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Comment published on 24 August 2023, see Molecules 2023, 28(17), 6215.
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Article

Revision and Extension of a Generally Applicable Group-Additivity Method for the Calculation of the Standard Heat of Combustion and Formation of Organic Molecules

by
Rudolf Naef
1,* and
William E. Acree, Jr.
2
1
Department of Chemistry, University of Basel, 4003 Basel, Switzerland
2
Department of Chemistry, University of North Texas, Denton, TX 76203, USA
*
Author to whom correspondence should be addressed.
Molecules 2021, 26(20), 6101; https://doi.org/10.3390/molecules26206101
Submission received: 15 September 2021 / Revised: 4 October 2021 / Accepted: 6 October 2021 / Published: 10 October 2021

Abstract

:
The calculation of the heats of combustion ΔH°c and formation ΔH°f of organic molecules at standard conditions is presented using a commonly applicable computer algorithm based on the group-additivity method. This work is a continuation and extension of an earlier publication. The method rests on the complete breakdown of the molecules into their constituting atoms, these being further characterized by their immediate neighbor atoms. The group contributions are calculated by means of a fast Gauss–Seidel fitting calculus using the experimental data of 5030 molecules from literature. The applicability of this method has been tested by a subsequent ten-fold cross-validation procedure, which confirmed the extraordinary accuracy of the prediction of ΔH°c with a correlation coefficient R2 and a cross-validated correlation coefficient Q2 of 1, a standard deviation σ of 18.12 kJ/mol, a cross-validated standard deviation S of 19.16 kJ/mol, and a mean absolute deviation of 0.4%. The heat of formation ΔH°f has been calculated from ΔH°c using the standard enthalpies of combustion for the elements, yielding a correlation coefficient R2 for ΔH°f of 0.9979 and a corresponding standard deviation σ of 18.14 kJ/mol.

1. Introduction

The present compilation of data on the heat of combustion and formation of more than 5000 organic molecules and their comparison with theoretical calculations based on a generally applicable atom-groups additivity method is a continuation of theoretical studies on the prediction of various molecular descriptors published in an earlier paper [1]. While this publication primarily focused on the extraordinary versatility of the applied version of the atom-group additivity method for a large number of descriptor predictions, which has been proven by its extension to several further molecular descriptors in subsequent papers [2,3,4,5,6], the present interest rests on the further increase in the trustworthiness of their calculated heats of combustion and formation and their extension to compound classes not yet covered by the earlier paper, particularly the ionic liquids. Previous versions of heat-of-combustion calculations have been based on the additivity of bond energies [7,8,9], on empirical relations within a series of molecules and their heat of combustion [10,11], on the “heat of atomization” [12], on the combustion value of the electrons in a molecule, corrected for its structural and functional features [13,14], or on the “molecular oxygen balance” [15], all of them outlined in more detail in [1]. An indirect approach to the prediction of the heat of combustion—due to their direct interdependence—is via the calculation of the heat of formation of a molecule, which is either accessible through elaborate quantum-theoretical methods (e.g., [16]) or through a group-additivity method [17,18] similar to the present one. Most of these various approaches have been optimized for a certain class of compounds and are therefore not generally applicable. In contrast, the present calculation method is easily extendable and in principle enables the calculation of the heat of combustion and formation of literally any organic molecule under the sun.

2. Method

The calculations rest upon a database of at present 34,380 molecules, recorded in their geometry-optimized 3D conformation, encompassing pharmaceuticals, plant protectors, dyes, ionic liquids, liquid crystals, metal-organics, intermediates, and many more, wherein—among many further experimentally determined and calculated molecular descriptors—for 5560 of them, the published experimental combustion and/or formation enthalpies have been stored. In order to avoid structural ambiguity, all six-membered aromatic rings have been defined by six aromatic bonds, in contrast to the more commonly used single-double-bond alternating style. Furthermore, for the same reason, the positive charge in amidinium, pyrazolium, and guanidinium fragments is positioned on the carbon atom between the nitrogen atoms, incidentally in better conformance with the true situation, as shown in, e.g., Figure 1 in [3]. (For the carboxylate or the nitro group, the analogous consideration of charge equilibration is not required within the present atom-group concept, as they are unambiguously defined.) Finally, compounds containing both acidic and basic groups, in particular primary alkylamines (e.g., amino acids) or guanidines (e.g., in creatine or arginine), are treated as zwitter-ionic molecules.

2.1. Definition of the Atom Groups

The principle of the breakdown of a molecule into its atom groups in a computer-readable form has been outlined in detail in [1]. Consequently, their naming and meaning are retained in the present work as explained in Table 1 of [1]. However, since then, a number of further atom groups had to be added to the group-contribution parameters set in order to cover the considerable amount of additional, structurally variable molecules. In particular, the inclusion of ordinary salts and ionic liquids required the charged atom groups listed and explained in Table 1, which are interpreted analogously by the computer algorithm as the remaining ones. (Some of these atom groups have already been introduced for the calculation of the liquid viscosity of molecules in [3].)
The atom groups do not take into account the characteristics of the molecules’ three-dimensional structures, such as intramolecular hydrogen-bridge bonds, intramolecular H-H interactions, or ring-strain forces. These effects have summarily been considered by means of the special groups listed and explained in Table 2, wherein the column titles are not to be interpreted literally. With regard to the ring-strain contributions (Angle60, Angle90, and Angle102), caused by forced angle constriction at each ring atom in small rings, it should be stressed that the calculated values inherently also encompass the effect of the compensatory angle widening between the ring atoms and any further atoms attached to them (e.g., the H-C-H and H-C-C angles on cyclopropane). These special groups are treated just like the ordinary atom groups in the calculation of their contribution as well as the subsequent molecular descriptor value.

