# 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: CO CCGG (Individual Flasks) # contact_name: Gabrielle Petron # contact_telephone: (720) 295-0145 # contact_email: Gabrielle.Petron@noaa.gov # comment: # comment: ************ COLLABORATORS *************** # comment: # comment: NOAA thanks the following collaborators without # comment: whom these measurements would not be possible. # comment: # collaborator_name: Environment Canada [EC] # collaborator_url: http://www.ec.gc.ca/default.asp?lang=En&n=FD9B0E51-1 # 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: alt # description_project-abbr: ccg_surface # description_strategy-abbr: flask # description_analysis-constraints: flag:..% # description_creation-time: 2022-07-28 12:38:44 # 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 ALT 1992 4 177.36 ALT 1992 5 165.29 ALT 1992 6 130.65 ALT 1992 7 95.36 ALT 1992 8 90.39 ALT 1992 9 102.69 ALT 1992 10 115.75 ALT 1992 11 134.23 ALT 1992 12 160.08 ALT 1993 1 175.57 ALT 1993 2 179.64 ALT 1993 3 185.35 ALT 1993 4 183.52 ALT 1993 5 154.33 ALT 1993 6 114.09 ALT 1993 7 87.82 ALT 1993 8 91.91 ALT 1993 9 107.92 ALT 1993 10 117.92 ALT 1993 11 127.43 ALT 1993 12 148.97 ALT 1994 1 173.75 ALT 1994 2 189.40 ALT 1994 3 196.17 ALT 1994 4 185.66 ALT 1994 5 157.22 ALT 1994 6 116.99 ALT 1994 7 92.43 ALT 1994 8 96.44 ALT 1994 9 115.63 ALT 1994 10 129.07 ALT 1994 11 137.52 ALT 1994 12 152.98 ALT 1995 1 169.90 ALT 1995 2 179.68 ALT 1995 3 181.16 ALT 1995 4 169.35 ALT 1995 5 144.68 ALT 1995 6 111.24 ALT 1995 7 92.41 ALT 1995 8 94.27 ALT 1995 9 101.66 ALT 1995 10 109.33 ALT 1995 11 124.19 ALT 1995 12 142.82 ALT 1996 1 158.57 ALT 1996 2 173.12 ALT 1996 3 178.13 ALT 1996 4 170.39 ALT 1996 5 147.75 ALT 1996 6 114.43 ALT 1996 7 93.04 ALT 1996 8 96.00 ALT 1996 9 110.56 ALT 1996 10 118.17 ALT 1996 11 127.15 ALT 1996 12 145.00 ALT 1997 1 166.70 ALT 1997 2 175.15 ALT 1997 3 172.03 ALT 1997 4 164.09 ALT 1997 5 141.12 ALT 1997 6 106.10 ALT 1997 7 81.52 ALT 1997 8 77.67 ALT 1997 9 88.65 ALT 1997 10 107.22 ALT 1997 11 126.31 ALT 1997 12 147.89 ALT 1998 1 173.59 ALT 1998 2 184.94 ALT 1998 3 181.99 ALT 1998 4 174.71 ALT 1998 5 157.53 ALT 1998 6 127.08 ALT 1998 7 98.48 ALT 1998 8 108.46 ALT 1998 9 146.88 ALT 1998 10 177.88 ALT 1998 11 181.52 ALT 1998 12 182.19 ALT 1999 1 188.02 ALT 1999 2 187.74 ALT 1999 3 184.77 ALT 1999 4 179.15 ALT 1999 5 155.58 ALT 1999 6 120.15 ALT 