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Dr Grant Forster

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Instrument Support Level 3
Instrument Support Level

Instrument Support Level 3

Manufacturer & Model

Trace Analytical, Inc, RGA3,

Daily Facility Charge

Not Applicable

Calendar

Calendar 2:
Reduction Gas Analyser - H2 Monitor

Reduction Gas Analyser - H2 Monitor

The Reduction Gas Analyser (RGA) at Weybourne Atmospheric Observatory is used to make quasi-continuous measurements of molecular hydrogen (H2) in atmospheric air. Measurements are made using a modified commercial Reduction Gas Analyser (RGA3, Trace Analytical, Inc., California, USA), which includes gas chromatography followed by the reduction of mercuric oxide. Mercury vapour from this reaction was detected by UVabsorption.

H2 Samples are analysed every six minutes and with reference to the MPI2009 scale

Routine analysis of molecular hydrogen (H2) is achieved using a modified commercial Reduction Gas Analyser (RGA3, Trace Analytical, Inc., California, USA), which includes gas chromatography followed by the reduction of mercuric oxide. Mercury vapour from this reaction is detected by UV absorption. Air is drawn from the top of the sampling tower through ¼” tubing (Synflex 1300) at a flow rate of 200 cm3 min1 using an air pump (Rietschle Thomas, UK) downstream of the sample loop. To prevent particulate matter from entering the analytical instrumentation the sample line is fitted with a 40-micron filter at the top of the tower and a 2-micron filter at the base of the tower (TF-series, Swagelok). The air is passed through a moisture trap (silica beads) before entering a 1 cm3 sample loop. The air pump is turned off 20 s prior to sample injection to allow pressure equilibration of the sample loop. The pressure and the temperature of the sample loop are monitored throughout analysis using a pressure sensor(WIKA A10) and temperature sensor (NOVUS TxRail), respectively.

When the sample loop has equilibrated the content is injected onto a pre-column consisting of Unibeads 1S (Grace, mesh 60/80; 1/8 in. OD x 76 cm length) at 95°C to separate H2 from any remaining contaminant water vapour (H2O), carbon dioxide (CO2) and hydrocarbons. After 1 min the sample is redirected to an analytical column containing Molecular Sieve 5A (Supelco, mesh 60/80; 1/8 in. OD x 76 cm length) also at 95°C to further separate H2. At this time the pre-column is back-flushed. H2 elute from the analytical column at 0.5 mins and 2.2 min, respectively, at which time they pass through the mercuric oxide bed (HgO). Any mercury vapour (Hg) liberated during the reduction of the HgO at 265°C enters the detector and is measured using UV absorption (Reaction 1).

             X + HgO (solid) → XO + Hg (vapour)       Reaction 1

where X is H2.

Synthetic air (BTCA air 178, BOC) is used as a carrier gas with a flow of 17 cm3 min-1. Prior to entering the system, any contaminant H2 is removed using SOFNOCAT 514 (Molecular Products Ltd). In addition, the carrier gas passes through a catalytic converter to convert any H2 to H2O. This is then removed using a molecular sieve trap before entering the GC columns.

A run time of 6 min allows eight air samples to be analysed every hour with a working standard analysed after every fourth run. This results in eight fully calibrated measurements of H2. Detector response, sample loop pressure and temperature are all recorded using a six-channel analogue to digital acquisition system (Model 302, SRI Instruments, California, USA) and subsequent peak analysis is performed using Peak Simple software (SRI Instruments). Normalised peak heights (peak height / average of bracketing working standards) measured from samples are referenced to the instruments non-linear response function determined using calibrated primary reference gases on the MPI-2009 scale for H2 (Jordan and Steinberg, 2011).  The range of concentrations in the primary reference gases is 375 ppb to 1182 ppb for H2 (5 cylinders). Instrument repeatability is assessed by calculating the deviation in the concentration of the working standard from the bracketing two working standards as the concentration of this is known as it is determined at the same time as the non-linear response function. Using this approach the repeatability of the system is typically better than ± 5 ppb for H2. The accuracy of the system is assessed through the analysis of a target gas every 6 hours. The target gas is a cylinder of gas with accurately assigned concentrations of the target species determined at a central calibration laboratory (in this instance MPI). This target gas is introduced to the system as a sample and the following analysis the deviation of H2 and CO concentration from the assigned concentrations are calculated. Estimated accuracies using this approach are routinely better than ± 5 ppb for H2.

Routine data work-up occurs on a monthly basis using bespoke procedures written for Igor Pro.

Reference

Jordan, A, and Steinberg, B. 2011. Calibration of atmospheric hydrogen measurements.

The non-linear response function of the Reduction Gas Analyser is determined using calibrated primary reference gases on the MPI-2009 scale for H2 (Jordan and Steinberg, 2011). The range of concentration in the primary reference gases is 375 ppb to 1182 ppb for H2 (5 cylinders). This non-linearity response function is determined every 1 – 2 months. Instrument repeatability is assessed by calculating the deviation in the concentration of the working standard from the bracketing two working standards as the concentration of this is known as it is determined at the same time as the non-linear response function. The accuracy of the system is assessed through the analysis of a target gas every 6 hours. The target gas is a cylinder of gas with accurately assigned concentrations of the target species determined at a central calibration laboratory (in this instance MPI). This target gas is introduced to the system as a sample and the following analysis the deviation of H2 concentration from the assigned concentrations is calculated. We also take part in International inter-comparison programs (i.e. WMO round-robins, Cucumbers),

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