Atlantic Oceanographic & Meteorological Laboratory Global Carbon Cycle

R/V Gordon Gunter Master Readme File

INTRODUCTION:
 
The information presented in this file is applicable to all the data sets collected 
on the R/V Gordon Gunter that are presented at:

     www.aoml.noaa.gov/ocd/gcc/rvgunter_introduction.php.

Any temporary changes in this information will be noted in the readme files for 
the individual expeditions.

Statement for use of data:

These data are made available to the public and the scientific community in the belief 
that their wide dissemination will lead to greater understanding and new insights. The 
availability of these data does not constitute publication of the data. We rely on the 
ethics and integrity of the user to insure that the AOML ocean carbon group receives 
fair credit for its work. Please consult with us prior to use so we can insure that 
the quality and limitations of the data are accurately represented.

Platform Information:

In 2008, the Ocean Carbon Group at NOAA's Atlantic Oceanographic and Meteorological 
Laboratory (AOML) installed an instrument to measure CO2 levels in surface water and 
air on the NOAA Ship Gordon Gunter. The Gordon Gunter primarily operates in the Gulf 
of Mexico, Atlantic and Caribbean waters.

Vessel Name: R/V Gordon Gunter

Class of Data:  Surface ocean carbon dioxide concentrations

Scientists responsible for the technical quality of this pCO2 dataset:

     Rik Wanninkhof and Denis Pierrot
     NOAA/AOML/Ocean Chemistry Division
     4301 Rickenbacker Causeway
     Miami, FL 33149
     Rik.Wanninkhof@noaa.gov
     Denis.Pierrot@noaa.gov

Contact persons for this dataset:

     Kevin Sullivan and Denis Pierrot
     NOAA/AOML/Ocean Chemistry Division
     4301 Rickenbacker Causeway
     Miami,  FL 33149
     Kevin.Sullivan@noaa.gov
     Denis.Pierrot@noaa.gov



COMPONENT SPECIFICATIONS and ACCURACIES:

The accuracies of all components, when operating optimally, are such that the calculated 
seawater fCO2 has an accuracy of 2 uatm or better and the calculated mole fraction of CO2 
(XCO2) in air has an accuracy of 0.1 uatm.

Infrared Analyzer:
    LI-COR model 6262 (2008-August 2010)
         ftp://ftp.licor.com/perm/env/LI-6262/Manual/LI-6262_Manual.pdf
         CO2 resolution:  0.01 umol/m
         CO2 accuracy: ± 1 ppm at 350 ppm
         Internal pressure transducer accuracy: ± 1.2 hPa 
              (manufacturer specifications: ±0.1% FS, where FS = 0-1150 hPa) 
   
   LI-COR model 7000 (August 2010 - current)
         ftp://ftp.licor.com/perm/env/LI-7000/Manual/LI-7000Manual.pdf
         CO2 resolution:  0.01 umol/m
         CO2 accuracy: ± 1% nominal
         Internal pressure transducer accuracy: ± 1.2 hPa 
             (manufacturer specifications: ±0.1% FS, where FS = 0-1150 hPa) 
 
Equilibrator Pressure Transducer:
    Setra model 239, differential pressure (2008 ? current)
        http://www.setra.com/ProductDetails/model_239.htm 
        Resolution:  0.01 hPa
        Accuracy: ± 0.052 hPa 
            (manufacturer specifications: ± 0.14% FS, where FS = ± 7.5 inches WC)

The absolute pressure of the equilibrator headspace reported in data files is the sum 
of the infrared analyzer pressure and the differential pressure from the pressure 
transducer attached to the equilibrator.