2.2. Calculation of the Group Contributions

The parameter values of the atom and special groups are calculated in four steps, outlined in detail in [1]: the first step creates a temporary compounds list and adds those compounds from the database into it for which the experimental heat of combustion is known. Secondly, for each of the “backbone” atoms (i.e., atoms bound to at least two other direct neighbor atoms) in the molecules, its atom group is defined according to the rules defined in [1], corresponding to the atom type and neighbors’ terms listed in Table 4, and then its occurrence in the molecule is counted. Next, an M × (N + 1) matrix is generated, where M is the number of molecules, where N + 1 is the number of atoms and special groups of Table 4 plus the molecules’ experimental heats of combustion, and where each matrix element (i,j) receives the number of occurrences of the jth atomic or special group in the ith molecule. Finally, normalization of this matrix into an Ax = B matrix and its subsequent balancing using a fast Gauss–Seidel calculus [19] yields the group contributions x, which are shown in Table 4.

2.3. Calculation of the Standard Heats of Combustion and Formation

The subsequent calculation of the heat of combustion ΔH°(c) is a simple summing up of the contributions of the atom groups in a molecule using the values shown in Table 4, applying Equation (1), wherein ai and bj are the contribution values, Ai is the number of occurrences of the ith atom group and Bj is the number of occurrences of the special groups.
∆H°c = Σi ai*Ai + Σj bj*Bj
It is immediately evident that these calculations are limited to compounds for which each atom group contained in it (excluding the special groups) has its corresponding one shown in Table 4. Beyond this, in order to receive reliable results, only “valid” group contributions are to be used, i.e., contributions that have been supported in the group-parameters calculation by at least three independent molecules, i.e., by the number in the rightmost column of Table 4 exceeding 2. As a consequence, the statistics data at the bottom of Table 4 show that the number of compounds for which finally the heat of combustion is calculated (lines B, C, and D) is smaller than that on which the computation of the complete set of group contributions is based (line A).
The heat of formation of the molecules is immediately calculated from their heat of combustion by the subtraction of the standard enthalpies of combustion of the elements as given in [20,21].
In Table 3, a simple example may explain the use of Table 4: the experimental heat of combustion of 4-methylene-2-oxetanone (diketene) is −1913.4 kJ/mol [21]. The atom groups and the special group defining this compound are collected in Table 3 and yield a calculated value of −1903.2 kJ/mol.

