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Raoult's law

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3083: 2481: 723: 736:, which is a limiting law valid when the interactive forces between molecules approach zero, for example as the concentration approaches zero. Raoult's law is instead valid if the physical properties of the components are identical. The more similar the components are, the more their behavior approaches that described by Raoult's law. For example, if the two components differ only in 1071: 2284:. This equation shows that, for an ideal solution where each pure component has a different vapor pressure, the gas phase is enriched in the component with the higher vapor pressure when pure, and the solution is enriched in the component with the lower pure vapor pressure. This phenomenon is the basis for 2296:
In elementary applications, Raoult's law is generally valid when the liquid phase is either nearly pure or a mixture of similar substances. Raoult's law may be adapted to non-ideal solutions by incorporating two factors that account for the interactions between molecules of different substances. The
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Raoult's law is a phenomenological relation that assumes ideal behavior based on the simple microscopic assumption that intermolecular forces between unlike molecules are equal to those between similar molecules, and that their molar volumes are the same: the conditions of an ideal solution. This is
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An ideal solution would follow Raoult's law, but most solutions deviate from ideality. Interactions between gas molecules are typically quite small, especially if the vapor pressures are low. However, the interactions in a liquid are very strong. For a solution to be ideal, the interactions between
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The presence of these limited linear regimes has been experimentally verified in a great number of cases, though large deviations occur in a variety of cases. Consequently, both its pedagogical value and utility have been questioned at the introductory college level. In a perfectly ideal system,
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to postulate that the vapor pressure above an ideal mixture of liquids is equal to the sum of the vapor pressures of each component multiplied by its mole fraction. Taking compliance with Raoult's Law as a defining characteristic of ideality in a solution, it is possible to
1509: 1709: 534:) is dissolved into a solvent A to form an ideal solution, the vapor pressure of the solution will be lower than that of the solvent. In an ideal solution of a nonvolatile solute, the decrease in vapor pressure is directly proportional to the mole fraction of solute: 705: 915: 398: 2528:, corresponding to a mixture that evaporates without change of composition. When these two components are mixed, the reaction is exothermic as ion-dipole intermolecular forces of attraction are formed between the resulting ions (H 904: 1282:
in the ideal solution. From this equation, other thermodynamic properties of an ideal solution may be determined. If the assumption that the vapor follows the ideal gas law is added, Raoult's law may be derived as follows.
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Vapor pressure of a binary solution that obeys Raoult's law. The black line shows the total vapor pressure as a function of the mole fraction of component B, and the two green lines are the partial pressures of the two
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unlike molecules must be of the same magnitude as those between like molecules. This approximation is only true when the different species are almost chemically identical. One can see that from considering the
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If the deviation is large, then the vapor pressure curve shows a maximum at a particular composition and forms a positive azeotrope (low-boiling mixture). Some mixtures in which this happens are (1)
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Where two volatile liquids A and B are mixed with each other to form a solution, the vapor phase consists of both components of the solution. Once the components in the solution have reached
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When the adhesion is weaker than cohesion, which is quite common, the liquid particles escape the solution more easily that increases the vapor pressure and leads to a positive deviation.
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When the adhesion is stronger than the cohesion, fewer liquid particles turn into vapor thereby lowering the vapor pressure and leading to negative deviation in the graph.
1570: 1101: 822: 795: 2366: 2336: 1066:{\displaystyle p=p_{\text{A}}^{\star }(1-x_{\text{B}})+p_{\text{B}}^{\star }x_{\text{B}}=p_{\text{A}}^{\star }+(p_{\text{B}}^{\star }-p_{\text{A}}^{\star })x_{\text{B}}.} 2096: 2274: 2219: 2067: 1543: 1260: 318: 279: 172: 1989: 2477:
forces (between similar molecules) are not uniform between the two liquids. Therefore, they deviate from Raoult's law, which applies only to ideal solutions.
2243: 1593: 1308: 1280: 768: 299: 252: 196: 830: 3540: 2914:"Solute-Solvent Complex Switching Dynamics of Chloroform between Acetone and Dimethylsulfoxide Two-Dimensional IR Chemical Exchange Spectroscopy" 1862: 2520:) has a negative deviation from Raoult's law, indicating an attractive interaction between the two components that have been described as a 2120: 3242: 520:{\displaystyle p={\dfrac {p_{\text{A}}^{\star }n_{\text{A}}+p_{\text{B}}^{\star }n_{\text{B}}+\cdots }{n_{\text{A}}+n_{\text{B}}+\cdots }}} 2582:
and water. When these pairs of components are mixed, the process is endothermic as weaker intermolecular interactions are formed so that Δ
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Comparing measured vapor pressures to predicted values from Raoult's law provides information about the true relative strength of
2524:. The system HCl–water has a large enough negative deviation to form a minimum in the vapor pressure curve known as a (negative) 1504:{\displaystyle \mu _{i,{\text{liq}}}^{\star }+RT\ln x_{i}=\mu _{i,{\text{vap}}}^{\ominus }+RT\ln {\frac {f_{i}}{p^{\ominus }}},} 3014: 750:
For a solution of two liquids A and B, Raoult's law predicts that if no other gases are present, then the total vapor pressure
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If deviations from the ideal are not too large, Raoult's law is still valid in a narrow concentration range when approaching
1704:{\displaystyle \mu _{i,{\text{liq}}}^{\star }=\mu _{i,{\text{vap}}}^{\ominus }+RT\ln {\frac {f_{i}^{\star }}{p^{\ominus }}}.} 1130: 540: 3621: 700:{\displaystyle \Delta p=p_{\text{A}}^{\star }-p=p_{\text{A}}^{\star }(1-x_{\text{A}})=p_{\text{A}}^{\star }x_{\text{B}}.} 3606: 2859: 3082: 3287: 2884: 2763: 2725: 3235: 403:
In other words, the vapor pressure of the solution is the mole-weighted mean of the individual vapour pressures:
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where ideal liquid and ideal vapor are assumed, a very useful equation emerges if Raoult's law is combined with
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Positive and negative deviations from Raoult's law. Maxima and minima in the curves (if present) correspond to
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must be equal to zero, and this can only be true if the interactions between the molecules are indifferent.
