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Real-time, in situ measurement of H2O generated during in situ combustion tests using 1f-normalized wavelength modulation spectroscopy with second harmonic detection

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Abstract

The development and deployment of a real-time, in situ, non-invasive sensor to monitor the concentration of ${{\rm H}_2}{\rm O}$ during in situ combustion (ISC) experiments with a heavy-crude oil is described. A real-time sensor to monitor the gas-phase products from ISC can support the study of the kinetics of the complex chemical reactive system in ISC. The mole fraction of ${{\rm H}_2}{\rm O}$ was measured using tunable diode laser (TDL) absorption spectroscopy coupled with $1f$-normalized wavelength modulation spectroscopy (WMS) and ${2f}$ detection. The WMS ${2f/1f}$ strategy was used to enhance sensitivity with effective noise rejection, particularly suitable when characterizing the water vapor evolved from oil–water emulsions. ${{\rm H}_2}{\rm O}$ was measured at ${3934.10}\;{{\rm cm}^{- 1}}$ from the fundamental band ${{v}_3}$. That transition was selected using the HITRAN database to increase the line strength and minimize interference from neighbor compounds. Measurements of ${{\rm H}_2}{\rm O}$ concentration were conducted at ambient temperature and pressure using a reference cell (${{\rm H}_2}{\rm O} = {2}\%$ at 98.6 kPa) to validate the sensor architecture under controlled laboratory environments. The TDL sensor was also successfully validated during real ISC experiments involving heavy-crude oil. Validation and combustion experiments showed the potential of the TDL-based sensor for non-invasive, real-time, in situ measurements of gas-phase species in conditions similar to those of laboratory-scale experimental ISC tests.

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Supplementary Material (9)

NameDescription
Data File 1       Calculated absorbance spectra of H2O, CO, and CO2 near 3934.10 cm-1. The figure legend indicates the mole fraction composition, temperature (T), pressure (P), and pathlength (L) used in the simulation.
Data File 2       Thermal sensitivity of the line at 3934.10 cm-1 that was selected for the measurement of the H2O concentration at conditions relevant to ISC experiments
Data File 3       Comparison of the measured and simulated laser signal after a preliminary fit of the parameters in the Airy function to determine the initial parameters of the time-dependent laser frequency ?(t).
Data File 4       Comparison of the measured and simulated laser signal after the final fine-tuning of the parameters in the Airy function of the time-dependent laser frequency ?(t).
Data File 5       Comparison of the simulated and measured WMS 2f/1f signals. The red signal can now be used to infer the water concentration
Data File 6       Variation of the H2O mole fraction when measuring air at room conditions. Three tests carried out at different times are presented. The variations agreed with those expected from an uncontrolled atmosphere
Data File 7       Measured variation of the H2O in the reactor when a stream of N2 with a known water concentration was diluted with N2. The flow of the dilution stream was increased at 3250 s, 4000 s, and 4950 s.
Data File 8       Measurement of water vapor production using the WMS 2f/1f TDL sensor during the in situ combustion of a Colombian heavy oil. The figure also shows CO2, CO, and O2 concentrations as measured downstream by a gas analyzer
Supplement 1       Supplemental document

Data Availability

Data underlying the results presented in this paper are available as Data File 1Data File 8 within the paper.

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