2.4. Cross-Validation Calculations

The results of the heat-of-combustion data are immediately tested for plausibility using a 10-fold cross-validation algorithm, requiring 10 recalculations that guarantee that each of the complete set of compounds has been used once as a test sample. The corresponding training and test data are added to each of the molecule files, and the respective statistics data are collected at the bottom of Table 4. Again, due to the 10% smaller number of training molecules used in the 10 cross-validation calculations, the number of compounds for which the heat of combustion is evaluated as the test value is even smaller (lines E, F, G, and H) than that of the training set (lines B, C, and D). The statistics data of Table 4 also show a significantly lower number of “valid” groups in line A than the total number of atoms and special groups. The residual “invalid” groups, although at present not applicable for heat-of-combustion calculations, have been left in Table 4 for future use in this continuing project. Interested scientists may want to help to increase the number of “valid” groups in this database by molecules carrying the under-represented atom groups. At present, the list of elements for heat-of-combustion calculations is limited to H, B, C, N, O, P, S, Si, and/or halogen.
Table 4. Atom Groups and their Contributions to ΔH°(c) Calculations (in kJ/mol).
Table 4. Atom Groups and their Contributions to ΔH°(c) Calculations (in kJ/mol).
EntryAtom TypeNeighborsContributionOccurrencesMolecules
1BC3−5771.411010
2BC2O−5234.322
3B(-)F4−128.4111
4C sp3H3B927.3431
5C sp3H3C−774.5356592598
6C sp3H3N−1273.86288183
7C sp3H3N(+)−1258.262210
8C sp3H3O−1273.9493333
9C sp3H3S−1435.833630
10C sp3H3P−1106.3531
11C sp3H3Si−1323.211649
12C sp3H2BC1052.3228
13C sp3H2C2−653.4791392066
14C sp3H2CN−1150.33632346
15C sp3H2CN(+)−1136.527651
16C sp3H2CO−1140.921209753
17C sp3H2CS−1313.58180118
18C sp3H2CP−825.6363
19C sp3H2CF−626.921514
20C sp3H2CCl−616.88170
21C sp3H2CBr−620.82320
22C sp3H2CJ−685.85129
23C sp3H2CSi−1211.7913051
24C sp3H2N2−1644.623312
25C sp3H2N2(+)−1666.8566
26C sp3H2NO−1630.6586
27C sp3H2NS−1776.9721
28C sp3H2NS(+)−1817.7311
29C sp3H2NP(+)−565.6811
30C sp3H2O2−1605.493126
31C sp3H2OSi−1715.4111
32C sp3H2OCl−1115.0943
33C sp3H2S2−1997.6797
34C sp3HBC2119762
35C sp3HC3−529.091386765
36C sp3HC2N−1026.3510684
37C sp3HC2N(+)−1004.994340
38C sp3HC2O−1010.37545330
39C sp3HC2S−1179.913425
40C sp3HC2Si−1076.9242
41C sp3HC2F−486.2955
42C sp3HC2Cl−491.94832
43C sp3HC2Br−499.1797
44C sp3HC2J−574.7243
45C sp3HCN2−1514.2954
46C sp3HCN2(+)−1537.2355
47C sp3HCNO−1525.3255
48C sp3HCNO(+)−1522.6942
49C sp3HCNS−1683.6642
50C sp3HCO2−1473.476354
51C sp3HCS2−1791.6611
52C sp3HCF2−447.71413
53C sp3HCFCl−470.2144
54C sp3HCCl2−494.971817
55C sp3HCClBr−510.3911
56C sp3HCBr2−475.6711
57C sp3HN3(+)−2166.0811
58C sp3HNO2−1989.1711
59C sp3HO3−1920.7966
60C sp3HOF2−891.8122
61C sp3BC31320.4331
62C sp3C4−403.7392287
63C sp3C3N−886.444634
64C sp3C3N(+)−875.682826
65C sp3C3O−876.38181135
66C sp3C3S−1050.272319
67C sp3C3F−451.56116
68C sp3C3Cl−355.2699
69C sp3C3Br−362.0722
70C sp3C3J−430.211
71C sp3C2N2(+)−1417.0599
72C sp3C2O2−1331.44238
73C sp3C2S2−1708.5441
74C sp3C2F2−318.7410428
75C sp3C2FCl−331.0932
76C sp3C2Cl2−357.3777
77C sp3CN3(+)−2020.091911
78C sp3CN2F(+)−1420.862416
79C sp3CN2Cl(+)−1451.1922
80C sp3CNF2−848.6762
81C sp3CNF2(+)−853.8132
82C sp3CO3−1771.5787
83C sp3COF2−802.9533
84C sp3COCl2−893.6711
85C sp3CF3−251.658364
86C sp3CF2Cl−306.09108
87C sp3CF2Br−319.6254
88C sp3CFCl2−317.277
89C sp3CFClBr−276.5111
90C sp3CCl3−371.892524
91C sp3CBr3−345.1911
92C sp3N2OF(+)−1875.9511
93C sp3N4(+)−2635.733
94C sp3N3F(+)−4981.4222
95C sp3O4−2239.9933
96C sp3O2F2−1255.7511
97C sp3OF3−692.5722
98C sp3OF2Cl−768.9111
99C(-) sp3C3−3078.3222
100C sp2H2=C−703.3255227
101C sp2H2=N−1694.7922
102C sp2HC=C−563.481268695
103C sp2HC=N−1522.256458
104C sp2HC=O−390.29115111
105C sp2H=CN−1024.99141103
106C sp2HC=N(+)−5278.2677
107C sp2H=CN(+)−1032.1744
108C sp2H=CO−619.085448
109C sp2H=CS−1228.758061
110C sp2H=CF−547.7322
111C sp2H=CCl−550.3186
112C sp2H=CBr−574.2222
113C sp2H=CSi−1051.13169
114C sp2HN=N−1998.614542
115C sp2HN=O−830.281211
116C sp2H=NO−1583.3222
117C sp2HO=O−410.951919
118C sp2H=NS−2218.7933
119C sp2C2=C−430.98318255
120C sp2C2=N−1378.538267
121C sp2C2=N(+)326.7766
122C sp2C=CN−893.418666
123C sp2C=CN(+)−928.071010
124C sp2C2=O−241.97400337
125C sp2C=CO−470.128669
126C sp2C=CS−1085.435645
127C sp2C=CF−452.8876
128C sp2C=CCl−418.162213
129C sp2C=CBr−412.6611
130C sp2=CN2−1367.071111
131C sp2=CN2(+)−1387.081010
132C sp2CN=N−1858.114840
133C sp2CN=N(+)−1939.366
134C sp2CN=O−687.04310243
135C sp2C=NO−1412.251816
136C sp2=CNO−980.2611
137C sp2=CNO(+)−1004.766
138C sp2CN=S−1516.7876
139C sp2C=NS−2037.9766
140C sp2=CNS(+)−1601.0122
141C sp2=CNCl−854.4611
142C sp2CO=O−256.511142872
143C sp2CO=O(-)98.045150
144C sp2C=OS−913.8177
145C sp2C=OF−193.6433
146C sp2C=OCl−202.041411
147C sp2C=OBr−203.5622
148C sp2C=OJ−281.0522
149C sp2=COF−297.8322
150C sp2CS=S−1716.1433
151C sp2=CS2−1853.9321
152C sp2=CF2−413.798
153C sp2=CFCl−362.0211
154C sp2=CCl2−420.1175
155C sp2=CJ2−544.2521
156C sp2N2=N−2333.016755
157C sp2N2=N(+)583.1122
158C sp2N2=O−1148.85124107
159C sp2N=NO−1909.1633
160C sp2N2=S−1999.022725
161C sp2N=NS−2485.54109
162C sp2NO=O−712.72221
163C sp2N=OS−1624.4511
164C sp2NO=S−1586.9955
165C sp2=NOS−2019.3211
166C sp2=NOCl−1416.8611
167C sp2NS=S−2180.966