Equilibrator Temperature:
    Hart model 1521 (August 2010 - current)
        http://www.testequipmentdepot.com/hart/pdfs/1521_1522.pdf 
        Resolution:  0.001°C 
        Accuracy:  ± 0.025°C

Atmospheric Pressure:
    Druck model RPT 350 (2008 - August 2010)
        http://www.ge-mcs.com/en/pressure-and-level/transducerstransmitters/rtp350.html
        Resolution: 0.01 hPa
        Accuracy: ± 0.08 hPa  
        (manufacturer specifications: ± 0.02% FS, where FS = 400 hPa)

    RMYoung model 61201 (maintained by ship) (August 2010 - present)
        http://jsinstruments.com/files/Model%2061201%20Barometric%20Pressure%20Sensor.pdf
        Resolution: 0.01 hPa
        Accuracy: ± 0.5 hPa  
       
Sea Surface Salinity (maintained by ship):
    SeaBird model SBE-21 (2008 - present)
        http://www.seabird.com/pdf_documents/manuals/21_027.pdf
        Temperature Accuracy: ± 0.01 °C 
        Salinity Accuracy:    0.05 ‰

Sea Surface Temperature (maintained by ship):
    Furuno model T2000 (2008 - 2012)
        Furuno T2000 Manual pdf
		Temperature Resolution: 0.01 °C 
        Temperature Accuracy: ± 0.02 °C 

Sea Surface Temperature (maintained by ship):
    SeaBird model SBE-38 (2013 - present)
        http://www.seabird.com/pdf_documents/manuals/38_013.pdf 
        Temperature Resolution: 0.00025°C
        Temperature Accuracy: ± 0.001°C
 
INSTRUMENT DESCRIPTION and CONFIGURATION:

The general principle of operation of the instrument can be found in Wanninkhof 
and Thoning (1993), Ho et al. (1995), Feely et al. (1998), and Pierrot et al. (2009). 
Seawater flows through an equilibrator chamber where CO2 exchanges between water and 
the air above it. Small changes in seawater CO2 concentration are rapidly translated 
into changes in CO2 concentration in the air of the chamber (headspace). The mole 
fraction of CO2 in the headspace gas is measured using a non-dispersive infrared 
(NDIR) analyzer from LICOR®.

The effects of water vapor on the signal can be compensated for by the analyzer 
(LiCOR model 6262) but are also kept to a minimum by removing as much water as 
possible. The water is first condensed out of the gas stream by cooling. Then it 
is further removed using Nafion® gas dryers before reaching the IR analyzer. 
Typical water content of the gas streams are less than 3 millimoles/mole with 
approximately 90% of the water removed.

The infrared analyzer is calibrated regularly using four standard gases (200 - 450 ppm 
CO2 in air) from Scott-Martin Inc. (Riverside, CA). Before and after use in the field, 
the standards are calibrated using primary reference gases from the laboratory of 
Dr. Charles P. Keeling, which are directly traceable to the WMO scale. Any value 
outside the range of the standards should be considered approximate (+/-5 ppm).  
While individual data points above the highest standard or below the lowest 
standard may be less accurate, the general trends would be indicative of the 
seawater chemistry. The exact concentrations of the standards used on a particular 
cruise are listed in the individual readme file.

The system also measures the CO2 content of the outside air, which is drawn from an inlet 
on the box mast approximately 15 meters above the water. Atmospheric air was constantly being pulled 
(6 liters/min maximum flow) through ~200 feet of tubing (3/8" OD Dekoron) to the analytical 
system located located in the web lab.  The seawater is drawn from the ship's flowing 
seawater line, which also feeds a thermosalinograph and Turner fluorometer.

The three CO2 standard cylinders come from Scott-Marrin, Inc., and are calibrated with 
primary standards that are directly traceable to the WMO scale. The zero gas is ultra-high 
purity air. Any value outside the range of the standards should be considered approximate 
(+/-5 ppm). While individual data points above the highest standard or below the lowest 
standard may less accurate, the general trends would be indicative of the seawater 
chemistry. The standards used on a particular cruise are listed in the individual readme file.

A 'Deck Box' containing a high precision pressure transducer, a GPS and Iridium satellite 
modem is located outside and several decks above the system on part of the ship's 
superstructure protected from severe weather. The instrumental system via the deck box 
records the atmospheric pressure and the position of the ship. The measured pressure is 
corrected for the height of the barometer above the sea surface with the addition of 
dgh/u - where d is atmospheric density (1.2 kg/m3), g is gravitational acceleration 
(9.8 m/sec2), h is height of the barometer above the sea surface, and u is the conversion 
factor from pascals to desired pressure units. The estimated height of 15 meters resulted 
in a change in the barometric pressure of approximately of 1.8 mbar.

