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1

Jain, Preeti, and Anil Kumar. "Enthalpic interactions in aqueous strong electrolytes upon addition of ionic liquids." Physical Chemistry Chemical Physics 20, no. 16 (2018): 11089–99. http://dx.doi.org/10.1039/c7cp07814e.

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The present study deals with the inter-ionic interactions between strong electrolytes and ionic liquids based on the thermodynamic properties such as excess partial molar enthalpy, HEIL, relative apparent molar enthalpy, ϕ<sub>L</sub>, and the enthalpic interaction parameters.
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2

White, Kenneth. "Muybridge’s enthalpy." Public 24, no. 47 (2013): 94–109. http://dx.doi.org/10.1386/public.24.47.94_1.

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3

Nazarov, S. A. "Surface enthalpy." Doklady Physics 53, no. 7 (2008): 383–87. http://dx.doi.org/10.1134/s1028335808070124.

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4

Torres, F. E., P. Kuhn, D. De Bruyker, et al. "Enthalpy arrays." Proceedings of the National Academy of Sciences 101, no. 26 (2004): 9517–22. http://dx.doi.org/10.1073/pnas.0403573101.

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5

Banayan, Nooriel, Arthur Palmer, John Hunt, Elaine Zhang, and Will Hyatt. "Exploring the role of Entropy-Enthalpy compensation in protein crystallization with Molecular Dynamics." Structural Dynamics 12, no. 2_Supplement (2025): A35. https://doi.org/10.1063/4.0000344.

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Protein crystallization is driven by the balance between two fundamental physical factors: entropy and enthalpy. Favorable enthalpic interactions in crystal-packing interfaces promote crystallization, but these generally involve immobilization of sidechains on the surface of the protein, resulting in an entropy loss that opposes crystallization strongly suggesting protein crystallization is strongly influenced by "entropy-enthalpy" compensation. Previous literature has emphasized the deleterious entropy factor in this thermodynamic equation while effectively ignoring the reciprocal beneficial
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6

Kleykamp, Heiko. "Enthalpy, heat capacity and enthalpy of transformation of Li2TiO3." Journal of Nuclear Materials 295, no. 2-3 (2001): 244–48. http://dx.doi.org/10.1016/s0022-3115(01)00550-5.

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7

Giraldo, Liliana, and Juan Carlos Moreno-Piraján. "Enthalpic Contribution of Ni(II) in the Interaction between Carbonaceous Material and Aqueous Solution." Journal of Chemistry 2017 (2017): 1–7. http://dx.doi.org/10.1155/2017/7308024.

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Solid adsorbents were prepared from corn cob that was modified with a solution of HNO3 6 M at different contact times. The solids are characterized by physical N2 adsorption at 77 K to know their surface area by applying the BET model and surface chemistry is determined using the Bohem method. Once we have prepared the adsorbents we determine the immersion enthalpy, ΔHim, of the solids in Ni(II) aqueous solutions of different concentrations between 20 and 800 mg·L−1, with values for ΔHim between 10.0 and 35.3 J·g−1. From the results obtained for the immersion enthalpy in function of the ion Ni
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8

Pinheiro, Bruno D. A., Ana R. R. P. Almeida, and Manuel J. S. Monte. "Phase transitions properties of N,N-dimethyl-4-nitroaniline." U.Porto Journal of Engineering 9, no. 5 (2023): 77–88. http://dx.doi.org/10.24840/2183-6493_009-005_002176.

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The present work reports an experimental study aiming to determine several thermodynamic properties of fusion and sublimation of the chromophore N,N-dimethyl-4-nitroaniline. This compound is commonly used as a reference in studies focused on the non-linear optical (NLO) characteristics of chromophores. Using the Knudsen mass-loss effusion method, the vapor pressures of the crystalline phase of N,N-dimethyl-4-nitroaniline were measured over the temperature range between 341.1 K and 363.5 K. The standard molar enthalpy, entropy, and Gibbs energy of sublimation were calculated from the experiment
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9

Ledo, Juan M., Henoc Flores, Fernando Ramos, and Elsa A. Camarillo. "Thermochemical Study of 1-Methylhydantoin." Molecules 27, no. 2 (2022): 556. http://dx.doi.org/10.3390/molecules27020556.