168C sp2NS=S(-)−2015.4944
169C sp2=NSCl−2036.6811
170C sp2O2=O−288.271414
171C sp2O=OCl−207.8544
172C sp2=OS2−1589.5222
173C sp2S2=S−2384.6833
174C aromaticH:C2−54410,7411946
175C aromaticH:C:N−677.57176121
176C aromaticH:C:N(+)−664.154625
177C aromaticH:N2−805.131210
178C aromatic:C3−404.91496193
179C aromaticC:C2−412.3925721349
180C aromaticC:C:N−537.5510662
181C aromaticC:C:N(+)−537.43721
182C aromatic:C2N−904.12521380
183C aromatic:C2N(+)−924.19323214
184C aromatic:C2:N−541.187354
185C aromatic:C2:N(+)−537.033318
186C aromatic:C2O−485.35724496
187C aromatic:C2P−739.7993
188C aromatic:C2S−1093.919475
189C aromatic:C2Si−977.523011
190C aromatic:C2F−400.2113667
191C aromatic:C2Cl−391.36235137
192C aromatic:C2Br−393.117250
193C aromatic:C2J−466.273934
194C aromaticC:N2−653.0453
195C aromatic:CN:N−1014.821713
196C aromatic:CN:N(+)−1105.8332
197C aromatic:C:NO−567.841111
198C aromatic:C:NCl−521.233021
199C aromatic:C:NBr−517.9843
200C aromaticN:N2−1126.332214
201C aromatic:N2O−708.43176
202C aromatic:N2S−1372.6411
203C aromatic:N2Cl−639.791110
204C(+) aromaticH:N2915.781717
205C(+) aromatic:N31847.8433
206C spH#C−654.95042
207C spC#C−502.89198108
208C sp=C2−532.171211
209C spC#N−495.27165139
210C spC#N(+)−521.6243
211C spC#N(-)378.0662
212C sp#CN−1069.6422
213C sp=C=N−1519.9822
214C sp=C=O−281.2443
215C sp#CS−1214.9422
216C sp#CCl−514.9332
217C sp#CSi−1091.5133
218C spN#N−982.3644
219C spN#N(-)−144.09105
220C sp=N2−2404.622
221C sp#NO−648.922
222C sp=N=O−1216.262216
223C sp#NS−1277.4111
224C sp=N=S−2056.0322
225C sp=N=S(-)−1076.322
226N sp3H2C218.816456
227N sp3H2C(pi)253.54334285
228N sp3H2N−304.072923
229N sp3H2N(pi)−266.7111
230N sp3H2S215.3699
231N sp3HC2814.556963
232N sp3HC2(pi)846.53138105
233N sp3HC2(2pi)845.11253200
234N sp3HCN288.2153
235N sp3HCN(pi)315.324128
236N sp3HCN(+)(pi)734.5354
237N sp3HCN(2pi)359.346964
238N sp3HCN(+)(2pi)717.6666
239N sp3HCO(pi)520.522
240N sp3HCS(pi)1015.1733
241N sp3HCSi829.1955
242N sp3HN2(2pi)−176.6611
243N sp3HNS552.3411
244N sp3HSi2850.7511
245N sp3C31409.088473
246N sp3C3(pi)1429.389884
247N sp3C3(2pi)1430.986952
248N sp3C3(3pi)1421.73123
249N sp3C2N871.2711
250N sp3C2N(pi)896.781311
251N sp3C2N(+)(pi)1320.44025
252N sp3C2N(2pi)9542322
253N sp3C2N(+)(2pi)1269.38127
254N sp3C2N(3pi)948.1199
255N sp3C2N(+)(3pi)1230.4333
256N sp3C2O1037.733
257N sp3C2S584.4463
258N sp3C2Si1437.1286
259N sp3C2F(2pi)−2337.0911
260N sp3C2Cl(2pi)878.711
261N sp3C2Br(2pi)900.6711
262N sp3CN2(2pi)491.4797
263N sp3CN2(+)(2pi)1183.5111
264N sp3CN2(3pi)550.3533
265N sp3CN2(+)(3pi)774.3133
266N sp3CF2197.51127
267N sp3CF2(pi)997.3111
268N sp3Si31479.0711
269N sp2H=C7601010
270N sp2C=C1411.35154133
271N sp2C=N375.867038
272N sp2C=N(+)714.593531
273N sp2=CN866.59141117
274N sp2=CN(+)1299.955
275N sp2C=O421.691312
276N sp2=CO935.487855
277N sp2=CS705.7521
278N sp2=CF011
279N sp2N=N−82.188041
280N sp2N=O1.3586
281N sp2=NO762.4721
282N sp2=NO(+)1041.44116
283N sp2O=O831.5299
284N sp2P=P−482.1472
285N aromaticH2:C(+)−1025.7353
286N aromaticHC:C(+)−363.2422
287N aromaticC2:C(+)216.633619
288N aromatic:C2214.34273189
289N aromatic:C:N41.4263
290N aromatic:C:N(+)2190.811
291N(+) sp3H3C57.664746
292N(+) sp3H2C2607.9699
293N(+) sp3HC31364.5564
294N(+) sp3C41885.7288
295N(+) sp2C=CO(-)5214.7577
296N(+) sp2C=NO442.92168
297N(+) sp2C=NO(-)155.641611
298N(+) sp2CO=O(-)548.28550310
299N(+) sp2=CO2(-)−568.2266
300N(+) sp2NO=O(-)−366.727654
301N(+) sp2O2=O(-)188.797337
302N(+) aromaticC:C2698.7511
303N(+) aromatic:C2O(-)234.675840
304N(+) aromatic:C:NO(-)−2193.111
305N(+) spC#C(-)−94.0766
306N(+) sp#CO(-)043
307N(+) sp=N2(-)−542.943026
308N(-)C2−776.8555
309OHC550.37663373
310OHC(pi)149.9795622
311OHN−183.4633
312OHN(pi)−66.292923
313OHO−35.982926
314OHP−107.2732
315OHS346.888
316OHSi241.5811
317OBC1904.2422
318OC21101.66471283
319OC2(pi)701.99896686
320OC2(2pi)278.25167156
321OCN(pi)−291.52418
322OCN(+)(pi)401.596329
323OCN(2pi)131.931414
324OCN(+)(2pi)398.511
325OCO523.4312065
326OCO(pi)113.286529
327OCS457.66189
328OCP542.76104
329OCP(pi)91.2631
330OCSi708.965421
331OCSi(pi)318.693815
332ON2(2pi)−65.351514
333ON2(+)(2pi)−220.155
334OOSi106.9284
335OSi2400.13113
336P3C3124.5433
337P4C3=O−243.1811
338P4C3=S−373.6111
339P4C2O=O−169.2411
340P4CO2=O197.0411
341P4CO2=O(-)−394.0711
342P4N=NCl2072
343P4O3=O14.144
344S2HC−88.464742
345S2HC(pi)−58.541010
346S2C2690.557866
347S2C2(pi)714.512621
348S2C2(2pi)750.838882
349S2CN(pi)−618.0311
350S2CS42.29189
351S2CS(pi)53.77168
352S2N225.2611
353S2N2(2pi)011
354S2NS−291.8721
355S4C2=O849.5388
356S4C2=O21073.534343
357S4CN=O2−41.351111
358S4CO=O2216.1433
359S4CO=O2(-)777.2722
360S4C=O2S394.5221
361S4N2=O2558.4911
362S4NO=O2−918.6911
363S4O2=O−92.9955
364S4O2=O2116.2344
365S4O2=O2(-)−556.3844
366S4O=O2F−470.0511
367S4O=O2Cl−463.6311
368SiH3C−740.1944
369SiH2C212.4222
370SiHC3602.132929
371SiHC2Cl67.1811
372SiHCCl2−100.0511
373SiHN3−2430.711
374SiHO3−931.4211
375SiC41327.161515
376SiC3N317.051512
377SiC3O813.971212
378SiC3Cl1013.3911
379SiC3Br1000.8511
380SiC2O2285.19168
381SiC2Cl2592.6933
382SiCO3−235.181616
383SiCCl3145.4311
384SiO4−763.9877
385HH Acceptor0.27241188
386H.H−5.79381142
387H..H−1.3149081297
388Angle60 −35.25405118
389Angle90 −24.5132166
390Angle102 −4.651663451
ABased onValid groups267 5030
BGoodness of fitR21 4886
CDeviationAverage13.66 4886
DDeviationStandard18.12 4886
EK-fold cvK10 4790
FGoodness of fitQ21 4790
GDeviationAverage (cv)14.44 4790
HDeviationStandard (cv)19.16 4790