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in the mixture. In consequence, the relative lowering of vapor pressure of a dilute solution of nonvolatile
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This is always negative, so mixing is spontaneous. However, the expression is, apart from a factor
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If the solute associates or dissociates in the solution, the expression of the law includes the
3445: 3440: 3297: 3169: 2925: 2657: 2747: 393:{\displaystyle p=p_{\text{A}}^{\star }x_{\text{A}}+p_{\text{B}}^{\star }x_{\text{B}}+\cdots .} 3601: 3545: 3525: 3194: 3000: 744: 711: 2075: 308:, the total vapor pressure of the solution can be determined by combining Raoult's law with 3259: 3251: 3107: 2912:
Kwak, Kyungwon; Rosenfeld, Daniel E.; Chung, Jean K.; Fayer, Michael D. (6 November 2008).
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is equal to the vapor pressure of the pure component (liquid or solid) multiplied by its
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of the two components. Thus the total pressure above the solution of A and B would be
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Mathematically, Raoult's law for a single component in an ideal solution is stated as
52: 899:{\displaystyle p=p_{\text{A}}^{\star }x_{\text{A}}+p_{\text{B}}^{\star }x_{\text{B}}.} 3550: 3509: 3412: 3138: 3062: 2953: 2880: 2855: 2783: 2759: 2721: 2704: 2836: 3485: 3480: 3312: 3272: 3179: 3067: 2943: 2935: 2822: 2700: 2599: 2567: 175: 64: 25: 2624: 3455: 3387: 3352: 3337: 3332: 3317: 3282: 3052: 3042: 2480: 2469:
In many pairs of liquids, there is no uniformity of attractive forces, i.e., the
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in a binary solution then, for the second component, the same must also hold.
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above the solution is equal to the weighted sum of the "pure" vapor pressures
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first factor is a correction for gas non-ideality, or deviations from the
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For the ideal gas, pressure and fugacity are equal, so introducing simple
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Felder, Richard M.; Rousseau, Ronald W.; Bullard, Lisa G. (2004-12-15).
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The corresponding equation when the system consists purely of component
3570: 3560: 3555: 3432: 2687:"Recherches expérimentales sur les tensions de vapeur des dissolutions" 2629: 2575: 2501: 2939: 2827: 2801: 2184:{\displaystyle x_{i}={\frac {y_{i}p_{\text{total}}}{p_{i}^{\star }}},} 3580: 3535: 3450: 3220: 3133: 2755: 2689:[Experimental research on the vapor pressures of solutions]. 2609: 2525: 2485: 531: 530:
If a non-volatile solute B (it has zero vapor pressure, so does not
3397: 2563: 2470: 1779: 1515: 3500: 3302: 3292: 3128: 2579: 2571: 2559: 2551: 2509: 2454:{\displaystyle y_{i}\phi _{p,i}p=x_{i}\gamma _{i}p_{i}^{\star }.} 1714:
Subtracting these equations and re-arranging leads to the result
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that if Raoult's law holds over the entire concentration range
80: 3322: 3148: 2555: 37: 34: 1365:{\displaystyle \mu _{i,{\text{liq}}}=\mu _{i,{\text{vap}}}.} 2371:
This modified or extended Raoult's law is then written as
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is equal to the mole fraction of solute in the solution.
2879:(seventh ed.), New York: McGraw-Hill, p. 545, 1545:, as a fraction of the pressure in the reference state, 1310:
must be the same in the liquid and gas states. That is,
2911: 2748:"Thermodynamics of Fluid Phase and Chemical Equilibria" 1193:{\displaystyle \mu _{i}=\mu _{i}^{\star }+RT\ln x_{i},} 2660:[General law of vapor pressures of solvents]. 1375:
Substituting the formula for chemical potential gives
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Since the sum of the mole fractions is equal to one,