1999 7 92.03 ALT 1999 8 86.19 ALT 1999 9 92.33 ALT 1999 10 103.36 ALT 1999 11 119.31 ALT 1999 12 140.55 ALT 2000 1 157.10 ALT 2000 2 165.70 ALT 2000 3 170.57 ALT 2000 4 166.07 ALT 2000 5 145.23 ALT 2000 6 109.53 ALT 2000 7 85.39 ALT 2000 8 84.31 ALT 2000 9 92.99 ALT 2000 10 101.46 ALT 2000 11 113.21 ALT 2000 12 130.56 ALT 2001 1 146.88 ALT 2001 2 157.58 ALT 2001 3 164.36 ALT 2001 4 164.13 ALT 2001 5 142.46 ALT 2001 6 106.54 ALT 2001 7 84.79 ALT 2001 8 82.86 ALT 2001 9 93.44 ALT 2001 10 105.68 ALT 2001 11 120.40 ALT 2001 12 136.93 ALT 2002 1 152.38 ALT 2002 2 161.98 ALT 2002 3 165.69 ALT 2002 4 161.67 ALT 2002 5 137.91 ALT 2002 6 102.43 ALT 2002 7 85.09 ALT 2002 8 97.73 ALT 2002 9 124.52 ALT 2002 10 139.83 ALT 2002 11 145.31 ALT 2002 12 154.07 ALT 2003 1 171.84 ALT 2003 2 186.48 ALT 2003 3 187.36 ALT 2003 4 177.16 ALT 2003 5 155.98 ALT 2003 6 128.91 ALT 2003 7 108.72 ALT 2003 8 107.92 ALT 2003 9 120.49 ALT 2003 10 133.55 ALT 2003 11 141.42 ALT 2003 12 148.99 ALT 2004 1 158.25 ALT 2004 2 164.70 ALT 2004 3 170.12 ALT 2004 4 170.78 ALT 2004 5 150.53 ALT 2004 6 117.72 ALT 2004 7 93.00 ALT 2004 8 92.62 ALT 2004 9 102.66 ALT 2004 10 109.21 ALT 2005 4 167.93 ALT 2005 5 142.80 ALT 2005 6 104.77 ALT 2005 7 83.93 ALT 2005 8 86.71 ALT 2005 9 96.35 ALT 2005 10 106.57 ALT 2005 11 122.63 ALT 2005 12 140.63 ALT 2006 1 147.57 ALT 2006 2 152.29 ALT 2006 3 162.52 ALT 2006 4 163.18 ALT 2006 5 145.07 ALT 2006 6 111.70 ALT 2006 7 86.22 ALT 2006 8 84.08 ALT 2006 9 93.95 ALT 2006 10 104.01 ALT 2006 11 120.33 ALT 2006 12 139.21 ALT 2007 1 149.19 ALT 2007 2 154.62 ALT 2007 3 162.97 ALT 2007 4 163.57 ALT 2007 5 139.80 ALT 2007 6 105.55 ALT 2007 7 87.70 ALT 2007 8 86.31 ALT 2007 9 92.36 ALT 2007 10 101.69 ALT 2007 11 119.13 ALT 2007 12 137.28 ALT 2008 1 149.81 ALT 2008 2 160.08 ALT 2008 3 166.32 ALT 2008 4 162.35 ALT 2008 5 139.85 ALT 2008 6 108.52 ALT 2008 7 88.91 ALT 2008 8 86.50 ALT 2008 9 90.96 ALT 2008 10 96.84 ALT 2008 11 108.86 ALT 2008 12 129.18 ALT 2009 1 149.10 ALT 2009 2 153.44 ALT 2009 3 153.34 ALT 2009 4 153.21 ALT 2009 5 135.24 ALT 2009 6 104.56 ALT 2009 7 82.51 ALT 2009 8 84.29 ALT 2009 9 93.36 ALT 2009 10 99.79 ALT 2009 11 109.03 ALT 2009 12 125.79 ALT 2010 1 140.88 ALT 2010 2 147.40 ALT 2010 3 151.04 ALT 2010 4 151.85 ALT 2010 5 137.46 ALT 2010 6 109.72 ALT 2010 7 87.22 ALT 2010 8 91.34 ALT 2010 9 108.19 ALT 2010 10 116.46 ALT 2010 11 118.79 ALT 2010 12 