2016
DOI: 10.1177/0003702815626672
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High-Pressure Measurements of Temperature and CO2 Concentration Using Tunable Diode Lasers at 2 μm

Abstract: A sensor for simultaneous measurements of temperature and carbon dioxide (CO2) concentration at elevated pressure is developed using tunable diode lasers at 2 µm. Based on some selection rules, a CO2 line pair at 5006.140 and 5010.725 cm(-1) is selected for the TDL sensor. In order to ensure the accuracy and rapidity of the sensor, a quasi-fixed-wavelength WMS is employed. Normalization of the 2f signal with the 1f signal magnitude is used to remove the need for calibration and correct for transmission variati… Show more

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Cited by 17 publications
(7 citation statements)
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“…Similarly, the temperature expression of WMS and WMS‐2f/1f can also be deduced with the following expressions 5,10,11 TWMS=italichckE2E1ln(RWMS)+lnS2(T0)S1(T0)+hckE2E1T0+lnI(ν2true¯)M2I(ν1true¯)M1, ${T}_{\mathrm{WMS}}=\frac{\frac{{hc}}{k}\left({E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }\right)}{\mathrm{ln}({R}_{\mathrm{WMS}})+\mathrm{ln}\left(\frac{{S}_{2}({T}_{0})}{{S}_{1}({T}_{0})}\right)+\left(\frac{{hc}}{k}\right)\left(\frac{{E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }}{{T}_{0}}\right)+\mathrm{ln}\left(\frac{I(\bar{{\nu }_{2}}){M}_{2}}{I(\bar{{\nu }_{1}}){M}_{1}}\right)},$ TWMS2f/1f=italichckE2E1ln(RWMS2normalf/1normalf)+lnS2(T0)S1(T0)+hckE2E1T0+lnM2M1, ${T}_{\mathrm{WMS}-2{\rm{f}}/1{\rm{f}}}=\frac{\frac{{hc}}{k}\left({E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }\right)}{\mathrm{ln}({R}_{\mathrm{WMS}-2{\rm{f}}/1{\rm{f}}})+\mathrm{ln}\left(\frac{{S}_{2}({T}_{0})}{{S}_{1}({T}_{0})}\right)+\left(\frac{{hc}}{k}\right)\left(\frac{{E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }}{{T}_{0}}\right)+\mathrm{ln}\left(\frac{{M}_{2}}{{M}_{1}}\right)},$<...…”
Section: The Principle Of Temperature Measurementmentioning
confidence: 99%
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“…Similarly, the temperature expression of WMS and WMS‐2f/1f can also be deduced with the following expressions 5,10,11 TWMS=italichckE2E1ln(RWMS)+lnS2(T0)S1(T0)+hckE2E1T0+lnI(ν2true¯)M2I(ν1true¯)M1, ${T}_{\mathrm{WMS}}=\frac{\frac{{hc}}{k}\left({E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }\right)}{\mathrm{ln}({R}_{\mathrm{WMS}})+\mathrm{ln}\left(\frac{{S}_{2}({T}_{0})}{{S}_{1}({T}_{0})}\right)+\left(\frac{{hc}}{k}\right)\left(\frac{{E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }}{{T}_{0}}\right)+\mathrm{ln}\left(\frac{I(\bar{{\nu }_{2}}){M}_{2}}{I(\bar{{\nu }_{1}}){M}_{1}}\right)},$ TWMS2f/1f=italichckE2E1ln(RWMS2normalf/1normalf)+lnS2(T0)S1(T0)+hckE2E1T0+lnM2M1, ${T}_{\mathrm{WMS}-2{\rm{f}}/1{\rm{f}}}=\frac{\frac{{hc}}{k}\left({E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }\right)}{\mathrm{ln}({R}_{\mathrm{WMS}-2{\rm{f}}/1{\rm{f}}})+\mathrm{ln}\left(\frac{{S}_{2}({T}_{0})}{{S}_{1}({T}_{0})}\right)+\left(\frac{{hc}}{k}\right)\left(\frac{{E}_{2}^{^{\prime\prime} }-{E}_{1}^{^{\prime\prime} }}{{T}_{0}}\right)+\mathrm{ln}\left(\frac{{M}_{2}}{{M}_{1}}\right)},$<...…”
Section: The Principle Of Temperature Measurementmentioning
confidence: 99%
“…TDLAS‐based temperature measurement has been extensively investigated and utilized in recent years. Cai et al demonstrated accurate and fast measurement of carbon dioxide concentration and temperature based on TDLAS 5 . Zhang et al presented the measurement of C 2 H 4 concentration and temperature using TDLAS in the combination of differential absorption scheme 6 …”
Section: Introductionmentioning
confidence: 99%
“…According to the Beer-Lambert law [10], when a monochromatic laser passes through a gas medium, the intensity change can be expressed as:…”
Section: Beer-lambert Lawmentioning
confidence: 99%
“…Sun et al demonstrated the measurement of multi-species concentrations and temperature in a slagging coal gasifier with high pressure and high temperature using TDLAS, proving the capability of TDL sensors to monitor transient changes in gas temperature and the syngas heating value [13]. Cai et al demonstrated accurate and fast measurement of carbon dioxide concentration and temperature based on TDLAS at high temperature and high pressure [14].…”
Section: Introductionmentioning
confidence: 99%
“…Through an investigation of relevant literature, it has been found that there are many studies on measurements of species concentration and temperature by direct absorption spectroscopy (DAS) or wavelength modulation spectroscopy (WMS) employing isolated absorption lines of the measured gas molecules [12][13][14][15][16][17][18][19]. However, for the molecules with dense absorption spectral features (such as ethylene and methane, which contain hydrocarbon bonds), there will be self-mixing or overlap with other molecules at an elevated temperature and pressure, making it difficult to accurately infer the complete transition properties through a single line or line pair.…”
Section: Introductionmentioning
confidence: 99%