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Law of thermodynamics for vapour pressure of a mixture
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Smith, J. M.; Van Ness, H. C.; Abbott, M. M. (2005),
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List of boiling and freezing information of solvents
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Raoult's law was first observed empirically and led
581:{\displaystyle p=p_{\text{A}}^{\star }x_{\text{A}},} 40: 31: 2877:
Introduction to Chemical Engineering Thermodynamics
2874: 28: 2742: 2453: 2360: 2330: 2268: 2237: 2213: 2183: 2090: 2061: 2013: 1983: 1957: 1835: 1767: 1703: 1587: 1564: 1537: 1503: 1364: 1302: 1274: 1254: 1227: 1192: 1095: 1065: 898: 816: 789: 762: 699: 580: 519: 392: 293: 273: 246: 222: 190: 166: 136: 2746:; Corti, David S.; Mallinson, Richard G. (2008). 2532:O and Cl) and the polar water molecules so that Δ 740:content, then Raoult's law is essentially exact. 3593: 1235:is the chemical potential in the pure state and 2902:(8th ed., W. H. Freeman 2006) p. 146. 1106: 1076:This is a linear function of the mole fraction 1514:as the gas-phase mole fraction depends on its 3236: 3008: 2677: 2675: 2648: 2646: 1124:of each component of the liquid is given by 2852:Elementary Principles of Chemical Processes 1290:, the chemical potential of each component 198:in the gaseous mixture above the solution, 3243: 3229: 3015: 3001: 2793: 2692:Journal de Physique ThĂ©orique et AppliquĂ©e 1836:{\displaystyle p_{i}=x_{i}p_{i}^{\star }.} 1768:{\displaystyle f_{i}=x_{i}f_{i}^{\star }.} 2978:Chapter 24, D. A. McQuarrie, J. D. Simon 2947: 2929: 2868: 2826: 2738: 2736: 2734: 2672: 2643: 137:{\displaystyle p_{i}=p_{i}^{\star }x_{i}} 2980:Physical Chemistry: A Molecular Approach 2752:Albright's Chemical Engineering Handbook 2479: 721: 3594: 3250: 2799: 2731: 2681: 2652: 281:is the mole fraction of the component 3224: 2996: 2542: 2492: 2014:{\displaystyle \Delta _{\text{mix}}H} 1782:to this result yields Raoult's law: 2473:(between dissimilar molecules) and 2291: 13: 2982:. University Science Books. (1997) 1999: 1867: 1854:Gibbs free energy change of mixing 1262:is the mole fraction of component 596: 14: 3638: 2970:Atkins and de Paula, p. 184. 2464: 1595:in equilibrium with its vapor is 1286:If the system is ideal, then, at 1228:{\displaystyle \mu _{i}^{\star }} 301:in the liquid or solid solution. 3081: 3022: 2989:. Clarendon Press. Oxford (1993) 24: 2964: 2905: 2782:(MacMillan 1969), p. 261. 1846: 2892: 2843: 2772: 2750:. In Albright, Lyle F. (ed.). 2711: 2705:10.1051/jphystap:0188900800500 2082: 2056: 2041: 1949: 1891: 1047: 1011: 959: 940: 663: 644: 223:{\displaystyle p_{i}^{\star }} 1: 2987:Basic Chemical Thermodynamics 2802:"Raoult's Law Is a Deception" 2636: 2488:or constant boiling mixtures. 717: 312:of partial pressures to give 59:. Proposed by French chemist 3531:Inorganic nonaqueous solvent 2098:for the majority phase (the 1565:{\displaystyle p^{\ominus }} 1107:Thermodynamic considerations 1096:{\displaystyle x_{\text{B}}} 817:{\displaystyle p_{\text{B}}} 790:{\displaystyle p_{\text{A}}} 63:in 1887, it states that the 7: 2898:P. Atkins and J. de Paula, 2800:Hawkes, Stephen J. (1995). 2592: 2500:For example, the system of 2361:{\displaystyle \gamma _{i}} 2331:{\displaystyle \phi _{p,i}} 10: 3643: 3622:Engineering thermodynamics 3516:Acid dissociation constant 3144:Spinning band distillation 2024:It can be shown using the 232:equilibrium vapor pressure 3607:Eponymous laws of physics 3499: 3431: 3361: 3258: 3157: 3121: 3090: 3079: 3030: 1103:, as shown in the graph. 3073:Vapor–liquid equilibrium 2718:A to Z of Thermodynamics 714:as a correction factor. 67:of each component of an 3481:Solubility table (data) 3348:Apparent molar property 3103:Continuous distillation 2780:Chemical Thermodynamics 55:, with implications in 3446:Total dissolved solids 3441:Solubility equilibrium 3366:and related quantities 2854:. Wiley. p. 293. 