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Using static bomb combustion calorimetry, the combustion energy of 1-methylhydantoin was obtained, from which the standard molar enthalpy of formation of the crystalline phase at T = 298.15 K of the compound studied was calculated. Through thermogravimetry, mass loss rates were measured as a function of temperature, from which the enthalpy of vaporization was calculated. Additionally, some properties of fusion were determined by differential scanning calorimetry, such as enthalpy and temperature. Adding the enthalpy of fusion to the enthalpy of vaporization, the enthalpy of sublimation of the
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10

DeTar, DeLos F., Seyhun Binzet, and Prashanth Darba. "Formal steric enthalpy." Journal of Organic Chemistry 50, no. 16 (1985): 2826–36. http://dx.doi.org/10.1021/jo00216a004.

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11

Zhao Tai-Ze, Wang Fei, Guo Shao-Feng, Guo Wen-Kang, and Xu Ping. "Rapid enthalpy probe." Acta Physica Sinica 56, no. 10 (2007): 5952. http://dx.doi.org/10.7498/aps.56.5952.

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12

Nilsson, Tor, and Hans Niedderer. "Undergraduate students' conceptions of enthalpy, enthalpy change and related concepts." Chem. Educ. Res. Pract. 15, no. 3 (2014): 336–53. http://dx.doi.org/10.1039/c2rp20135f.

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13

Wormald, C. J., and T. K. Yerlett. "A new enthalpy-increment calorimeter enthalpy increments for n-hexane." Journal of Chemical Thermodynamics 17, no. 12 (1985): 1171–86. http://dx.doi.org/10.1016/0021-9614(85)90044-8.

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14

Michael, Ioelovich. "Application of thermochemical methods for the study of cellulose and cellulose esters." World Journal of Advanced Research and Reviews 18, no. 3 (2023): 1477–88. https://doi.org/10.5281/zenodo.8435885.

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In this research, the enthalpy of the interaction of cellulose and cellulose esters with various polar liquids was studied. Besides, the standard enthalpies of combustion and formation of cellulose and its esters were determined. It was shown that the absolute value of the standard exothermic enthalpy of the interaction of cellulose with the polar liquids is an indicator of the accessibility of the supramolecular structure for these liquids. It has been also established that the interaction enthalpy of cellulose materials with water, i.e., wetting enthalpy, is directly proportional to the cont
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15

Duan, L., and M. P. Martín. "Direct numerical simulation of hypersonic turbulent boundary layers. Part 4. Effect of high enthalpy." Journal of Fluid Mechanics 684 (September 6, 2011): 25–59. http://dx.doi.org/10.1017/jfm.2011.252.

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AbstractIn this paper we present direct numerical simulations (DNS) of hypersonic turbulent boundary layers to study high-enthalpy effects. We study high- and low-enthalpy conditions, which are representative of those in hypersonic flight and ground-based facilities, respectively. We find that high-enthalpy boundary layers closely resemble those at low enthalpy. Many of the scaling relations for low-enthalpy flows, such as van-Driest transformation for the mean velocity, Morkovin’s scaling and the modified strong Reynolds analogy hold or can be generalized for high-enthalpy flows by removing t
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16

Liu, Xiaochen, Xiaohua Liu, Tao Zhang, and Ying Xie. "Experimental analysis and performance optimization of a counter-flow enthalpy recovery device using liquid desiccant." Building Services Engineering Research and Technology 39, no. 6 (2018): 679–97. http://dx.doi.org/10.1177/0143624418780852.

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The liquid desiccant enthalpy recovery is an efficient way to save energy in air-conditioning systems. In this study, a counter-flow liquid desiccant enthalpy recovery device was proposed and experimentally analyzed. Enthalpy transfer capacity, enthalpy efficiency and pressure drop per height of packing were used as indices to describe its performances. Based on the experiment results, the heat and mass transfer model of a packed tower was used to simulate and optimize the performance of this device. The maximum enthalpy efficiency and enthalpy transfer capacity were achieved when the optimal
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17

Mazeina, Lena, Suraj Deore та Alexandra Navrotsky. "Energetics of Bulk and Nano-Akaganeite, β-FeOOH: Enthalpy of Formation, Surface Enthalpy, and Enthalpy of Water Adsorption". Chemistry of Materials 18, № 7 (2006): 1830–38. http://dx.doi.org/10.1021/cm052543j.

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18

Runjun, Huang, Huang Zengwei, Song Baoling, Liao Sen, Wei Dongping, and Yuan Aiqun. "Standard Molar Formation Enthalpy of NH4Zn2PO4HPO4and Its Standard Molar Formation Enthalpy." Integrated Ferroelectrics 162, no. 1 (2015): 46–54. http://dx.doi.org/10.1080/10584587.2015.1038133.

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19

Elbaev, E. R., N. I. Matskevich, S. A. Luk’yanova, V. P. Zaitsev, and E. N. Tkachev. "Enthalpy of Formation and Lattice Enthalpy of Erbium-Substituted Bismuth Oxide." Russian Journal of Physical Chemistry A 98, no. 9 (2024): 1941–44. http://dx.doi.org/10.1134/s003602442470105x.