3. Sources of Heat-of-Combustion and Formation Data

The present list of references encompasses the sources for the experimental standard heats of combustion as well as those of formation, because the input of the heat of combustion into a molecule’s database immediately also triggers the calculation and addition of its heat of formation and vice versa. Experimental data given in kcal/mol are translated into kJ/mol by multiplication with 4.1858.
A large number of experimental data have been provided by several comprehensive papers; in particular, Domalski’s collection [21] published an extended variation of compounds containing the elements C, H, N, O, P, and S. The CRC Handbook of Chemistry and Physics [22] included a chapter containing the heats of formation of another large list of compounds. In the last 6 years since the publication of the predecessor version [1] of this paper, a large number of publications have been found, which produced further experimental combustion and formation data. In the following, they have been sorted by their dominant contributory structural features to the present subject. An especially extended amount of research has been done with hydrocarbons including alkanes, alkenes, alkynes, and aromatics [23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60], forming the core of the various carbon groups. In addition, many data have dealt specifically with alcohols and phenol derivatives [61,62,63,64,65,66,67,68,69,70,71,72,73,74], ethers [75,76,77,78,79,80,81,82,83,84], carbaldehydes [85,86,87,88,89,90,91,92,93,94], ketones [95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112], carboxylic acids [113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135], carboxylic esters, carbonates and lactones [136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154], sugars [155], peroxides [156,157,158,159,160,161], amines and imines [162,163,164,165,166,167,168,169], amides, imides, amidines and hydrazides [170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186], guanidines [187,188], ureas [189,190,191,192,193,194,195,196], urethanes [197], carbamates [198], azides [199,200], nitriles and nitriloxides [201,202,203,204,205,206,207,208], isocyanates [209], oximes [210], nitramines [211], azo- and azoxy compounds [212,213,214], N-oxides [215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230], nitroso [231] and nitro compounds [232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263], nitrates [264], amino acids [265,266,267,268,269,270,271,272,273,274,275,276,277], sulfur-containing [278,279,280,281,282,283,284,285,286,287,288,289], phosphorus-containing [290], silicon-containing [291,292,293,294], and boron-containing compounds [295]. Beyond these, a large number of halogen-substituted compounds, many of them carrying any of the further functional groups just mentioned, have been found [296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339,340,341,342,343,344,345,346,347,348,349,350,351,352,353,354,355,356,357]. A considerable number of experimental combustion and formation data have been published for heterocyclic compounds, including hetarenes, unsubstituted and substituted by functional groups just mentioned. According to the hetero elements in the ring system, they have been subdivided into Nx-heterocycles (where x is 1 to 4) [358,359,360,361,362,363,364,365,366,367,368,369,370,371,372,373,374,375,376,377,378,379,380,381,382,383,384,385,386,387,388,389,390,391,392,393,394,395,396,397,398,399,400,401,402,403,404,405,406,407,408,409,410,411,412,413,414,415,416,417,418,419,420,421,422,423], N,O-heterocycles [424,425,426,427,428,429,430,431,432,433], N,S-heterocycles [434,435,436,437,438], Ox-heterocycles [439,440,441,442,443,444,445,446,447,448,449,450,451,452], and Sx-heterocycles [280,282,283,284,453,454,455,456,457,458,459,460,461]. A small number of papers contributed data for hetarenes with several element combinations [462,463,464,465,466,467,468,469,470,471]. In addition, and as an important extension to the earlier paper [1], a great variety of ionic liquids has been added [472,473,474,475,476,477,478,479,480,481,482,483,484,485,486,487,488,489,490,491,492,493,494,495,496,497,498]. Finally, a number of publications contributed combustion and/or formation data that could not be assigned to any of the aforementioned classes [499,500,501,502,503,504,505,506,507,508,509,510,511,512,513,514,515,516,517,518,519,520,521,522,523,524,525,526].