2489: 2455: 2362: 2332: 2270: 2239: 2215: 2185: 2092: 2091:{\displaystyle x\to 1} 2063: 2015: 1985: 1959: 1837: 1769: 1705: 1589: 1566: 1539: 1505: 1366: 1304: 1276: 1256: 1229: 1194: 1097: 1067: 900: 818: 791: 764: 728: 701: 582: 521: 394: 295: 275: 248: 234:of the pure component 224: 192: 168: 138: 51:law) is a relation of 3617:Equilibrium chemistry 3546:Partition coefficient 3526:Polar aprotic solvent 2578:and ethanol, and (5) 2483: 2456: 2363: 2333: 2271: 2269:{\displaystyle y_{i}} 2240: 2216: 2214:{\displaystyle x_{i}} 2186: 2093: 2064: 2062:{\displaystyle x\in } 2016: 1986: 1960: 1838: 1770: 1706: 1590: 1567: 1540: 1538:{\displaystyle f_{i}} 1506: 1367: 1305: 1277: 1257: 1255:{\displaystyle x_{i}} 1230: 1195: 1113:François-Marie Raoult 1098: 1068: 901: 819: 792: 765: 745:intermolecular forces 725: 702: 583: 522: 395: 296: 276: 274:{\displaystyle x_{i}} 249: 225: 193: 169: 167:{\displaystyle p_{i}} 139: 61:François-Marie Raoult 3461:Enthalpy of solution 3388:Volume concentration 3383:Number concentration 3108:Fractionating column 3091:Industrial processes 3058:McCabe–Thiele method 2758:. pp. 255–392. 2378: 2345: 2340:activity coefficient 2309: 2303:fugacity coefficient 2253: 2229: 2198: 2121: 2076: 2032: 2026:Gibbs–Duhem equation 1995: 1972: 1863: 1789: 1721: 1602: 1579: 1549: 1522: 1382: 1317: 1294: 1266: 1239: 1207: 1131: 1080: 916: 831: 801: 774: 754: 593: 541: 410: 319: 285: 258: 238: 202: 182: 151: 93: 3373:Molar concentration 3343:Dilution (equation) 2924:(44): 13906–13915. 2819:1995JChEd..72..204H 2447: 2338:). The second, the 2301:. It is called the 2175: 1829: 1761: 1685: 1653: 1627: 1458: 1407: 1224: 1161: 1046: 1028: 1007: 979: 939: 882: 854: 683: 643: 619: 564: 465: 437: 370: 342: 219: 123: 3612:Physical chemistry 3413:Isotopic abundance 3378:Mass concentration 3252:Chemical solutions 3122:Laboratory methods 3098:Batch distillation 2900:Physical Chemistry 2720:by Pierre Perrot. 2543:Positive deviation 2493:Negative deviation 2490: 2451: 2433: 2358: 2328: 2266: 2235: 2211: 2181: 2161: 2088: 2059: 2011: 1984:{\displaystyle -T} 1981: 1955: 1833: 1815: 1765: 1747: 1701: 1671: 1631: 1605: 1585: 1562: 1535: 1501: 1436: 1385: 1362: 1300: 1272: 1252: 1225: 1210: 1190: 1147: 1122:chemical potential 1093: 1063: 1032: 1014: 993: 965: 925: 896: 868: 840: 814: 787: 760: 729: 712:van 't Hoff factor 697: 669: 629: 605: 578: 550: 517: 515: 451: 423: 390: 356: 328: 291: 271: 244: 220: 205: 188: 164: 134: 109: 53:physical chemistry 3589: 3588: 3218: 3217: 3139:Rotary evaporator 3063:Theoretical plate 2940:10.1021/jp806035w 2828:10.1021/ed072p204 2238:{\displaystyle i} 2176: 2157: 2052: 2005: 1873: 1696: 1645: 1619: 1588:{\displaystyle i} 1496: 1450: 1399: 1355: 1334: 1303:{\displaystyle i} 1275:{\displaystyle i} 1090: 1057: 1039: 1021: 1000: 987: 972: 956: 932: 890: 875: 862: 847: 811: 784: 763:{\displaystyle p} 732:analogous to the 691: 676: 660: 636: 612: 572: 557: 514: 504: 491: 473: 458: 445: 430: 378: 363: 350: 335: 294:{\displaystyle i} 247:{\displaystyle i} 191:{\displaystyle i} 178:of the component 3634: 3486:Solubility chart 3313:Phase separation 3273:Aqueous solution 3245: 3238: 3231: 3222: 3221: 3085: 3068:Partial pressure 3017: 3010: 3003: 2994: 2993: 2971: 2968: 2962: 2961: 2951: 2933: 2918:J. Phys. Chem. B 2909: 2903: 2896: 2890: 2889: 2872: 2866: 2865: 2847: 2841: 2840: 2830: 2797: 2791: 2776: 2770: 2769: 2740: 2729: 2715: 2709: 2708: 2679: 2670: 2669: 2650: 2600:Antoine equation 2568:carbon disulfide 2460: 2458: 2457: 2452: 2446: 2441: 2432: 2431: 2422: 2421: 2406: 2405: 2390: 2389: 2367: 2365: 2364: 2359: 2357: 2356: 2337: 2335: 2334: 2329: 2327: 2326: 2292:Non-ideal mixing 2275: 2273: 2272: 2267: 2265: 2264: 2244: 2242: 2241: 2236: 2220: 2218: 2217: 2212: 2210: 2209: 2190: 2188: 2187: 2182: 2177: 2174: 2169: 2160: 2159: 2158: 2155: 2149: 2148: 2138: 2133: 2132: 2097: 2095: 2094: 2089: 2068: 2066: 2065: 2060: 2050: 2020: 2018: 2017: 2012: 2007: 2006: 2003: 1990: 1988: 1987: 1982: 1964: 1962: 1961: 1956: 1948: 1947: 1932: 1931: 1919: 1918: 1903: 1902: 1875: 1874: 1871: 1842: 1840: 1839: 1834: 1828: 1823: 1814: 1813: 1801: 1800: 