# number_of_header_lines: 70 # comment: # comment: ************ USE OF GML 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: CH4C13 SIL (Individual Flasks) # contact_name: Bruce H Vaughn # contact_telephone: (303) 492-7985 # contact_email: Bruce.Vaughn@colorado.edu # comment: # comment: ************ COLLABORATORS *************** # comment: # comment: NOAA thanks the following collaborators without # comment: whom these measurements would not be possible. # comment: # collaborator_name: National Institute of Water and Atmospheric # collaborator_name: Research [NIWA] # 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, modeled mole fractions, and additional information # comment: necessary for other scientists to repeat the work and to run # comment: modified versions. Model availability includes collaborative # comment: support for new users of the models. # comment: # comment: ************ DATA DESCRIPTION *************** # comment: # description_site-code: bhd # description_project-abbr: ccg_surface # description_strategy-abbr: flask # description_analysis-constraints: flag:..% # description_creation-time: 2022-12-15 17:24:42 # comment: # comment: ************ DATA DOCUMENTATION *************** # comment: # comment: Please refer to the species-specific README file in the # comment: appropriate directory folder at https://gml.noaa.gov/aftp/data/trace_gases/. # comment: # data_fields: site year month value BHD 2009 3 -47.008 BHD 2009 4 -47.047 BHD 2009 5 -47.081 BHD 2009 6 -47.084 BHD 2009 7 -47.083 BHD 2009 8 -47.111 BHD 2009 9 -47.156 BHD 2009 10 -47.168 BHD 2010 3 -46.886 BHD 2010 4 -46.985 BHD 2010 5 -47.102 BHD 2010 6 -47.166 BHD 2010 7 -47.170 BHD 2010 8 -47.149 BHD 2010 9 -47.127 BHD 2010 10 -47.102 BHD 2010 11 -47.059 BHD 2010 12 -47.012 BHD 2011 1 -46.979 BHD 2011 2 -46.993 BHD 2011 3 -47.052 BHD 2011 4 -47.129 BHD 2011 5 -47.194 BHD 2011 6 -47.218 BHD 2011 7 -47.217 BHD 2011 8 -47.217 BHD 2011 9 -47.216 BHD 2011 10 -47.183 BHD 2011 11 -47.107 BHD 2011 12 -47.025 BHD 2012 1 -46.969 BHD 2012 2 -46.981 BHD 2012 3 -47.039 BHD 2012 4 -47.105 BHD 2012 5 -47.144 BHD 2012 6 -47.163 BHD 2012 7 -47.193 BHD 2012 8 -47.249 BHD 2012 9 -47.323 BHD 2012 10 -47.389 BHD 2013 5 -47.200 BHD 2013 6 -47.172 BHD 2013 7 -47.163 BHD 2013 8 -47.183 BHD 2013 9 -47.210 BHD 2013 10 -47.200 BHD 2013 11 -47.142 BHD 2013 12 -47.055 BHD 2014 1 -47.011 BHD 2014 2 -47.047 BHD 2014 3 -47.133 BHD 2014 4 -47.196 BHD 2014 5 -47.206 BHD 2014 6 -47.199 BHD 2014 7 -47.205 BHD 2014 8 -47.217 BHD 2014 9 -47.213 BHD 2014 10 -47.198 BHD 2014 11 -47.182 BHD 2014 12 -47.164 BHD 2015 1 -47.143 BHD 2015 2 -47.135 BHD 2015 3 -47.164 BHD 2015 7 -47.216 BHD 2015 8 -47.173 BHD 2015 9 -47.157 BHD 2015 10 -47.162 BHD 2015 11 -47.167 BHD 2015 12 -47.155 BHD 2016 1 -47.128 BHD 2016 2 -47.104 BHD 2016 3 -47.099 BHD 2016 4 -47.111 BHD 2016 5 -47.134 BHD 2016 6 -47.153 BHD 2016 7 -47.170 BHD 2016 8 -47.189 BHD 2016 9 -47.200 BHD 2017 1 -47.132 BHD 2017 2 -47.144 BHD 2017 3 -47.166 BHD 2017 4 -47.188 BHD 2017 5 -47.204 BHD 2017 6 -47.221 BHD 2017 7 -47.247 BHD 2017 8 -47.272 BHD 2017 9 -47.279 BHD 2017 10 -47.263 BHD 2017 11 -47.231 BHD 2017 12 -47.206 BHD 2018 1 -47.209 BHD 2018 2 -47.235 BHD 2018 3 -47.261 BHD 2018 4 -47.264 BHD 2018 5 -47.239 BHD 2018 6 -47.220 BHD 2018 7 -47.239 BHD 2018 8 -47.302 BHD 2018 9 -47.377 BHD 2018 10 -47.414 BHD 2018 11 -47.393 BHD 2018 12 -47.326 BHD 2019 7 -47.340 BHD 2019 11 -47.456 BHD 2019 12 -47.334 BHD 2020 1 -47.255 BHD 2020 2 -47.266 BHD 2020 3 -47.327 BHD 2020 4 -47.370 BHD 2020 5 -47.372 BHD 2020 6 -47.365 BHD 2020 7 -47.374 BHD 2020 8 -47.393 BHD 2020 9 -47.408 BHD 2020 10 -47.411 BHD 2020 11 -47.401 BHD 2020 12 -47.377 BHD 2021 1 -47.344 BHD 2021 2 -47.323 BHD 2021 3 -47.329 BHD 2021 8 -47.499 BHD 2021 9 -47.554 BHD 2021 10 -47.572