A typical sequence of continuous analyses was:

STEP     TYPE                  REPETITIONS
 1       Standards (all four)      1
 2       ATM                       5
 3       EQU                      60

The amount of time between analyses depends on whether the analyses are of the same type 
of gas (e.g., STD, ATM, EQU) or not. When switching between different gases, the connecting 
tubes and analyzer are flushed for an initial interval called the 'PRE-FLUSH' time plus an 
interval called the 'REGULAR FLUSH' time. Between successive measurements of the same type 
of gas, the system is flushed for only the 'REGULAR FLUSH' time. The gas flow is then stopped. 
After the 'STOP FLOW' time interval, which is 10 seconds for all analyses, the output of the 
NDIR analyzer is read. The pre-flush time is set to 180 seconds and the regular flush time is 
set to 60 seconds for standard and air analyses. Both the pre-flush and regular flush times 
are 120 seconds for equilibrator headspace analyses. With these settings, a complete set of 
standards and the atmospheric analyses are done every 3 hours and a full day contains about 
480 analyses of the equilibrator headspace.



CALCULATIONS:

The measured xCO2 values are linearly corrected for instrument response using the standard 
measurements (see Pierrot et al., 2009).

For ambient air and equilibrator headspace the fCO2a or fCO2eq is calculated assuming 100% 
water vapor content:

   fCO2 = xCO2 P (1-pH2O) exp[(B11+2d12)P/RT]

where fCO2 is the fugacity in ambient air or equilibrator, pH2O is the water vapor pressure 
at the sea surface or equilibrator temperature, P is the equilibrator or outside atmospheric 
pressure (in atm), T is the SST or equilibrator temperature (in K) and R is the ideal gas 
constant (82.057 cm^3·atm·deg^-1·mol^-1). The exponential term is the fugacity correction 
where B11 is the first virial coefficient of pure CO2 

   B11 = -1636.75 + 12.0408 T - 0.0327957 T^2 + 3.16528E-5 T^3

and

   d12 = 57.7 - 0.118 T

is the correction for an air-CO2 mixture in units of cm^3·mol^-1 (Weiss, 1974). 

The fugacity as measured in the equilibrator is corrected for any temperature difference 
between sea surface temperature and equilibrator chamber using the empirical correction 
outlined in Takahashi et al. (1993).

   fCO2(SST) = fCO2(teq)exp[0.0423(SST-teq)]
   
where fCO2(SST) is the fugacity at the sea surface temperature and fCO2(teq) is the fugacity 
at the equilibrator temperature. SST and teq are the sea surface and equilibrator temperatures 
in degrees C, respectively.  



DATA FILE STRUCTURE:

List of variables included in this dataset:

COLUMN  HEADER                    EXPLANATION

1.   Group_Ship                   AOML_GGunter

2.   Cruise_ID                    dependent upon expedition's name

3.   JD_GMT                       Decimal year day

4.   DATE_UTC_ddmmyyyy            UTC Date

5.   TIME_UTC_hh:mm:ss            UTC Time

6.   LAT_dec_degree               Latitude in decimal degrees (negative
                                  values are in southern hemisphere)

7.   LONG_ dec_degree             Longitude in decimal degrees (negative
                                  values are in western latitudes)

8.   xCO2_EQU_ppm                 Mole fraction of CO2 in the equilibrator
                                  headspace (dry) at equilibrator
                                  temperature, in parts per million

9.   xCO2_ATM_ppm                 Mole fraction of CO2 in outside air (dry), 
                                  in parts per million

10.  xCO2_ATM_interpolated_ppm    xCO2 in outside air associated with each 
                                  water analysis.  These values are 
                                  interpolated between the bracketing 
                                  averaged good xCO2_ATM analyses, in parts 
                                  per million

