D. Godhani, Anwar Saiyad, U. Mehta, Kuldip Parmar, J. Mehta
{"title":"基于吡啶的 1,3,4-恶二唑支架的热力学性质","authors":"D. Godhani, Anwar Saiyad, U. Mehta, Kuldip Parmar, J. Mehta","doi":"10.2174/0118779468275261231117053704","DOIUrl":null,"url":null,"abstract":"\n\nThe present work describes the synthesis, characterization, and\nthermo-acoustical parameters of binary solutions of 1-(2-(4-fluorophenyl)-5-(pyridin-4-\nyl)-1,3,4-oxadiazol-3(2H)-yl)-3-(pyridin-2-yl)prop-2-en-1-one, (AS1-08) and 1-(2-(4-\nmethoxyphenyl)-5-(pyridin-4-yl)-1,3,4-oxadiazol-3(2H)-yl)-3-(pyridin-2-yl)prop-2-en-1-\none, (AS1-12) in dimethyl sulfoxide (DMSO) and N, N-dimethylformamide (DMF) were\nestimated.\n\n\n\nViscosity, ultrasonic velocity, and density methods at different solvents (DMSO\nand DMF) and different temperatures (298.15, 308.15, and 318.15 K) were used during the\nexperimental research work.\n\n\n\nSome acoustic parameters such as adiabatic compressibility (κs), intermolecular\nfree path length (Lf), Rao’s molar sound function (Rm), Van der Waals constant (b), internal\npressure (π), free volume (Vf) and solvation number (Sn) were calculated. The results obtained were interpreted in terms of solute-solvent and solute-solute interactions.\n\n\n\nThe thermodynamic and various acoustical properties were determined at\nthree different temperatures viz. (298.15, 308.15, and 318.15 K) at atmospheric pressure.\nLikewise, the similarity between experimental results of the binary solutions was studied to\nanalyze how the change in the structural modification and solvent changes the values of\nGibbs energy of activation (ΔG*), enthalpy of activation (ΔH*), and entropy of activation\n(ΔS*).\n","PeriodicalId":89671,"journal":{"name":"Current physical chemistry","volume":"8 3","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-12-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Thermodynamic Properties of Pyridine Based 1,3,4-Oxadiazole\\nScaffolds\",\"authors\":\"D. Godhani, Anwar Saiyad, U. Mehta, Kuldip Parmar, J. Mehta\",\"doi\":\"10.2174/0118779468275261231117053704\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"\\n\\nThe present work describes the synthesis, characterization, and\\nthermo-acoustical parameters of binary solutions of 1-(2-(4-fluorophenyl)-5-(pyridin-4-\\nyl)-1,3,4-oxadiazol-3(2H)-yl)-3-(pyridin-2-yl)prop-2-en-1-one, (AS1-08) and 1-(2-(4-\\nmethoxyphenyl)-5-(pyridin-4-yl)-1,3,4-oxadiazol-3(2H)-yl)-3-(pyridin-2-yl)prop-2-en-1-\\none, (AS1-12) in dimethyl sulfoxide (DMSO) and N, N-dimethylformamide (DMF) were\\nestimated.\\n\\n\\n\\nViscosity, ultrasonic velocity, and density methods at different solvents (DMSO\\nand DMF) and different temperatures (298.15, 308.15, and 318.15 K) were used during the\\nexperimental research work.\\n\\n\\n\\nSome acoustic parameters such as adiabatic compressibility (κs), intermolecular\\nfree path length (Lf), Rao’s molar sound function (Rm), Van der Waals constant (b), internal\\npressure (π), free volume (Vf) and solvation number (Sn) were calculated. The results obtained were interpreted in terms of solute-solvent and solute-solute interactions.\\n\\n\\n\\nThe thermodynamic and various acoustical properties were determined at\\nthree different temperatures viz. (298.15, 308.15, and 318.15 K) at atmospheric pressure.\\nLikewise, the similarity between experimental results of the binary solutions was studied to\\nanalyze how the change in the structural modification and solvent changes the values of\\nGibbs energy of activation (ΔG*), enthalpy of activation (ΔH*), and entropy of activation\\n(ΔS*).\\n\",\"PeriodicalId\":89671,\"journal\":{\"name\":\"Current physical chemistry\",\"volume\":\"8 3\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-12-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Current physical chemistry\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.2174/0118779468275261231117053704\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Current physical chemistry","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2174/0118779468275261231117053704","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Thermodynamic Properties of Pyridine Based 1,3,4-Oxadiazole
Scaffolds
The present work describes the synthesis, characterization, and
thermo-acoustical parameters of binary solutions of 1-(2-(4-fluorophenyl)-5-(pyridin-4-
yl)-1,3,4-oxadiazol-3(2H)-yl)-3-(pyridin-2-yl)prop-2-en-1-one, (AS1-08) and 1-(2-(4-
methoxyphenyl)-5-(pyridin-4-yl)-1,3,4-oxadiazol-3(2H)-yl)-3-(pyridin-2-yl)prop-2-en-1-
one, (AS1-12) in dimethyl sulfoxide (DMSO) and N, N-dimethylformamide (DMF) were
estimated.
Viscosity, ultrasonic velocity, and density methods at different solvents (DMSO
and DMF) and different temperatures (298.15, 308.15, and 318.15 K) were used during the
experimental research work.
Some acoustic parameters such as adiabatic compressibility (κs), intermolecular
free path length (Lf), Rao’s molar sound function (Rm), Van der Waals constant (b), internal
pressure (π), free volume (Vf) and solvation number (Sn) were calculated. The results obtained were interpreted in terms of solute-solvent and solute-solute interactions.
The thermodynamic and various acoustical properties were determined at
three different temperatures viz. (298.15, 308.15, and 318.15 K) at atmospheric pressure.
Likewise, the similarity between experimental results of the binary solutions was studied to
analyze how the change in the structural modification and solvent changes the values of
Gibbs energy of activation (ΔG*), enthalpy of activation (ΔH*), and entropy of activation
(ΔS*).