# 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: N2O 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 13:04:10 # 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 3 324.04 DSI 2010 4 323.92 DSI 2010 5 323.94 DSI 2010 6 323.94 DSI 2010 7 323.70 DSI 2010 8 323.64 DSI 2010 9 323.93 DSI 2010 10 324.36 DSI 2010 11 324.61 DSI 2010 12 324.70 DSI 2011 1 324.85 DSI 2011 2 325.04 DSI 2011 3 325.18 DSI 2011 4 325.23 DSI 2011 5 325.12 DSI 2011 6 325.00 DSI 2011 7 324.99 DSI 2011 8 324.99 DSI 2011 9 325.10 DSI 2011 10 325.50 DSI 2011 11 325.80 DSI 2011 12 325.83 DSI 2012 1 325.85 DSI 2012 2 325.89 DSI 2012 3 325.88 DSI 2012 4 325.96 DSI 2012 5 326.05 DSI 2012 6 325.91 DSI 2012 7 325.67 DSI 2012 8 325.69 DSI 2012 9 325.95 DSI 2012 10 326.29 DSI 2012 11 326.63 DSI 2012 12 326.78 DSI 2013 1 326.90 DSI 2013 2 327.16 DSI 2013 3 327.36 DSI 2013 4 327.21 DSI 2013 5 326.88 DSI 2013 6 326.62 DSI 2013 7 326.58 DSI 2013 8 326.78 DSI 2013 9 327.06 DSI 2013 10 327.22 DSI 2013 11 327.37 DSI 2013 12 327.62 DSI 2014 1 327.77 DSI 2014 2 327.85 DSI 2014 3 328.03 DSI 2014 4 328.06 DSI 2014 5 327.70 DSI 2014 6 327.55 DSI 2014 7 327.85 DSI 2014 8 328.12 DSI 2014 9 328.28 DSI 2014 10 328.56 DSI 2014 11 328.83 DSI 2014 12 329.02 DSI 2015 1 329.21 DSI 2015 2 329.32 DSI 2015 3 329.31 DSI 2015 4 329.17 DSI 2015 5 328.92 DSI 2015 6 328.80 DSI 2015 7 328.87 DSI 2015 8 329.00 DSI 2015 9 329.22 DSI 2015 10 329.52 DSI 2015 11 329.82 DSI 2015 12 330.19 DSI 2016 1 330.44 DSI 2016 2 330.27 DSI 2016 3 330.03 DSI 2016 4 330.08 DSI 2016 5 330.14 DSI 2016 6 329.93 DSI 2016 7 329.78 DSI 2016 11 330.91 DSI 2016 12 330.72 DSI 2017 1 330.52 DSI 2017 2 330.59 DSI 2017 3 330.74 DSI 2017 4 330.70 DSI 2017 5 330.59 DSI 2017 6 330.46 DSI 2017 7 330.40 DSI 2017 8 330.50 DSI 2017 9 330.80 DSI 2017 10 331.23 DSI 2017 11 331.53 DSI 2017 12 331.54 DSI 2018 1 331.53 DSI 2018 2 331.80 DSI 2018 3 332.03 DSI 2018 4 331.80 DSI 2018 5 331.45 DSI 2018 6 331.27 DSI 2018 7 331.38 DSI 2018 8 331.77 DSI 2018 9 332.19 DSI 2018 10 332.51 DSI 2018 11 332.95 DSI 2018 12 333.28 DSI 2019 1 333.22 DSI 2019 2 332.94 DSI 2019 3 332.73 DSI 2019 4 332.73 DSI 2019 5 332.74 DSI 2019 6 332.69 DSI 2019 7 332.64 DSI 2019 8 332.77 DSI 2019 9 333.15 DSI 2019 10 333.42 DSI 2019 11 333.46 DSI 2019 12 333.53 DSI 2020 1 333.80 DSI 2020 2 334.05 DSI 2020 3 334.18 DSI 2020 4 334.13 DSI 2020 5 333.85 DSI 2020 6 333.62 DSI 2020 7 333.68 DSI 2020 8 333.98 DSI 2020 9 334.36 DSI 2020 10 334.70 DSI 2020 11 334.95 DSI 2020 12 335.14