1774: 1772: 1771: 1766: 1760: 1755: 1746: 1745: 1733: 1732: 1710: 1708: 1707: 1702: 1697: 1695: 1694: 1684: 1679: 1670: 1652: 1647: 1646: 1643: 1626: 1621: 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524: 523: 518: 516: 513: 506: 505: 502: 493: 492: 489: 482: 475: 474: 471: 464: 459: 456: 447: 446: 443: 436: 431: 428: 421: 399: 397: 396: 391: 380: 379: 376: 369: 364: 361: 352: 351: 348: 341: 336: 333: 300: 298: 297: 292: 280: 278: 277: 272: 270: 269: 253: 251: 250: 245: 229: 227: 226: 221: 218: 213: 197: 195: 194: 189: 176:partial pressure 173: 171: 170: 165: 163: 162: 143: 141: 140: 135: 133: 132: 122: 117: 105: 104: 65:partial pressure 50: 49: 46: 45: 42: 39: 36: 33: 30: 3642: 3641: 3637: 3636: 3635: 3633: 3632: 3631: 3592: 3591: 3590: 3585: 3495: 3456:Solvation shell 3427: 3365: 3357: 3353:Miscibility gap 3338:Serial dilution 3333:Supersaturation 3283:Buffer solution 3254: 3249: 3219: 3214: 3153: 3117: 3086: 3077: 3053:Fenske equation 3026: 3021: 2975: 2974: 2969: 2965: 2931:10.1.1.560.3553 2910: 2906: 2897: 2893: 2887: 2873: 2869: 2862: 2848: 2844: 2798: 2794: 2778:Rock, Peter A. 2777: 2773: 2766: 2744:Chao, Kwang-Chu 2741: 2732: 2716: 2712: 2680: 2673: 2651: 2644: 2639: 2634: 2595: 2585: 2545: 2538: 2531: 2519: 2515: 2507: 2495: 2467: 2442: 2437: 2427: 2423: 2417: 2413: 2395: 2391: 2385: 2381: 2379: 2376: 2375: 2352: 2348: 2346: 2343: 2342: 2316: 2312: 2310: 2307: 2306: 2294: 2260: 2256: 2254: 2251: 2250: 2230: 2227: 2226: 2205: 2201: 2199: 2196: 2195: 2170: 2165: 2154: 2150: 2144: 2140: 2139: 2137: 2128: 2124: 2122: 2119: 2118: 2077: 2074: 2073: 2033: 2030: 2029: 2002: 1998: 1996: 1993: 1992: 1973: 1970: 1969: 1943: 1939: 1927: 1923: 1914: 1910: 1898: 1894: 1870: 1866: 1864: 1861: 1860: 1849: 1824: 1819: 1809: 1805: 1796: 1792: 1790: 1787: 1786: 1756: 1751: 1741: 1737: 1728: 1724: 1722: 1719: 1718: 1690: 1686: 1680: 1675: 1669: 1648: 1642: 1635: 1622: 1616: 1609: 1603: 1600: 1599: 1580: 1577: 1576: 1556: 1552: 1550: 1547: 1546: 1529: 1525: 1523: 1520: 1519: 1490: 1486: 1480: 1476: 1474: 1453: 1447: 1440: 1427: 1423: 1402: 1396: 1389: 1383: 1380: 1379: 1352: 1345: 1341: 1331: 1324: 1320: 1318: 1315: 1314: 1295: 1292: 1291: 1267: 1264: 1263: 1246: 1242: 1240: 1237: 1236: 1219: 1214: 1208: 1205: 1204: 1181: 1177: 1156: 1151: 1138: 1134: 1132: 1129: 1128: 1109: 1087: 1083: 1081: 1078: 1077: 1054: 1050: 1041: 1036: 1023: 1018: 1002: 997: 984: 980: 974: 969: 953: 949: 934: 929: 917: 914: 913: 887: 883: 877: 872: 859: 855: 849: 844: 832: 829: 828: 808: 804: 802: 799: 798: 781: 777: 775: 772: 771: 755: 752: 751: 720: 688: 684: 678: 673: 657: 653: 638: 633: 614: 609: 594: 591: 590: 569: 565: 559: 554: 542: 539: 538: 501: 497: 488: 484: 483: 470: 466: 460: 455: 442: 438: 432: 427: 422: 419: 411: 408: 407: 375: 371: 365: 360: 347: 343: 337: 332: 320: 317: 316: 286: 283: 282: 265: 261: 259: 256: 255: 239: 236: 235: 214: 209: 203: 200: 199: 183: 180: 179: 158: 154: 152: 149: 148: 128: 124: 118: 113: 100: 96: 94: 91: 90: 27: 23: 17: 12: 11: 5: 3640: 3630: 3629: 3624: 3619: 3614: 3609: 3604: 3587: 3586: 3584: 3583: 3578: 3573: 3568: 3563: 3558: 3553: 3548: 3543: 3538: 3533: 3528: 3523: 3521:Protic solvent 3518: 3513: 3505: 3503: 3497: 3496: 3494: 3493: 3488: 3483: 3478: 3473: 3468: 3466:Lattice energy 3463: 3458: 3453: 3448: 3443: 3437: 3435: 3429: 3428: 3426: 3425: 3420: 3415: 3410: 3405: 3400: 3395: 3390: 3385: 3380: 3375: 3369: 3367: 3359: 3358: 3356: 3355: 3350: 3345: 3340: 3335: 3330: 3325: 3320: 3318:Eutectic point 3315: 3310: 3305: 3300: 3295: 3290: 3285: 3280: 3278:Solid solution 3275: 3270: 3268:Ideal solution 3264: 3262: 3256: 3255: 3248: 3247: 3240: 3233: 3225: 3216: 3215: 3213: 3212: 3207: 3202: 3197: 3192: 3187: 3182: 3177: 3172: 3167: 3161: 3159: 3155: 3154: 3152: 3151: 3146: 3141: 3136: 3131: 3125: 3123: 3119: 3118: 3116: 3115: 3110: 3105: 3100: 3094: 3092: 3088: 3087: 3080: 3078: 3076: 3075: 3070: 3065: 3060: 3055: 3050: 3045: 3040: 3034: 3032: 3028: 3027: 3020: 3019: 3012: 3005: 2997: 2991: 2990: 2983: 2973: 2972: 2963: 2904: 2891: 2885: 2867: 2861:978-0471687573 2860: 2842: 2813:(3): 204–205. 