア ) との共同研究振興会対応機関

More information

Kinetic Analysis of the Oxidation of Ascorbic Acid in an Open Reactor with Gas Bubbling

Kinetic Analysis of the Oxidation of Ascorbic Acid in an Open Reactor with Gas Bubbling Original Paper Japan Journal of Food Engineering, Vol. 17, No. 2, pp. 51-55, June. 2016 Kinetic Analysis of the Oxidation of Ascorbic Acid in an Open Reactor with Gas Bubbling Osato MIYAWAKI, Taira SUGIYAMA,

More information

非弾性散乱を利用した不安定核 核構造研究 佐藤義輝東京工業大学

非弾性散乱を利用した不安定核 核構造研究 佐藤義輝東京工業大学 非弾性散乱を利用した不安定核 核構造研究 佐藤義輝東京工業大学 Unbound excited states in,17 C Ground state deformation property of carbon isotopes Y.Satou et al., Phys. Lett. B 660, 320(2008). Be BC Li H He Ne O F N N=8 C 17 C Neutron

More information

Illustrating SUSY breaking effects on various inflation models

Illustrating SUSY breaking effects on various inflation models 7/29 基研研究会素粒子物理学の進展 2014 Illustrating SUSY breaking effects on various inflation models 山田悠介 ( 早稲田大 ) 共同研究者安倍博之 青木俊太朗 長谷川史憲 ( 早稲田大 ) H. Abe, S. Aoki, F. Hasegawa and Y. Y, arxiv:1408.xxxx 7/29 基研研究会素粒子物理学の進展

More information

XENON SHORT ARC LAMPS キセノンショートアークランプ

XENON SHORT ARC LAMPS キセノンショートアークランプ 光源事業 / キセノンショートアークランプ XENON SHORT ARC LAMPS キセノンショートアークランプ 当社のキセノンショートアークランプは 自然太陽光に近似し た光波長 分光分布を有する特性を生かし 太陽電池の性能評 価 基礎研究のための弊社製ソーラシミュレータ用標準光源と して採用しているだけでなく 高輝度 点光源 高演色という 特性を生かし 分光器用光源 映写機用光源 プラネタリウム

More information

Fast response silicon pixel detector using SOI. 2016/08/10 Manabu Togawa

Fast response silicon pixel detector using SOI. 2016/08/10 Manabu Togawa Fast response silicon pixel detector using SOI 2016/08/10 Manabu Togawa 1 100 ps High intensity fixed target NA62200 ps J-PARC MEG TOF-PET TOF-PET 400 ps α K + -> π + νν : NA62 expriment At CERN SPS Goal

More information

SOLID STATE PHYSICAL CHEMISTRY

SOLID STATE PHYSICAL CHEMISTRY SOLID STATE PHYSICAL CHEMISTRY Annual Research Highlights (1) ε-al x Fe 2 x O 3 : an advanced nanomagnets exhibiting millimeter-wave absorption In this work, aluminum-substituted epsilon-phase iron oxides,

More information

FDM Simulation of Broadband Seismic Wave Propagation in 3-D Heterogeneous Structure using the Earth Simulator

FDM Simulation of Broadband Seismic Wave Propagation in 3-D Heterogeneous Structure using the Earth Simulator Chapter 1 Earth Science FDM Simulation of Broadband Seismic Wave Propagation in 3-D Heterogeneous Structure using the Earth Simulator Project Representative Takashi Furumura Center for Integrated Disaster

More information

EU 向けに輸出される食品等に関する証明書の発行に係る事務処理要領 ( 国際 ) 通知に基づき 欧州連合 ( 以下 EU という ) へ輸出される食品及び飼料の証明書の発行条件及び手続きを定めるものとする

EU 向けに輸出される食品等に関する証明書の発行に係る事務処理要領 ( 国際 ) 通知に基づき 欧州連合 ( 以下 EU という ) へ輸出される食品及び飼料の証明書の発行条件及び手続きを定めるものとする EU 向けに輸出される食品等に関する証明書の発行に係る事務処理要領 平成 23 年 4 月 7 日山口県農林水産部流通企画室 ( 趣旨 ) 第 1 平成 23 年 3 月 27 日付け22 国際第 1144 号農林水産省大臣官房総括審議官 ( 国際 ) 通知に基づき 欧州連合 ( 以下 EU という ) へ輸出される食品及び飼料の証明書の発行条件及び手続きを定めるものとする ( 対象となる食品等 )

More information

Adaptation Oriented Simulations for Climate Variability

Adaptation Oriented Simulations for Climate Variability Chapter 1 Earth Science Adaptation Oriented Simulations for Climate Variability Project Representative Keiko Takahashi Earth Simulator Center, Japan Agency for Marine-Earth Science and Technology Authors

More information

高エネルギーニュートリノ : 理論的な理解 の現状

高エネルギーニュートリノ : 理論的な理解 の現状 第 24 回 宇宙ニュートリノ 研究会 高エネルギーニュートリノ : 理論的な理解 の現状 京都大学基礎物理学研究所 長滝重博 Kaji Yasuyuki 9th March 2011, ICRR, Tokyo Overview History of the Universe UHECRs? VHE-ν? When? Who? How? CMB 3000k -> 2.75k Mysteries of

More information

TDK Lambda INSTRUCTION MANUAL. TDK Lambda A B 1/40

TDK Lambda INSTRUCTION MANUAL. TDK Lambda A B 1/40 A273 57 01B 1/40 INDEX PAGE 1. MTBF 計算値 Calculated Values of MTBF 3~4 2. 部品ディレーティング Component Derating 5~9 3. 主要部品温度上昇値 Main Components Temperature Rise ΔT List 10~11 4. 電解コンデンサ推定寿命計算値 Electrolytic Capacitor