4. Results

4.1. Heat of Combustion

The first preliminary calculations of the group contributions were based on the complete set of 5560 compounds for which experimental heats of combustion and/or formation were available. However, contrary to the approach in the earlier paper [1], a further restriction was introduced in that only those compounds were allowed to remain in the consecutive calculations, the experimental values of which did not deviate by more than three times the cross-validated standard error from the cross-validated calculated value. Accordingly, the final group contributions rested on 5030 compounds, as shown on row A in Table 4. The discarded molecules have been collected in an outliers list, available with Supplementary Materials. As a consequence, the correlation coefficient Q2 is even better than the previously published value of 0.9999 and is now indistinguishable from 1 (row F in Table 4). Analogously, the new cross-validated standard error of 19.16 kJ/mol (row H in Table 4) is considerably better than the earlier one of 25.2 kJ/mol. Not surprisingly, the mean absolute deviation over 4886 compounds is just 0.4% over a calculated heat-of-combustion range of from −72 kJ/mol (hydrogen peroxide) to −35,112.2 kJ/mol (glycerol trioleate). These excellent statistical data are well reflected in the straight line of the data points in the correlation diagram of Figure 1 and the perfectly symmmetrically balanced Gaussian bell curve of the histogram in Figure 2. The only downside, however, is the much longer list of 390 atoms and special groups required (compared to the 273 of the earlier paper [1]), of which only 267 are “valid” for predictions. However, the latter still enable the calculation of the heats of combustion and formation of presently 29,067 molecules, i.e., ca. 84.5% of the complete dataset. The complete set of molecules used for the group-parameters calculations is available in the Supplementary Material.
The extraordinary accuracy of the predictions allows a deeper analysis of the actual structural state of certain classes of molecules for which alternative structures are possible at standard conditions, in particular as to which prototropic forms are prevailing in amino acids and which tautomeric form is prevalent in compounds that may exist in both hydroxyazo and hydrazone or keto and enol forms. Beyond this, an educated estimate as to what the enthalpy difference is between the alternative forms might be possible.

4.1.1. Amino Acids

It is common knowledge that amino acids exist in zwitterionic form both in the crystalline as well as the liquid state [527], whereas in the gas phase they exist in their non-ionic form. To our knowledge, the difference in the enthalpies of combustion between these two forms has not yet been systematically analyzed. In Table 5, the calculated values for the non-ionic and zwitter-ionic forms of a series of amino acids are compared with their experimental data.
The average ΔH°(c) difference was calculated as ca. 61.5 kJ/mol, with the non-ionic form exhibiting the more negative value. Cystine is an outlier in that it contains two amino-acid functions. Interestingly, sarcosine (N-methylglycine) shows the lowest difference between the two forms, which is due to the fact that it carries a less basic dialkylamino group. Similarly, N-phenylglycine differs from the remaining amino acids by an amino group that is conjugated to the phenyl ring, again lowering its basicity. Except for these special cases, the experimental values are in better compliance with the calculated values of the zwitter forms.

4.1.2. Azo-Hydrazone Tautomerism

The observation of the hydroxyazo-hydrazone tautomerism is well known among dye chemists dealing with azo dyes, as it has a drastic effect on the electronic absorption spectra. In an earlier paper [1], it was demonstrated that the direction of the tautomeric equilibrium is fairly predictable on the basis of the calculated heats of formation of the hydroxyazo and the hydrazone form. Analogously, the heats of combustion, now founded on a much larger structural basis, should confirm these observations, with the less negative enthalpy indicating the dominating form. Indeed, in conformance with experimental observation, the calculated values listed in Table 6 confirm that arylazo-naphthols primarily exist in their hydrazone form, whereas the opposite is true for the arylazo-naphthylamines. On the other hand, the small enthalpy difference found between the two forms of the phenylazophenols confirms their weak tendency to tautomerize. In addition, the available experimental heats of combustion for 4-phenylazophenol and 4-aminoazobenzene are in fairly good agreement with their prevailing forms.

4.1.3. Keto-Enol Tautomerism

Prediction of the dominant forms in keto-enol tautomers under standard conditions has been shown to be at best coincidental in [1], which is not surprising in view of the mostly small enthalpy differences between the two forms. Recalculated values of the heat of combustion of the example molecules in [1], based on the updated group-parameters set, are compared with their experimental values, where available, in Table 7. As is evident, except for acetone, the enol form is supposed to be the dominant tautomer throughout, which clearly contradicts the experience, most prominently with cyclohexanone and cyclopentanone. Beyond this, the experimental values are of no help despite the small standard error Q2 of 19.16 kJ/mol (see Table 4) because the deviations between the enthalpies of both forms with the experiment are well within the tolerated boundaries.

4.1.4. Ionic Liquids

The main extension of the present atom-groups additivity method enabled the inclusion of the heats of combustion of the ionic liquids. Unfortunately, of the 679 ionic liquids presently stored in the database, only for 28 of them was the experimental heat of combustion comparable with calculated values to this date due to the restrictions mentioned earlier. They essentially cover nitrates, dicyanamides, sulfates, dialkyldithiocarbamates, and halogenides of various imidazolium, ammonium, and glycinium cations. In Table 8, these compounds are listed, and their experimental values are compared with the calculated ones. Their conformance is exceptionally good, resulting in a mean absolute deviation of only 0.23%.

4.2. Heat of Formation

The heat of formation has been calculated indirectly from the calculated heat of combustion for each compound for which experimental data were available using the heats of combustion for the elements given in [20,21]. Accordingly, the same restrictions concerning “te” valid “ty” of the atom groups as well as the elements themselves apply. Therefore, the number of compounds in the correlation diagram of Figure 3 is identical with that of Figure 1. However, due to the distinctly smaller range of heat-of-formation values from −7238.2 (perfluorohexadecane) to +1039.7 kJ/mol (2,4,6-triazido-s-triazine) and the error-propagation effect, the correlation coefficient R2 is “only” 0.9979, and since the standard error σ is still 18.14 kJ/mol, their mean absolute deviation is 27.23%. The histogram of Figure 4 again confirms the symmetrical Gaussian error distribution of the experimental heats of formation about the calculated ones.

5. Conclusions

The present paper is proof of the easy expandability of the group-additivity method outlined in [1] for the calculation of the heats of combustion and formation of in principle any organic molecule to consider. A large amount of more than 5000 molecules upon which the atom-group parameters are based allowed strict filtering out of the worst outliers without undue sacrifice of “invalidated” atom groups, resulting in an as-yet unsurpassed accuracy of the predicted heat of combustion with a mean absolute deviation of only 0.4% for up to 84.5% of nearly any kind of organic compound. Beyond this, the present method basically allows the accurate calculation of a molecule’s heat of combustion simply by means of paper and pencil, using the presented group parameters in Table 4. As this work is ongoing, the number of compounds for which—based on the same algorithm—up to 17 physical, thermodynamic, solubility-, optics-, charge-, and environment-related descriptors [1,2,3,4,5,6] can be reliably predicted, will steadily increase.
The mentioned software project is called ChemBrain IXL, available from Neuronix Software (www.neuronix.ch, Rudolf Naef, Lupsingen, Switzerland).

