2022
DOI: 10.1021/acs.iecr.1c02970
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[C2mim][CH3SO3]─A Suitable New Heat Transfer Fluid? Part 2: Thermophysical Properties of Its Mixtures with Water

Abstract: Ionic liquids have proved to be excellent heat transfer fluids and alternatives to common HTFs used in industries for heat exchangers and other heat transfer equipment. However, its industrial utilization depends on the cost per kg of its production, to be competitive for industrial applications with biphenyl and diphenyl oxide, alkylated aromatics, and dimethyl polysiloxane oils, which degrade above 200 °C and possess some environmental problems. The efficiency of a heat transfer fluid depends on the fundamen… Show more

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Cited by 4 publications
(7 citation statements)
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References 68 publications
(264 reference statements)
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“…The thermomechanical coefficients (isobaric expansivity, α P , isothermal compressibility, κ T , and isentropic compressibility, κ S ), which can provide useful information about an ionic liquid’s structure and molecular interactions, can be easily derived from eqs –): α P = true( 1 ρ true) true( ρ T true) P κ T = κ S + T V m α P 2 C P , m κ S = 1 ρ c 2 where κ S , T , V m , and C P ,m are the isentropic compressibility, temperature, molar volume, and molar isobaric heat capacity of the liquid, respectively. The possible existence of ultrasound absorption, as discussed for [C 2 mim][CH 3 SO 3 ] and as previously discussed by Dzida et al, would originate a lack of reproducibility of the measurements, which was not found for the systems studied here. Therefore, we can conclude that the speed of sound can be considered a pure thermodynamic property, and eq is applicable.…”
Section: Resultssupporting
confidence: 43%
See 3 more Smart Citations
“…The thermomechanical coefficients (isobaric expansivity, α P , isothermal compressibility, κ T , and isentropic compressibility, κ S ), which can provide useful information about an ionic liquid’s structure and molecular interactions, can be easily derived from eqs –): α P = true( 1 ρ true) true( ρ T true) P κ T = κ S + T V m α P 2 C P , m κ S = 1 ρ c 2 where κ S , T , V m , and C P ,m are the isentropic compressibility, temperature, molar volume, and molar isobaric heat capacity of the liquid, respectively. The possible existence of ultrasound absorption, as discussed for [C 2 mim][CH 3 SO 3 ] and as previously discussed by Dzida et al, would originate a lack of reproducibility of the measurements, which was not found for the systems studied here. Therefore, we can conclude that the speed of sound can be considered a pure thermodynamic property, and eq is applicable.…”
Section: Resultssupporting
confidence: 43%
“…The previous analysis showed that the thermal conductivity of water was measured within a value of 0.8%, thus justifying our uncertainty estimate of 2%. The measurements for [C 12 mim][(CF 3 SO 2 ) 2 N] were performed in the LOW heating mode, , and the assumed linear variation transient temperature rise of the hot-wire with the logarithm of time, as given by the theory of the transient hot-wire (THW) method, was confirmed. Figure shows examples of two of the runs, one at 299.92 K and one at 347.95 K, using a heat input per unit length of wire of Q = 0.913 W/m, with a total temperature rise of 1.59 and 1.22 K, respectively.…”
Section: Resultsmentioning
confidence: 99%
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“…Thermal conductivity, λ , measurements were performed at temperatures 295.06 < T /K < 345.55, using commercial equipment from Hukseflux Thermal Sensors TPSYS02 and a non-steady-state probe (NSSP) TP08, SN# 283, with a temperature standard uncertainty of u ( T ) = 0.02 K, as reported earlier . Measurements with water permitted the validation of the probe operation, as described in a recent publication, with data obtained between 300 and 350 K not deviating from the standard reference data value (IUPAC SRD correlation) by more than 0.5%, as obtained before.…”
Section: Methodsmentioning
confidence: 99%