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20

Papina, T. S., V. P. Kolesov, V. A. Lukyanova, O. V. Boltalina, A. Yu Lukonin, and L. N. Sidorov. "Enthalpy of Formation and C−F Bond Enthalpy of Fluorofullerene C60F36." Journal of Physical Chemistry B 104, no. 23 (2000): 5403–5. http://dx.doi.org/10.1021/jp000409a.

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21

Majzlan, Juraj, Lena Mazeina та Alexandra Navrotsky. "Enthalpy of water adsorption and surface enthalpy of lepidocrocite (γ-FeOOH)". Geochimica et Cosmochimica Acta 71, № 3 (2007): 615–23. http://dx.doi.org/10.1016/j.gca.2006.10.010.

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22

Pinto, Isabel, Helena Cardoso, Cecélia Leão, and N. van Uden. "High enthalpy and low enthalpy death inSaccharomyces cerevisiaeinduced by acetic acid." Biotechnology and Bioengineering 33, no. 10 (1989): 1350–52. http://dx.doi.org/10.1002/bit.260331019.

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23

Zhang, Yi, Dong Ming Guo, and Da Liu. "Utilization and Research on Medium-Enthalpy and Low-Enthalpy Geothermal Energy in WSHP System." Advanced Materials Research 374-377 (October 2011): 392–97. http://dx.doi.org/10.4028/www.scientific.net/amr.374-377.392.

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Geothermal energy is a stable energy, stored underground and not influenced by the geographical, seasonal weather and the change of day and night. Medium-enthalpy and low-enthalpy geothermal energy are distributed in many areas of China, having a broad prospect for development. Taking water resources heat pump (WSHP) engineering in Tianqiao District as an example, medium-enthalpy and low-enthalpy geothermal energy is combined with the technology of aquifer thermal energy storage (ATES), providing cold energy in summer and warm energy in winter for the buildings. On the base of analysis of hydr
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24

Murthy, Varun S., and William R. Boos. "Role of Surface Enthalpy Fluxes in Idealized Simulations of Tropical Depression Spinup." Journal of the Atmospheric Sciences 75, no. 6 (2018): 1811–31. http://dx.doi.org/10.1175/jas-d-17-0119.1.

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AbstractAn idealized, three-dimensional, cloud-system-resolving model is used to investigate the influence of surface enthalpy flux variations on tropical depression (TD) spinup, an early stage of tropical cyclogenesis in which the role of surface fluxes remains incompletely understood. A range of simulations supports the hypothesis that a negative radial gradient of surface enthalpy flux outside the storm center is necessary for TD spinup but can arise from multiple mechanisms. The negative radial gradient is typically created by the wind speed dependence of surface enthalpy fluxes, consisten
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25

Hong, Beichuan, Varun Venkataraman, and Andreas Cronhjort. "Numerical Analysis of Engine Exhaust Flow Parameters for Resolving Pre-Turbine Pulsating Flow Enthalpy and Exergy." Energies 14, no. 19 (2021): 6183. http://dx.doi.org/10.3390/en14196183.

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Energy carried by engine exhaust pulses is critical to the performance of a turbine or any other exhaust energy recovery system. Enthalpy and exergy are commonly used concepts to describe the energy transport by the flow based on the first and second laws of thermodynamics. However, in order to investigate the crank-angle-resolved exhaust flow enthalpy and exergy, the significance of the flow parameters (pressure, velocity, and temperature) and their demand for high resolution need to be ascertained. In this study, local and global sensitivity analyses were performed on a one-dimensional (1D)
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26

Gurov, A. A., S. V. Kozhevnikova, A. N. Ozhogina, and S. N. Solovyev. "Nickel Sulfate Aqueous Solutions Thermal Chemistry and Enthalpy of Ni2+ Cation Formation at the Temperature 298.15 K." Herald of the Bauman Moscow State Technical University. Series Natural Sciences, no. 1 (88) (February 2020): 93–99. http://dx.doi.org/10.18698/1812-3368-2020-1-93-99.

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Calorimeter with an isothermal shell was used at a temperature of 298.15 K to measure the following parameters: enthalpy of NiSO4(k) dissolution in water followed by generation of two molar concentration solutions; enthalpy of four NiSO4 aqueous solutions dilution having various molar concentrations followed by generation of solutions with approximately the same concentration values. Based on the data obtained, enthalpy and ion association constant in the NiSO4 aqueous solution, as well as standard enthalpy of the aqueous solution formation, were determined for the indicated compound. The latt
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27

Suraya Md Nasrudin, Farah, and Shafaruniza Mahadi. "Enthalpy method for one dimensional heat conduction." International Journal of Engineering & Technology 7, no. 2.14 (2018): 9. http://dx.doi.org/10.14419/ijet.v7i2.14.11143.