Supplementary Materials

The following are available online. The list of compounds used in the present work, their experimental data and 3D structures are available online as standard SDF files, accessible for external chemistry software, under the name of “S01_Compounds List for deltaH°(c) Calculations.sdf”. The list of the compounds used in the correlation diagrams and histograms containing their names and their experimental and calculated values are available under the names of “S02. Experimental vs. calculated deltaH°(c) Data Table.doc” and “S03. Experimental vs. calculated deltaH°(f) Data Table.doc”. In addition, the list of outliers is available under the name “S04. Outliers of deltaH°(c) calculations.xls”. Finally, the figures are available as tif files and the tables as doc files under the names given in the text.

Author Contributions

R.N. developed project ChemBrain and its software upon which this paper is based and also fed the database, calculated and analyzed the results, and wrote the paper. W.E.A.J. suggested the extension of ChemBrain’s tool and contributed experimental data and the majority of the literature references. Beyond this, R.N. is indebted to W.E.A.J. for the many valuable discussions. Both authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The data presented in this study are available in Supplementary Material.

Acknowledgments

R. Naef is indebted to the library of the University of Basel for allowing him full and free access to the electronic literature database.

Conflicts of Interest

The authors declare no conflict of interest.

Sample Availability

Samples of the compounds are not available from the authors.