11.  PRES_EQU_hPa                 Barometric pressure in the equilibrator 
                                  headspace, in hectopascals (1 hPa = 1 millibar)

12.  PRES_ATM@SSP_hPa             Pressure measured by outside barometer,
                                  corrected to sea level, in hectopascals 

13.  TEMP_EQU_C                   Water temperature in equilibrator, in 
                                  degrees centigrade

14.  SST_C                        Sea surface temperature from the ship's 
                                  remote temperature sensor, in degrees centigrade 
                                  [interpolated, see note below]

15.  SAL_permil                   Salinity from the thermosalinograph
                                  (SBE45), on the Practical Salinity Scale

16.  fCO2_SW@SST_uatm             Fugacity of CO2 in sea water, in 
                                  Microatmospheres (100% humidity)

17.  fCO2_ATM_interpolated_uatm   Fugacity of CO2 in air corresponding to the 
                                  interpolated xCO2, in microatmospheres
                                  (100% humidity)

18.  dfCO2_uatm                   Sea water fCO2 minus interpolated air fCO2, 
                                  in microatmospheres
									 
19.  WOCE_QC_FLAG                 Quality control flag for fCO2 values
                                  (2 = good value, 3 = questionable value)

20.  QC_SUBFLAG                   Quality control sub flag for fCO2 values 
                                  provides explanation for atypical data,
                                  when QC_FLAG = 3

The quality control flags are provided as an aid to the interpretation of the CO2 data. 
The amount of time between the sea water entering the ship and the water flowing through 
the equilibrator is estimated before assigning an SST value to each analysis. The patterns 
in the temperature records for the equilibrator and for SST over time are compared, and a 
time offset that optimizes the match of these patterns is determined.  The time offset is 
applied to the SST measurements. A linear interpolation between the time-adjusted SST 
data yields the SST value assigned to each CO2 analysis and used in the fugacity calculations.



REFERENCES:

DOE (1994). Handbook of methods for the analysis of the various parameters of the carbon 
	dioxide system in sea water; version 2. DOE.
Feely, R. A., R. Wanninkhof, H. B. Milburn, C. E. Cosca, M. Stapp and P. P. Murphy (1998). 
	A new automated underway system for making high precision pCO2 measurements onboard 
	research ships. Analytica Chim. Acta 377: 185-191.
Ho, D. T., R. Wanninkhof, J. Masters, R. A. Feely and C. E. Cosca (1997). Measurement of 
	underway fCO2 in the Eastern Equatorial Pacific on NOAA ships BALDRIGE and 
	DISCOVERER, NOAA data report ERL AOML-30, 52 pp., NTIS Springfield, 
Pierrot, D., C. Neill, K. Sullivan, R. Castle, R. Wanninkhof, H. Luger, T. Johannessen,
    A. Olsen, R. A. Feely, and C. E. Cosca (2009).  Recommendations for autonomous 
    underway pCO2 measuring systems and data-reduction routines.  Deep Sea Research II,
    56: 512-522. 
Wanninkhof, R. and K. Thoning (1993) Measurement of fugacity of CO2 in surface water using 
	continuous and discrete sampling methods. Mar. Chem. 44(2-4): 189-205.
Weiss, R. F. (1970). The solubility of nitrogen, oxygen and argon in water and seawater. 
	Deep-Sea Research 17: 721-735.
Weiss, R. F. (1974). Carbon dioxide in water and seawater: the solubility of a non-ideal gas. 
	Mar. Chem. 2: 203-215.
Weiss, R. F., R. A. Jahnke and C. D. Keeling (1982). Seasonal effects of temperature and 
	salinity on the partial pressure of CO2 in seawater. Nature 300: 511-513.
Takahashi, T., J. Olafsson, J. G. Goddard, D. W. Chipman, and S. C. Sutherland (1993).
    Seasonal variation of CO2 and nutrients in the high-latitude surface oceans: a comparative
    study, Global Biogeochem. Cycles, 7, 843-878.

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