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In this paper, the Enthalpy Method is employed to compute an approximate solution of the system of nonlinear differential equations focusing on the simulation of moving boundary for one dimensional heat conduction. This paper is only considered in the problem of a technical grade paraffin’s melting process. In order to seek the solution in term of temperature distribution, Finite Difference Method will be used. The results obtained are compared between solving with enthalpy and without enthalpy. The enthalpy method is more versatile, convenient, adaptable and easily programmable.
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28

Tsvetkov, D. S., D. A. Malyshkin, M. O. Mazurin, V. V. Sereda, and A. Yu Zuev. "Mixing Enthalpy Estimation for CsX–PbX2 Melts (X = Cl, Br) by Differential Scanning Calorimetry." Russian Journal of Physical Chemistry A 98, no. 12 (2024): 2675–80. http://dx.doi.org/10.1134/s0036024424701887.

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Abstract A comparatively simple method for estimating the mixing enthalpy of melts by differential scanning calorimetry using standard equipment is proposed. The enthalpies of mixing of CsX–PbX2 (X = Cl, Br) melts are determined by this method. The measured values of mixing enthalpy in the CsCl–PbCl2 system are in good agreement with those obtained by means of independent measurements. For the CsBr–PbBr2 system, the enthalpy of mixing was measured for the first time. The similar values of mixing enthalpy were found for both studied systems.
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29

Majzlan, Juraj. "Surface Enthalpy of Boehmite." Clays and Clay Minerals 48, no. 6 (2000): 699–707. http://dx.doi.org/10.1346/ccmn.2000.0480611.

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30

Mulero, A., and I. Cachadiña. "Boiling enthalpy from correlations." Thermochimica Acta 443, no. 1 (2006): 37–48. http://dx.doi.org/10.1016/j.tca.2005.12.018.

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31

Head-Gordon, Teresa, and Frank H. Stillinger. "Enthalpy of knotted polypeptides." Journal of Physical Chemistry 96, no. 19 (1992): 7792–96. http://dx.doi.org/10.1021/j100198a054.

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32

Van Ness, Hendrick C. "H Is for Enthalpy." Journal of Chemical Education 80, no. 5 (2003): 486. http://dx.doi.org/10.1021/ed080p486.1.

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33

Vine, M. D., and C. J. Wormald. "The enthalpy of benzene." Journal of Chemical Thermodynamics 23, no. 12 (1991): 1175–80. http://dx.doi.org/10.1016/s0021-9614(05)80151-x.

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34

Watson, Christopher B., Dustin Tan, and David E. Bergbreiter. "Enthalpy-Driven Polyisobutylene Depolymerization." Macromolecules 52, no. 8 (2019): 3042–48. http://dx.doi.org/10.1021/acs.macromol.9b00313.

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35

Yerlett, T. K., and C. J. Wormald. "The enthalpy of acetone." Journal of Chemical Thermodynamics 18, no. 4 (1986): 371–79. http://dx.doi.org/10.1016/0021-9614(86)90083-2.

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36

Yerlett, T. K., and C. J. Wormald. "The enthalpy of methanol." Journal of Chemical Thermodynamics 18, no. 8 (1986): 719–26. http://dx.doi.org/10.1016/0021-9614(86)90105-9.

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37

Vine, M. D., and C. J. Wormald. "The enthalpy of ethanol." Journal of Chemical Thermodynamics 21, no. 11 (1989): 1151–57. http://dx.doi.org/10.1016/0021-9614(89)90101-8.

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38

Ivanova, N., and S. Chaichenets. "COMMON ENVELOPE: ENTHALPY CONSIDERATION." Astrophysical Journal 731, no. 2 (2011): L36. http://dx.doi.org/10.1088/2041-8205/731/2/l36.

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39

Mazeina, Lena, and Alexandra Navrotsky. "Surface enthalpy of goethite." clays and clay minerals 53, no. 2 (2005): 113–22. http://dx.doi.org/10.1346/ccmn.2005.0530201.

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40

Wiegand, Fred J. "ENTHALPY OF SUPERHEATED STEAM." Journal of the American Society for Naval Engineers 51, no. 1 (2009): 99–100. http://dx.doi.org/10.1111/j.1559-3584.1939.tb01455.x.