More information

高分解能 GSMaP アルゴリズムの 構造と考え方 牛尾知雄 ( 大阪大 )

高分解能 GSMaP アルゴリズムの 構造と考え方 牛尾知雄 ( 大阪大 ) 高分解能 GSMaP アルゴリズムの 構造と考え方 牛尾知雄 ( 大阪大 ) Curret GSMaP products GSMaP_MWR Microwave radiometer product GSMaP_MVK Global precipitatio mappig from microwave ad ifrared radiometric data GSMaP_Gauge Gauge adjusted

More information

Method for making high-quality thin sections of native sulfur

Method for making high-quality thin sections of native sulfur Bulletin of the Geological Survey of Japan, vol. 69 (2), p. 135 139, 2018 Notes and Comments Method for making high-quality thin sections of native sulfur Takayuki S 1,*, Akira Owada 1 and Eri Hirabayashi

More information

2006 Inter-laboratory Comparison Study for Reference Material for Nutrients in Seawater

2006 Inter-laboratory Comparison Study for Reference Material for Nutrients in Seawater ISSN 0386-4049 TECHNICAL REPORTS OF THE METEOROLOGICAL RESEARCH INSTITUTE No.58 2006 Inter-laboratory Comparison Study for Reference Material for Nutrients in Seawater 気象研究所技術報告 第 58 号 栄養塩測定用海水組成標準の 2006

More information

Simulations of Atmospheric General Circulations of Earth-like Planets by AFES

Simulations of Atmospheric General Circulations of Earth-like Planets by AFES Chapter 1 Earth Science Simulations of Atmospheric General Circulations of Earth-like Planets by AFES Project Representative Yoshi-Yuki Hayashi Department of Earth and Planetary Sciences, Kobe University

More information

低温物質科学研究センター誌 : LTMセンター誌 (2013), 23: 22-26

低温物質科学研究センター誌 : LTMセンター誌 (2013), 23: 22-26 Title サロンセミナー報告 Author(s) Citation 低温物質科学研究センター誌 : LTMセンター誌 (2013), 23: 22-26 Issue Date 2013-12-01 URL https://doi.org/10.14989/189250 Right Type Departmental Bulletin Paper Textversion publisher Kyoto

More information

すばる望遠鏡将来装置計画 WS TMT の観測装置開発. Project Overview TMT FL instruments Japanese instruments. 柏川伸成 (NAOJ/TMT project) Jan. 2011

すばる望遠鏡将来装置計画 WS TMT の観測装置開発. Project Overview TMT FL instruments Japanese instruments. 柏川伸成 (NAOJ/TMT project) Jan. 2011 2011.01 すばる望遠鏡将来装置計画 WS TMT の観測装置開発 Project Overview TMT FL instruments Japanese instruments 柏川伸成 (NAOJ/TMT project) Jan. 2011 Overview TMT Fast Facts 30m aperture Filled segmented primary Active and adaptive

More information

Predictability Variation in Numerical Weather Prediction: a Multi-Model Multi-Analysis Approach

Predictability Variation in Numerical Weather Prediction: a Multi-Model Multi-Analysis Approach Chapter 1 Earth Science Predictability Variation in Numerical Weather Prediction: a Multi-Model Multi-Analysis Approach Project Representative Takeshi Enomoto Authors Takeshi Enomoto Shozo Yamane Akira

More information

スペース赤外線天文学の 現状と将来 ~ 波長の壁を越えて ~ 中川貴雄 (ISAS/JAXA)

スペース赤外線天文学の 現状と将来 ~ 波長の壁を越えて ~ 中川貴雄 (ISAS/JAXA) スペース赤外線天文学の 現状と将来 ~ 波長の壁を越えて ~ 中川貴雄 (ISAS/JAXA) 日本の スペース赤外線天文学の歩み? IRTS (1995) あかり (2006) Where are we from? Are we alone? Formation & evolution of galaxies Birth & evolution of stars and planetary systems

More information

din Linguistics 一 一 St1'uctur~s a proposals representagrammati squite incomplete. Although generate al

din Linguistics 一 一 St1'uctur~s a proposals representagrammati squite incomplete. Although generate al G D M G Nw B C 英語教授法通信 第 号 ι 年 月 日勺 WHA RANSFORM AONALYNAX 一一 A R! L 一 一 ず 併 j ~ ;! ~も Wm Y m m m x N~w B~ mx j (; ; qw m M w SC mj m S~ Cm mx mm C J q m A H CmS S m m m mm m Cm R P S ; x mm w A と w R

More information

Hypocenter Distribution of Deep Low-frequency Tremors in Nankai Subduction Zone, Japan

Hypocenter Distribution of Deep Low-frequency Tremors in Nankai Subduction Zone, Japan Hypocenter Distribution of Deep Low-frequency Tremors in Nankai Subduction Zone, Japan Takuto MAEDA * and Kazushige OBARA ** * Earthquake Research Department, National Research Institute for Earth Science

More information

SML-811x/812x/813x Series

SML-811x/812x/813x Series SML-811x/812x/813x Series Data Sheet 特 背面実装可能タイプ 外観図 サイズ情報 3412 (15) 3.4 1.25mm (t=1.1mm) Color Type V U D W M B WB 外形寸法図 3.4 はんだ付け推奨パターン 1.2 R 1.25 1.25 φ2.4 4-R.3 レジスト +.5 1.1 -.1 Hole + 1.25.28 カソードインデックス

More information