127.83 ALT 2011 1 141.70 ALT 2011 2 150.93 ALT 2011 3 155.68 ALT 2011 4 150.53 ALT 2011 5 130.13 ALT 2011 6 99.53 ALT 2011 7 81.79 ALT 2011 8 80.66 ALT 2011 9 86.74 ALT 2011 10 98.41 ALT 2011 11 114.27 ALT 2011 12 130.10 ALT 2012 1 136.63 ALT 2012 2 140.40 ALT 2012 3 150.40 ALT 2012 4 153.53 ALT 2012 5 131.41 ALT 2012 6 98.57 ALT 2012 7 88.33 ALT 2012 8 104.92 ALT 2012 9 120.99 ALT 2012 10 120.47 ALT 2012 11 120.59 ALT 2012 12 133.54 ALT 2013 1 147.26 ALT 2013 2 150.91 ALT 2013 3 151.31 ALT 2013 4 149.81 ALT 2013 5 132.20 ALT 2013 6 102.53 ALT 2013 7 86.49 ALT 2013 8 88.89 ALT 2013 9 97.50 ALT 2013 10 103.13 ALT 2013 11 111.96 ALT 2013 12 122.56 ALT 2014 1 132.38 ALT 2014 2 142.54 ALT 2014 3 149.47 ALT 2014 4 146.38 ALT 2014 5 126.48 ALT 2014 6 97.82 ALT 2014 7 85.55 ALT 2014 8 98.62 ALT 2014 9 111.70 ALT 2014 10 114.55 ALT 2014 11 120.03 ALT 2014 12 130.55 ALT 2015 1 140.80 ALT 2015 2 149.84 ALT 2015 3 154.43 ALT 2015 4 146.32 ALT 2015 5 123.55 ALT 2015 6 101.48 ALT 2015 7 90.47 ALT 2015 8 92.38 ALT 2015 9 98.27 ALT 2015 10 107.65 ALT 2015 11 118.90 ALT 2015 12 130.17 ALT 2016 1 140.06 ALT 2016 2 145.98 ALT 2016 3 148.97 ALT 2016 4 143.38 ALT 2016 5 124.50 ALT 2016 6 96.92 ALT 2016 7 81.93 ALT 2016 8 83.88 ALT 2016 9 92.67 ALT 2016 10 101.38 ALT 2016 11 111.22 ALT 2016 12 126.24 ALT 2017 1 139.29 ALT 2017 2 145.74 ALT 2017 3 147.76 ALT 2017 4 139.91 ALT 2017 5 119.94 ALT 2017 6 90.49 ALT 2017 7 72.88 ALT 2017 8 82.34 ALT 2017 9 104.03 ALT 2017 10 115.33 ALT 2017 11 119.94 ALT 2017 12 127.69 ALT 2018 1 135.34 ALT 2018 2 139.42 ALT 2018 3 144.08 ALT 2018 4 144.98 ALT 2018 5 125.77 ALT 2018 6 92.79 ALT 2018 7 75.76 ALT 2018 8 85.45 ALT 2018 9 104.83 ALT 2018 10 110.97 ALT 2018 11 112.54 ALT 2018 12 121.89 ALT 2019 1 132.64 ALT 2019 2 138.67 ALT 2019 3 141.69 ALT 2019 4 137.43 ALT 2019 5 116.47 ALT 2019 6 90.10 ALT 2019 7 83.52 ALT 2019 8 100.89 ALT 2019 9 116.46 ALT 2019 10 112.88 ALT 2019 11 109.45 ALT 2019 12 117.92 ALT 2020 1 131.18 ALT 2020 2 138.15 ALT 2020 3 139.02 ALT 2020 4 133.75 ALT 2020 5 115.91 ALT 2020 6 93.52 ALT 2020 7 79.84 ALT 2020 8 86.70 ALT 2020 9 105.40 ALT 2020 10 123.13 ALT 2020 11 127.65 ALT 2020 12 125.88 ALT 2021 1 128.24 ALT 2021 2 134.77 ALT 2021 3 140.61 ALT 2021 4 138.03 ALT 2021 5 120.04 ALT 2021 6 93.74 ALT 2021 7 82.81 ALT 2021 8 111.92 ALT 2021 9 145.02 ALT 2021 10 143.37 ALT 2021 11 130.07 ALT 2021 12 133.56