2807:J. Chem. Educ. 2792: 2771: 2764: 2730: 2710: 2671: 2662:Comptes rendus 2641: 2640: 2638: 2635: 2633: 2632: 2627: 2622: 2617: 2615:DĂŒhring's rule 2612: 2607: 2602: 2596: 2594: 2591: 2583: 2544: 2541: 2536: 2529: 2517: 2513: 2505: 2494: 2491: 2466: 2465:Real solutions 2463: 2462: 2461: 2450: 2445: 2440: 2436: 2430: 2426: 2420: 2416: 2412: 2409: 2404: 2401: 2398: 2394: 2388: 2384: 2355: 2351: 2325: 2322: 2319: 2315: 2293: 2290: 2263: 2259: 2234: 2208: 2204: 2192: 2191: 2180: 2173: 2168: 2164: 2153: 2147: 2143: 2136: 2131: 2127: 2087: 2084: 2081: 2058: 2055: 2049: 2046: 2043: 2040: 2037: 2010: 2001: 1980: 1977: 1966: 1965: 1954: 1951: 1946: 1942: 1938: 1935: 1930: 1926: 1922: 1917: 1913: 1909: 1906: 1901: 1897: 1893: 1890: 1887: 1884: 1881: 1878: 1869: 1848: 1845: 1844: 1843: 1832: 1827: 1822: 1818: 1812: 1808: 1804: 1799: 1795: 1776: 1775: 1764: 1759: 1754: 1750: 1744: 1740: 1736: 1731: 1727: 1712: 1711: 1700: 1693: 1689: 1683: 1678: 1674: 1668: 1665: 1662: 1659: 1656: 1651: 1641: 1638: 1634: 1630: 1625: 1615: 1612: 1608: 1584: 1559: 1555: 1532: 1528: 1512: 1511: 1500: 1493: 1489: 1483: 1479: 1473: 1470: 1467: 1464: 1461: 1456: 1446: 1443: 1439: 1435: 1430: 1426: 1422: 1419: 1416: 1413: 1410: 1405: 1395: 1392: 1388: 1373: 1372: 1361: 1351: 1348: 1344: 1340: 1330: 1327: 1323: 1299: 1271: 1249: 1245: 1222: 1217: 1213: 1201: 1200: 1189: 1184: 1180: 1176: 1173: 1170: 1167: 1164: 1159: 1154: 1150: 1146: 1141: 1137: 1108: 1105: 1086: 1074: 1073: 1062: 1053: 1049: 1044: 1035: 1031: 1026: 1017: 1013: 1010: 1005: 996: 992: 983: 977: 968: 964: 961: 952: 948: 945: 942: 937: 928: 924: 921: 907: 906: 895: 886: 880: 871: 867: 858: 852: 843: 839: 836: 807: 780: 759: 719: 716: 708: 707: 696: 687: 681: 672: 668: 665: 656: 652: 649: 646: 641: 632: 628: 625: 622: 617: 608: 604: 601: 598: 588: 577: 568: 562: 553: 549: 546: 528: 527: 512: 509: 500: 496: 487: 481: 478: 469: 463: 454: 450: 441: 435: 426: 418: 415: 401: 400: 389: 386: 383: 374: 368: 359: 355: 346: 340: 331: 327: 324: 290: 268: 264: 243: 217: 212: 208: 187: 161: 157: 145: 144: 131: 127: 121: 116: 112: 108: 103: 99: 57:thermodynamics 15: 9: 6: 4: 3: 2: 3639: 3628: 3625: 3623: 3620: 3618: 3615: 3613: 3610: 3608: 3605: 3603: 3600: 3599: 3597: 3582: 3579: 3577: 3574: 3572: 3569: 3567: 3564: 3562: 3559: 3557: 3554: 3552: 3549: 3547: 3544: 3542: 3539: 3537: 3534: 3532: 3529: 3527: 3524: 3522: 3519: 3517: 3514: 3511: 3507: 3506: 3504: 3502: 3498: 3492: 3489: 3487: 3484: 3482: 3479: 3477: 3474: 3472: 3469: 3467: 3464: 3462: 3459: 3457: 3454: 3452: 3449: 3447: 3444: 3442: 3439: 3438: 3436: 3434: 3430: 3424: 3421: 3419: 3416: 3414: 3411: 3409: 3408:Mass fraction 3406: 3404: 3403:Mole fraction 3401: 3399: 3396: 3394: 3391: 3389: 3386: 3384: 3381: 3379: 3376: 3374: 3371: 3370: 3368: 3364: 3363:Concentration 3360: 3354: 3351: 3349: 3346: 3344: 3341: 3339: 3336: 3334: 3331: 3329: 3326: 3324: 3321: 3319: 3316: 3314: 3311: 3309: 3308:Phase diagram 3306: 3304: 3301: 3299: 3296: 3294: 3291: 3289: 3288:Flory–Huggins 3286: 3284: 3281: 3279: 3276: 3274: 3271: 3269: 3266: 3265: 3263: 3261: 3257: 3253: 3246: 3241: 3239: 3234: 3232: 3227: 3226: 3223: 3211: 3208: 3206: 3203: 3201: 3198: 3196: 3193: 3191: 3188: 3186: 3183: 3181: 3178: 3176: 3173: 3171: 3168: 3166: 3163: 3162: 3160: 3156: 3150: 3147: 3145: 3142: 3140: 3137: 3135: 3132: 3130: 3127: 3126: 3124: 3120: 3114: 3113:Spinning cone 3111: 3109: 3106: 3104: 3101: 3099: 3096: 3095: 3093: 3089: 3084: 3074: 3071: 3069: 3066: 3064: 3061: 3059: 3056: 3054: 3051: 3049: 3046: 3044: 3041: 3039: 3036: 3035: 3033: 3029: 3025: 3018: 3013: 3011: 3006: 3004: 2999: 2998: 2995: 2988: 2984: 2981: 2977: 2976: 2967: 2959: 2955: 2950: 2945: 2941: 2937: 2932: 2927: 2923: 2919: 2915: 2908: 2901: 2895: 2888: 2886:0-07-310445-0 2882: 2878: 2871: 2863: 2857: 2853: 2846: 2838: 2834: 2829: 2824: 2820: 2816: 2812: 2809: 2808: 2803: 2796: 2789: 2785: 2781: 2775: 2767: 2765:9780824753627 2761: 2757: 2753: 2749: 2745: 2739: 2737: 2735: 2727: 2726:0-19-856556-9 2723: 2719: 2714: 2706: 2702: 2698: 2695:(in French). 