# number_of_header_lines: 69 # comment: # comment: ************ USE OF ESRL GMD DATA **************** # comment: # comment: These data are made freely available to the public and the # comment: scientific community in the belief that their wide dissemination # comment: will lead to greater understanding and new scientific insights. # comment: The availability of these data does not constitute publication # comment: of the data. NOAA relies on the ethics and integrity of the user to # comment: ensure that GML receives fair credit for their work. If the data # comment: are obtained for potential use in a publication or presentation, # comment: GML should be informed at the outset of the nature of this work. # comment: If the GML data are essential to the work, or if an important # comment: result or conclusion depends on the GML data, co-authorship # comment: may be appropriate. This should be discussed at an early stage in # comment: the work. Manuscripts using the GML data should be sent to GML # comment: for review before they are submitted for publication so we can # comment: ensure that the quality and limitations of the data are accurately # comment: represented. # comment: Please see accompanying README file, if available, for citation text. # comment: # comment: Every effort is made to produce the most accurate and precise # comment: measurements possible. However, we reserve the right to make # comment: corrections to the data based on recalibration of standard gases # comment: or for other reasons deemed scientifically justified. # comment: # comment: We are not responsible for results and conclusions based on use # comment: of these data without regard to this warning. # comment: # contact_parameter: CH4 CCGG (Individual Flasks) # contact_name: Ed Dlugokencky # contact_telephone: (303) 497-6228 # contact_email: Ed.Dlugokencky@noaa.gov # comment: # comment: ************ COLLABORATORS *************** # comment: # comment: NOAA thanks the following collaborators without # comment: whom these measurements would not be possible. # comment: # collaborator_name: National Central University, Taiwan [NCU] # comment: # comment: ************ RECIPROCITY AGREEMENT *************** # comment: # comment: Use of these data implies an agreement to reciprocate. # comment: Laboratories making similar measurements agree to make their # comment: own data available to the general public and to the scientific # comment: community in an equally complete and easily accessible form. # comment: Modelers are encouraged to make available to the community, # comment: upon request, their own tools used in the interpretation # comment: of the GML data, namely well documented model code, transport # comment: fields, and additional information necessary for other # comment: scientists to repeat the work and to run modified versions. # comment: Model availability includes collaborative support for new # comment: users of the models. # comment: # comment: ************ DATA DESCRIPTION *************** # comment: # description_site-code: dsi # description_project-abbr: ccg_surface # description_strategy-abbr: flask # description_analysis-constraints: flag:..% # description_creation-time: 2021-07-19 11:47:28 # comment: # comment: ************ DATA DOCUMENTATION *************** # comment: # comment: Please refer to the species-specific README file in the # comment: appropriate directory folder at ftp://aftp.cmdl.noaa.gov/data/trace_gases/. # comment: # data_fields: site year month value DSI 2010 3 1884.59 DSI 2010 4 1883.40 DSI 2010 5 1876.55 DSI 2010 6 1821.91 DSI 2010 7 1776.56 DSI 2010 8 1787.41 DSI 2010 9 1811.97 DSI 2010 10 1871.05 DSI 2010 11 1908.07 DSI 2010 12 1897.08 DSI 2011 1 1901.51 DSI 2011 2 1904.38 DSI 2011 3 1902.50 DSI 2011 4 1885.42 DSI 2011 5 1821.02 DSI 2011 6 1797.96 DSI 2011 7 1806.59 DSI 2011 8 1816.23 DSI 2011 9 1862.63 DSI 2011 10 1889.81 DSI 2011 11 1880.21 DSI 2011 12 1891.60 DSI 2012 1 1904.33 DSI 2012 2 1886.93 DSI 2012 3 1868.57 DSI 2012 4 1852.37 DSI 2012 5 1849.97 DSI 2012 6 1838.36 DSI 2012 7 1799.31 DSI 2012 8 1799.50 DSI 2012 9 1849.27 DSI 2012 10 1881.55 DSI 2012 11 1903.82 DSI 2012 12 1911.96 DSI 2013 1 1888.27 DSI 2013 2 1877.71 DSI 2013 3 1910.12 DSI 2013 4 1894.23 DSI 2013 5 1820.81 DSI 2013 6 1805.48 DSI 2013 7 1815.19 DSI 2013 8 1835.96 DSI 2013 9 1875.46 DSI 2013 10 1892.84 DSI 2013 11 1906.21 DSI 2013 12 1927.93 DSI 2014 1 1919.52 DSI 2014 2 1903.49 DSI 2014 3 1910.91 DSI 2014 4 1904.70 DSI 2014 5 1850.07 DSI 2014 6 1822.91 DSI 2014 7 1826.18 DSI 2014 8 1849.42 DSI 2014 9 1916.93 DSI 2014 10 1925.71 DSI 2014 11 1908.02 DSI 2014 12 1935.99 DSI 2015 1 1956.44 DSI 2015 2 1944.08 DSI 2015 3 1921.67 DSI 2015 4 1897.19 DSI 2015 5 1845.08 DSI 2015 6 1831.13 DSI 2015 7 1838.90 DSI 2015 8 1837.91 DSI 2015 9 1886.70 DSI 2015 10 1913.55 DSI 2015 11 1916.24 DSI 2015 12 1953.88 DSI 2016 1 1964.98 DSI 2016 2 1941.82 DSI 2016 3 1922.47 DSI 2016 4 1885.76 DSI 2016 5 1870.35 DSI 2016 6 1850.24 DSI 2016 7 1827.11 DSI 2016 11 1927.82 DSI 2016 12 1941.87 DSI 2017 1 1944.79 DSI 2017 2 1939.37 DSI 2017 3 1935.60 DSI 2017 4 1902.53 DSI 2017 5 1869.30 DSI 2017 6 1841.90 DSI 2017 7 1843.64 DSI 2017 8 1855.20 DSI 2017 9 1883.04 DSI 2017 10 1922.01 DSI 2017 11 1938.66 DSI 2017 12 1949.41 DSI 2018 1 1952.31 DSI 2018 2 1943.33 DSI 2018 3 1952.60 DSI 2018 4 1939.19 DSI 2018 5 1878.81 DSI 2018 6 1844.00 DSI 2018 7 1864.70 DSI 2018 8 1901.42 DSI 2018 9 1934.22 DSI 2018 10 1966.04 DSI 2018 11 1953.36 DSI 2018 12 1954.77 DSI 2019 1 1979.28 DSI 2019 2 1946.89 DSI 2019 3 1925.39 DSI 2019 4 1920.85 DSI 2019 5 1882.67 DSI 2019 6 1863.78 DSI 2019 7 1860.36 DSI 2019 8 1877.59 DSI 2019 9 1944.38 DSI 2019 10 1985.12 DSI 2019 11 1969.07 DSI 2019 12 1946.92 DSI 2020 1 1956.56 DSI 2020 2 1965.75 DSI 2020 3 1965.92 DSI 2020 4 1959.78 DSI 2020 5 1905.23 DSI 2020 6 1856.64 DSI 2020 7 1860.06 DSI 2020 8 1882.27 DSI 2020 9 1919.94 DSI 2020 10 1958.10 DSI 2020 11 1976.76 DSI 2020 12 1991.65