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41

Murdock., James W. "ENTHALPY OF SUPERHEATED STEAM." Journal of the American Society for Naval Engineers 54, no. 3 (2009): 370–71. http://dx.doi.org/10.1111/j.1559-3584.1942.tb02103.x.

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42

SWAMINATHAN, C. R., and V. R. VOLLER. "ON THE ENTHALPY METHOD." International Journal of Numerical Methods for Heat & Fluid Flow 3, no. 3 (1993): 233–44. http://dx.doi.org/10.1108/eb017528.

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43

Poland, Douglas. "Enthalpy distributions in proteins." Biopolymers 58, no. 1 (2000): 89–105. http://dx.doi.org/10.1002/1097-0282(200101)58:1<89::aid-bip90>3.0.co;2-7.

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44

Ribeiro da Silva, Manuel A. V., Ana M. M. V. Reis, Manuel J. S. Monte, Madalena M. S. S. F. Bártolo, and João A. R. G. O. Rodrigues. "Enthalpy of combustion, vapour pressures, and enthalpy of sublimation of 3-nitrophenol." Journal of Chemical Thermodynamics 24, no. 6 (1992): 653–59. http://dx.doi.org/10.1016/s0021-9614(05)80037-0.

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45

Mazeina, Lena, Sergey V. Ushakov, Alexandra Navrotsky, and Lynn A. Boatner. "Formation enthalpy of ThSiO4 and enthalpy of the thorite → huttonite phase transition." Geochimica et Cosmochimica Acta 69, no. 19 (2005): 4675–83. http://dx.doi.org/10.1016/j.gca.2005.03.053.

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46

Pimenova, Svetlana M., Svetlana V. Melkhanova, Victor P. Kolesov, and Anatolii S. Lobach. "The Enthalpy of Formation and C−H Bond Enthalpy of Hydrofullerene C60H36." Journal of Physical Chemistry B 106, no. 9 (2002): 2127–30. http://dx.doi.org/10.1021/jp012258x.

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47

Cherifa, A. Ben, M. Jemal, A. Nounah, and J. L. Lacout. "Enthalpy of formation and enthalpy of mixing of calcium and cadmium hydroxyapatites." Thermochimica Acta 237, no. 2 (1994): 285–93. http://dx.doi.org/10.1016/0040-6031(94)80186-x.

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48

Benn, D. I., A. C. Fowler, I. Hewitt, and H. Sevestre. "A general theory of glacier surges." Journal of Glaciology 65, no. 253 (2019): 701–16. http://dx.doi.org/10.1017/jog.2019.62.

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AbstractWe present the first general theory of glacier surging that includes both temperate and polythermal glacier surges, based on coupled mass and enthalpy budgets. Enthalpy (in the form of thermal energy and water) is gained at the glacier bed from geothermal heating plus frictional heating (expenditure of potential energy) as a consequence of ice flow. Enthalpy losses occur by conduction and loss of meltwater from the system. Because enthalpy directly impacts flow speeds, mass and enthalpy budgets must simultaneously balance if a glacier is to maintain a steady flow. If not, glaciers unde
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49

Michael Ioelovich. "Application of thermochemical methods for the study of cellulose and cellulose esters." World Journal of Advanced Research and Reviews 18, no. 3 (2023): 1477–88. http://dx.doi.org/10.30574/wjarr.2023.18.3.1260.

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In this research, the enthalpy of the interaction of cellulose and cellulose esters with various polar liquids was studied. Besides, the standard enthalpies of combustion and formation of cellulose and its esters were determined. It was shown that the absolute value of the standard exothermic enthalpy of the interaction of cellulose with the polar liquids is an indicator of the accessibility of the supramolecular structure for these liquids. It has been also established that the interaction enthalpy of cellulose materials with water, i.e., wetting enthalpy, is directly proportional to the cont
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50

Jeong, Dahai, Brian K. Haus, and Mark A. Donelan. "Enthalpy Transfer across the Air–Water Interface in High Winds Including Spray." Journal of the Atmospheric Sciences 69, no. 9 (2012): 2733–48. http://dx.doi.org/10.1175/jas-d-11-0260.1.

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Abstract Controlled experiments were conducted in the Air–Sea Interaction Saltwater Tank (ASIST) at the University of Miami to investigate air–sea moist enthalpy transfer rates under various wind speeds (range of 0.6–39 m s−1 scaled to equivalent 10-m neutral winds) and water–air temperature differences (range of 1.3°–9.2°C). An indirect calorimetric (heat content budget) measurement technique yielded accurate determinations of moist enthalpy flux over the full range of wind speeds. These winds included conditions with significant spray generation, the concentrations of which were of the same
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