2694: 2693: 2688: 2684: 2683:Raoult, F.-M. 2678: 2676: 2667: 2664:(in French). 2663: 2659: 2655: 2654:Raoult, F.-M. 2649: 2647: 2642: 2631: 2628: 2626: 2625:Köhler theory 2623: 2621: 2618: 2616: 2613: 2611: 2608: 2606: 2605:Atomic theory 2603: 2601: 2598: 2597: 2590: 2589:is positive. 2588: 2581: 2577: 2573: 2569: 2565: 2561: 2557: 2553: 2548: 2540: 2539:is negative. 2535: 2527: 2523: 2522:hydrogen bond 2511: 2503: 2498: 2487: 2482: 2478: 2476: 2472: 2448: 2443: 2438: 2434: 2428: 2424: 2418: 2414: 2410: 2407: 2402: 2399: 2396: 2392: 2386: 2382: 2374: 2373: 2372: 2369: 2353: 2349: 2341: 2323: 2320: 2317: 2313: 2304: 2300: 2299:ideal-gas law 2289: 2287: 2283: 2279: 2278:mole fraction 2261: 2257: 2248: 2232: 2225:of component 2224: 2223:mole fraction 2206: 2202: 2178: 2171: 2166: 2162: 2151: 2145: 2141: 2134: 2129: 2125: 2117: 2116: 2115: 2113: 2107: 2105: 2101: 2085: 2079: 2070: 2053: 2047: 2044: 2038: 2035: 2027: 2022: 2008: 1978: 1975: 1952: 1944: 1940: 1936: 1933: 1928: 1924: 1920: 1915: 1911: 1907: 1904: 1899: 1895: 1888: 1885: 1882: 1879: 1876: 1859: 1858: 1857: 1855: 1830: 1825: 1820: 1816: 1810: 1806: 1802: 1797: 1793: 1785: 1784: 1783: 1781: 1762: 1757: 1752: 1748: 1742: 1738: 1734: 1729: 1725: 1717: 1716: 1715: 1698: 1691: 1687: 1681: 1676: 1672: 1666: 1663: 1660: 1657: 1654: 1649: 1639: 1636: 1632: 1628: 1623: 1613: 1610: 1606: 1598: 1597: 1596: 1582: 1573: 1557: 1553: 1530: 1526: 1517: 1498: 1491: 1487: 1481: 1477: 1471: 1468: 1465: 1462: 1459: 1454: 1444: 1441: 1437: 1433: 1428: 1424: 1420: 1417: 1414: 1411: 1408: 1403: 1393: 1390: 1386: 1378: 1377: 1376: 1359: 1349: 1346: 1342: 1338: 1328: 1325: 1321: 1313: 1312: 1311: 1297: 1289: 1284: 1269: 1247: 1243: 1220: 1215: 1211: 1187: 1182: 1178: 1174: 1171: 1168: 1165: 1162: 1157: 1152: 1148: 1144: 1139: 1135: 1127: 1126: 1125: 1123: 1119: 1114: 1104: 1084: 1060: 1051: 1042: 1033: 1029: 1024: 1015: 1008: 1003: 994: 990: 981: 975: 966: 962: 950: 946: 943: 935: 926: 922: 919: 912: 911: 910: 893: 884: 878: 869: 865: 856: 850: 841: 837: 834: 827: 826: 825: 805: 778: 757: 748: 746: 741: 739: 735: 734:ideal gas law 724: 715: 713: 694: 685: 679: 670: 666: 654: 650: 647: 639: 630: 626: 623: 620: 615: 606: 602: 599: 589: 575: 566: 560: 551: 547: 544: 537: 536: 535: 533: 510: 507: 498: 494: 485: 479: 476: 467: 461: 452: 448: 439: 433: 424: 416: 413: 406: 405: 404: 387: 384: 381: 372: 366: 357: 353: 344: 338: 329: 325: 322: 315: 314: 313: 311: 307: 302: 288: 266: 262: 241: 233: 215: 210: 206: 185: 177: 159: 155: 129: 125: 119: 114: 110: 106: 101: 97: 89: 88: 87: 84: 82: 78: 77:mole fraction 74: 70: 69:ideal mixture 66: 62: 58: 54: 48: 21: 3602:Distillation 3471:Raoult's law 3470: 3423:Ternary plot 3418:Mixing ratio 3210:Vacuum-based 3043:Dalton's law 3038:Raoult's law 3037: 3024:Distillation 2986: 2985:E. B. Smith 2979: 2966: 2921: 2917: 2907: 2899: 2894: 2876: 2870: 2851: 2845: 2810: 2805: 2795: 2779: 2774: 2751: 2717: 2713: 2696: 2690: 2668:: 1430–1433. 2665: 2661: 2586: 2549: 2546: 2533: 2499: 2496: 2468: 2370: 2295: 2286:distillation 2281: 2246: 2193: 2112:Dalton's Law 2108: 2099: 2071: 2023: 1967: 1850: 1847:Ideal mixing 1777: 1713: 1574: 1513: 1374: 1285: 1202: 1110: 1075: 908: 749: 742: 730: 709: 529: 402: 310:Dalton's law 303: 146: 85: 72: 20:Raoult's law 19: 18: 3576:Lyonium ion 3491:Miscibility 3476:Henry's law 3205:Steam-based 3200:Salt-effect 3175:Destructive 2699:(1): 5–20. 2620:Henry's law 2104:Henry's law 1288:equilibrium 727:components. 