# 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: CO2 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: 2021-07-30 09:43:50 # 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 3 395.50 DSI 2010 4 397.59 DSI 2010 5 397.46 DSI 2010 6 392.16 DSI 2010 7 387.94 DSI 2010 8 385.89 DSI 2010 9 385.82 DSI 2010 10 392.17 DSI 2010 11 396.49 DSI 2010 12 396.26 DSI 2011 1 399.74 DSI 2011 2 401.32 DSI 2011 3 400.66 DSI 2011 4 400.64 DSI 2011 5 396.11 DSI 2011 6 391.15 DSI 2011 7 389.24 DSI 2011 8 387.43 DSI 2011 9 387.46 DSI 2011 10 392.89 DSI 2011 11 396.78 DSI 2011 12 397.91 DSI 2012 1 398.75 DSI 2012 2 397.71 DSI 2012 3 396.83 DSI 2012 4 397.74 DSI 2012 5 397.70 DSI 2012 6 394.25 DSI 2012 7 392.26 DSI 2012 8 392.68 DSI 2012 9 391.93 DSI 2012 10 394.01 DSI 2012 11 400.53 DSI 2012 12 402.15 DSI 2013 1 399.04 DSI 2013 2 397.20 DSI 2013 3 399.40 DSI 2013 4 401.69 DSI 2013 5 398.40 DSI 2013 6 396.09 DSI 2013 7 395.76 DSI 2013 8 392.19 DSI 2013 9 391.73 DSI 2013 10 396.21 DSI 2013 11 401.53 DSI 2013 12 405.11 DSI 2014 1 405.35 DSI 2014 2 406.43 DSI 2014 3 406.25 DSI 2014 4 405.99 DSI 2014 5 403.09 DSI 2014 6 398.37 DSI 2014 7 397.55 DSI 2014 8 396.86 DSI 2014 9 397.58 DSI 2014 10 399.30 DSI 2014 11 401.31 DSI 2014 12 406.75 DSI 2015 1 410.65 DSI 2015 2 408.35 DSI 2015 3 406.80 DSI 2015 4 407.71 DSI 2015 5 404.37 DSI 2015 6 401.45 DSI 2015 7 401.50 DSI 2015 8 396.80 DSI 2015 9 395.87 DSI 2015 10 400.33 DSI 2015 11 403.17 DSI 2015 12 408.73 DSI 2016 1 414.10 DSI 2016 2 411.40 DSI 2016 3 408.43 DSI 2016 4 407.74 DSI 2016 5 407.59 DSI 2016 6 404.85 DSI 2016 7 402.24 DSI 2016 11 408.71 DSI 2016 12 411.31 DSI 2017 1 412.47 DSI 2017 2 411.96 DSI 2017 3 412.71 DSI 2017 4 411.09 DSI 2017 5 408.05 DSI 2017 6 405.83 DSI 2017 7 405.23 DSI 2017 8 404.25 DSI 2017 9 403.91 DSI 2017 10 406.42 DSI 2017 11 410.61 DSI 2017 12 413.55 DSI 2018 1 414.60 DSI 2018 2 413.36 DSI 2018 3 412.68 DSI 2018 4 416.04 DSI 2018 5 413.92 DSI 2018 6 407.47 DSI 2018 7 405.95 DSI 2018 8 406.37 DSI 2018 9 407.36 DSI 2018 10 411.95 DSI 2018 11 415.39 DSI 2018 12 417.41 DSI 2019 1 417.70 DSI 2019 2 413.63 DSI 2019 3 413.73 DSI 2019 4 416.24 DSI 2019 5 413.98 DSI 2019 6 410.81 DSI 2019 7 410.23 DSI 2019 8 409.11 DSI 2019 9 408.45 DSI 2019 10 412.38 DSI 2019 11 416.42 DSI 2019 12 416.92 DSI 2020 1 418.35 DSI 2020 2 419.20 DSI 2020 3 420.12 DSI 2020 4 422.08 DSI 2020 5 419.31 DSI 2020 6 414.47 DSI 2020 7 412.70 DSI 2020 8 410.54 DSI 2020 9 411.10 DSI 2020 10 416.06 DSI 2020 11 420.33 DSI 2020 12 423.07