306:equilibrium 3596:Categories 3571:Amphiphile 3566:Lipophilic 3561:Hydrophile 3556:Hydrophobe 3433:Solubility 3328:Saturation 3298:Suspension 3190:Fractional 3185:Extractive 3165:Azeotropic 3158:Techniques 3031:Principles 2788:1891389327 2637:References 2630:Solubility 2576:chloroform 2502:chloroform 2486:azeotropes 718:Principles 3627:Solutions 3581:Lyate ion 3536:Solvation 3451:Solvation 3393:Normality 3170:Catalytic 3134:Kugelrohr 2926:CiteSeerX 2756:CRC Press 2610:Azeotrope 2526:azeotrope 2444:⋆ 2425:γ 2393:ϕ 2350:γ 2314:ϕ 2282:gas phase 2172:⋆ 2083:→ 2039:∈ 2000:Δ 1976:− 1937:⁡ 1908:⁡ 1868:Δ 1826:⋆ 1780:pressures 1758:⋆ 1692:⊖ 1682:⋆ 1667:⁡ 1650:⊖ 1633:μ 1624:⋆ 1607:μ 1558:⊖ 1492:⊖ 1472:⁡ 1455:⊖ 1438:μ 1421:⁡ 1404:⋆ 1387:μ 1343:μ 1322:μ 1221:⋆ 1212:μ 1175:⁡ 1158:⋆ 1149:μ 1136:μ 1120:that the 1043:⋆ 1030:− 1025:⋆ 1004:⋆ 976:⋆ 947:− 936:⋆ 879:⋆ 851:⋆ 680:⋆ 651:− 640:⋆ 621:− 616:⋆ 597:Δ 561:⋆ 532:evaporate 511:⋯ 480:⋯ 462:⋆ 434:⋆ 385:⋯ 367:⋆ 339:⋆ 216:⋆ 120:⋆ 3551:Polarity 3510:Category 3398:Molality 3260:Solution 3195:Reactive 2958:18855462 2837:95146940 2685:(1889). 2656:(1886). 2593:See also 2564:methanol 2475:cohesive 2471:adhesive 2247:solution 1516:fugacity 738:isotopic 3501:Solvent 3303:Colloid 3293:Mixture 3129:Alembic 2949:2646412 2815:Bibcode 2580:glycine 2572:acetone 2560:benzene 2552:ethanol 2510:acetone 2280:in the 2276:is its 2245:in the 2221:is the 2100:solvent 230:is the 174:is the 73:liquids 3048:Reflux 2956:  2946:  2928:  2883:  2858:  2835:  2786:  2762:  2724:  2574:, (4) 2566:, (3) 2558:, (2) 2508:) and 2249:, and 2194:where 2051:  1203:where 1118:deduce 254:, and 147:where 81:solute 3323:Alloy 3149:Still 2833:S2CID 2556:water 2504:(CHCl 2156:total 2954:PMID 2881:ISBN 2856:ISBN 2784:ISBN 2760:ISBN 2722:ISBN 2570:and 2562:and 2554:and 2516:COCH 797:and 3180:Dry 2944:PMC 2936:doi 2922:112 2823:doi 2701:doi 2666:104 2584:mix 2537:mix 2512:(CH 2004:mix 1872:mix 1644:vap 1618:liq 1449:vap 1398:liq 1354:vap 1333:liq 71:of 3598:: 2952:. 2942:. 2934:. 2920:. 2916:. 2831:. 2821:. 2811:72 2804:. 2754:. 2733:^ 2674:^ 2645:^ 2288:. 2114:: 2106:. 1934:ln 1905:ln 1856:: 1664:ln 1572:. 1518:, 1469:ln 1418:ln 1172:ln 38:uː 35:ɑː 3512:) 3508:( 3244:e 3237:t 3230:v 3016:e 3009:t 3002:v 2960:. 2938:: 2864:. 2839:. 2825:: 2817:: 2790:. 2768:. 2728:. 2707:. 2703:: 2697:8 2587:H 2534:H 2530:3 2518:3 2514:3 2506:3 2449:. 2439:i 2435:p 2429:i 2419:i 2415:x 2411:= 2408:p 2403:i 2400:, 2397:p 2387:i 2383:y 2354:i 2324:i 2321:, 2318:p 2305:( 2262:i 2258:y 2233:i 2207:i 2203:x 2179:, 2167:i 2163:p 2152:p 2146:i 2142:y 2135:= 2130:i 2126:x 2086:1 2080:x 2057:] 2054:1 2048:, 2045:0 2042:[ 2036:x 2009:H 1979:T 1953:. 1950:) 1945:2 1941:x 1929:2 1925:x 1921:+ 1916:1 1912:x 1900:1 1896:x 1892:( 1889:T 1886:R 1883:n 1880:= 1877:G 1831:. 1821:i 1817:p 1811:i 1807:x 1803:= 1798:i 1794:p 1763:. 1753:i 1749:f 1743:i 1739:x 1735:= 1730:i 1726:f 1699:. 1688:p 1677:i 1673:f 1661:T 1658:R 1655:+ 1640:, 1637:i 1629:= 1614:, 1611:i 1583:i 1554:p 1531:i 1527:f 1499:, 1488:p 1482:i 1478:f 1466:T 1463:R 1460:+ 1445:, 1442:i 1434:= 1429:i 1425:x 1415:T 1412:R 1409:+ 1394:, 1391:i 1360:. 1350:, 1347:i 1339:= 1329:, 1326:i 1298:i 1270:i 1248:i 1244:x 1216:i 1188:, 1183:i 1179:x 1169:T 1166:R 1163:+ 1153:i 1145:= 1140:i 1089:B 1085:x 1061:. 1056:B 1052:x 1048:) 1038:A 1034:p 1020:B 1016:p 1012:( 1009:+ 999:A 995:p 991:= 986:B 982:x 971:B 967:p 963:+ 960:) 955:B 951:x 944:1 941:( 931:A 927:p 923:= 920:p 894:. 889:B 885:x 874:B 870:p 866:+ 861:A 857:x 846:A 842:p 838:= 835:p 810:B 806:p 783:A 779:p 758:p 695:. 690:B 686:x 675:A 671:p 667:= 664:) 659:A 655:x 648:1 645:( 635:A 631:p 627:= 624:p 611:A 607:p 603:= 600:p 576:, 571:A 567:x 556:A 552:p 548:= 545:p 508:+ 503:B 499:n 495:+ 490:A 486:n 477:+ 472:B 468:n 457:B 453:p 449:+ 444:A 440:n 429:A 425:p 417:= 414:p 388:. 382:+ 377:B 373:x 362:B 358:p 354:+ 349:A 345:x 334:A 330:p 326:= 323:p 289:i 267:i 263:x 242:i 211:i 207:p 186:i 160:i 156:p 130:i 126:x 115:i 111:p 107:= 102:i 98:p 47:/ 44:z 41:l 32:r 29:ˈ 26:/ 22:(

Index

/ˈrɑːuːlz/
physical chemistry
thermodynamics
François-Marie Raoult
partial pressure
ideal mixture
mole fraction
solute
partial pressure
equilibrium vapor pressure
equilibrium
Dalton's law
evaporate
van 't Hoff factor

ideal gas law
isotopic
intermolecular forces
François-Marie Raoult
deduce
chemical potential
equilibrium
fugacity
pressures
Gibbs free energy change of mixing
Gibbs–Duhem equation
Henry's law
Dalton's Law
mole fraction
mole fraction

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