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Figure 1. Correlation diagram of the heat-of-combustion data in kJ/mol. Cross-validation data are added as red circles. (10-fold cross-validated: N = 4886, Q2 = 1, regression line: intercept = −1.0111; slope = 0.9998).
Figure 1. Correlation diagram of the heat-of-combustion data in kJ/mol. Cross-validation data are added as red circles. (10-fold cross-validated: N = 4886, Q2 = 1, regression line: intercept = −1.0111; slope = 0.9998).
Molecules 26 06101 g001
Figure 2. Histogram of the heat-of-combustion data in kJ/mol. Cross-validation data are superpositioned as red bars. (σ = 18.12; S = 19.16; experimental values range from −35,100 to −98.2).
Figure 2. Histogram of the heat-of-combustion data in kJ/mol. Cross-validation data are superpositioned as red bars. (σ = 18.12; S = 19.16; experimental values range from −35,100 to −98.2).
Molecules 26 06101 g002
Figure 3. Correlation diagram of the heat of formation (in kJ/mol), (N = 4886, R2 = 0.9979, regression line: intercept = −0.5539; slope = 0.9979).
Figure 3. Correlation diagram of the heat of formation (in kJ/mol), (N = 4886, R2 = 0.9979, regression line: intercept = −0.5539; slope = 0.9979).
Molecules 26 06101 g003
Figure 4. Histogram of the heat of formation (in kJ/mol) (σ = 18.14; experimental values range from −7238.2 to +1039.7 kJ/mol).
Figure 4. Histogram of the heat of formation (in kJ/mol) (σ = 18.14; experimental values range from −7238.2 to +1039.7 kJ/mol).
Molecules 26 06101 g004
Table 1. Charged Atom Groups and their Meaning.
Table 1. Charged Atom Groups and their Meaning.
NoAtom TypeNeighborsMeaningExample
1B(-)F4BF4-tetrafluoroborate
2C(-) sp3C3C-C-(C)-Ctricyanomethanide
3C sp2NS=S(-)N-C(=S)-S-dithiocarbamate
4C aromaticH:C:N(+)C:CH:N+C2 in pyridinium
5C(+) aromaticH:N2N:C+(H):NC2 in imidazolium
6C spC#N(-)N#C-C-tricyanomethanide
7C spN#N(-)N#C-N-dicyanoamide
8C sp=N=S(-)N=C=S-Thiocyanate
9N(+) sp3C4NC4+tetraalkylammonium
10N(+) sp2O2=O(-)NO3-nitrate
11N aromaticC2:C(+)(C)(C):C+N1 in 1-alkylimidazolium
12N(+) aromaticC:C(C):N+(C):CN in 1-alkylpyridinium
13N(-)C2C-N--Cdicyanoamide
14S4O2=O2(-)SO4-hydrosulfate
15S4CO=O2(-)C-SO3-methylsulfonate
Table 2. Special Groups and their Meaning.
Table 2. Special Groups and their Meaning.
Atom TypeNeighborsMeaning
HH AcceptorIntramolecular H bridge between acidic H (on O, N or S) and basic acceptor (O, N or F) at distance <1.75 Angstroms
H.HIntramolecular H–H distance <2 Angstroms
H..HIntramolecular H–H distance 2–2.3 Angstroms
Angle60 Bond angle <74 deg
Angle90 Bond angle 74–98 deg
Angle102 Bond angle 98–106 deg
Table 3. Example Calculation of the Standard Heat of Combustion (in kJ/mol) of 4-Methylene-2-oxetanone.
Table 3. Example Calculation of the Standard Heat of Combustion (in kJ/mol) of 4-Methylene-2-oxetanone.
Atom Type
Neighbors
C sp3 H2C2C sp2 H2=CC sp2 C=COC sp2 CO=OO C2(2pi)Angle90Sum
Contribution−653.47−703.3−470.12−256.51278.25−24.51
n Groups111114
N × Contrib.−653.47−703.3−470.12−256.51278.25−98.04−1903.19
Table 5. Calculated ΔH°(c) (in kJ/mol) of Non-ionic and Zwitter-ionic Forms of Amino Acids.
Table 5. Calculated ΔH°(c) (in kJ/mol) of Non-ionic and Zwitter-ionic Forms of Amino Acids.
Molecule nameΔH°c calc
Non-Ionic Form
Diff.ΔH°c calc
Zwitter Form
ΔH°c expReferences
(l)-Alanine−1688.7−64.9−1623.8−1621.0[267,268]
(l)-Cy(l)-Cysteine−2316.2−64.9−2251.3−2263.0[21]
(l)-Cystine−4373.5−132.3−4241.2−4248.0[21]
(l)-Histidine−3230.8−64.9−3165.9−3180.6[275]
(l)-Hydroxyproline−2605.5−37.9−2567.6−2594.1[21]
(l)-Methionine−3626.5−62.3−3564.2−3564.1[266]
2-Aminobutyric acid−2342.1−62.2−2279.9−2254.0[21]
2-Methylalanine−2323.3−54.3−2269.0−2265.9[21]
2-Phenylglycine−4046.5−62.2−3984.3−4005.1[21]
4-Aminobutyric acid−2345.1−57.3−2287.8−2283.9[21]
5-Aminovaleric acid−2998.5−57.3−2941.2−2937.0[21]
8-Aminocaprylic acid−4958.9−57.3−4901.6−4884.0[21]
Asparagine−2000.8−64.8−1936.0−1928.5[265,266,269]
Aspartic acid−1674.0−64.9−1609.1−1602.9[21]
beta-Alanine−1691.6−57.3−1634.3−1622.9[21]
Dopa−4285.5−67.5−4218.0−4177.8[21]
epsilon-Aminocaproic acid−3652.0−57.3−3594.7−3582.2[21]
Glutamic acid−2327.7−62.2−2265.5−2277.0[21]
Glutamine−2654.6−62.3−2592.3−2572.8[265,269]
Glycine−1038.1−57.3−980.8−978.6[268,269]
Isoleucine−3651.0−62.2−3588.8−3583.7[269]
Isoserine−1497.9−57.4−1440.5−1438.2[21]
Leucine−3648.4−64.9−3583.5−3581.2[269]
Norleucine−3649.1−62.3−3586.8−3582.2[21]
N-Phenylglycine−4074.7−40.2−4034.5−4037.6[21]
Phenylalanine−4702.6−67.5−4635.1−4646.3[269]
Proline−2798.9−56.5−2742.4−2746.2[269]
Sarcosine−1716.2−27.4−1688.8−1675.1[270]
Serine−1504.4−64.8−1439.6−1438.9[269]
Threonine−2151.3−62.2−2089.1−2087.1[269,275,277]
Tryptophane−5671.0−64.9−5606.1−5629.4[269,274]
Tyrosine−4494.1−64.9−4429.2−4428.1[269]
Valine−2994.9−62.2−2932.7−2933.9[269]
Table 6. Calculated ΔH°(c) (in kJ/mol) of Azo and Hydrazone Forms of some Azo Dyes.
Table 6. Calculated ΔH°(c) (in kJ/mol) of Azo and Hydrazone Forms of some Azo Dyes.
CompoundHydrazone Form
∆Hc calc
Azo Form
∆Hc calc
∆Hc expaRef.
4-Phenylazophenol−6275.2−6288.0−6314.1+ −[528]
2-Phenylazophenol−6272.3−6287.2-+ −[528]
4-Aminoazobenzene−6651.1−6603.1−6617.4+[529]
2-Aminoazobenzene−6648.4−6602.4 +
1-Phenylazo-2-naphthol−8145.8−8185.1 +[530,531]
4-Phenylazo-1-naphthol−8148.5−8185.4 +[532]
1-Phenylazo-2-naphthylamine−8533.8−8500.3 +[530,531]
4-Phenylazo-1-naphthylamine−8524.6−8503.0 +[533]
a Conformance with experimental data.
Table 7. Calculated and experimental ΔH°(c) (in kJ/mol) of Tautomeric Ketones and β-Diketones.
Table 7. Calculated and experimental ΔH°(c) (in kJ/mol) of Tautomeric Ketones and β-Diketones.
CompoundKeto Form
∆Hc ealc
Enol Form
∆Hc ealc
∆Hc expaRef.
1-(N-Phenylformimidoyl)-2-naphthol−8608.3−8560.3 +[534]
Acetone−1791.0−1798.0−1816.5+[535]
Cyclohexanone−3509.3−3497.6−3517.6[535]
Cyclopentanone−2865.1−2858.1−2873.5[536]
Phenol−3149.4−3055.4−3055.5+[537]
2-Pyridone−2557.4−2513.2−2517.62[538,539,540]
4-Pyridone−2573.8−2564.2−2537.5+[538,539,540]
Carbostyril−4461.4−4413.7−4397.1[541,542,543]
Acetylacetone−2686.5−2674.5−2687.0+[544]
Bis(trifluoroacetyl)methane−1640.7−1628.7−1673.7+[544]
Dibenzoylmethane−7404.8−7394.1−7398.5+[544]
1,1-Bis(benzoyl)ethane−8057.6−8036.1 [544]
a Conformance with experimental data.
Table 8. Calculated and experimental ΔH°(c) (in kJ/mol) of some Ionic Liquids.
Table 8. Calculated and experimental ΔH°(c) (in kJ/mol) of some Ionic Liquids.
Molecule NameΔH°c expΔH°c calcDeviationDev. in %
1,1,3,3-Tetramethylguanidinium nitrate−3656.5−3656.50.00.00
1-Butyl-1-methylpyrrolidinium dicyanamide−7244.8−7250.15.3−0.07
1-Butyl-3-methylimidazolium chloride−5232.3−5206.6−25.70.49
1-Butyl-3-methylimidazolium dicyanoamide−6273.9−6271.6−2.30.04
1-Butyl-3-methylimidazolium nitrate−5013.2−5017.84.6−0.09
1-Decyl-3-methylimidazolium bromide−9105.2−9127.422.2−0.24
1-Dodecyl-3-methylimidazolium bromide−10,406.0−10,434.428.4−0.27
1-Ethanol-3-methyl-imidazolium dicyanoamide−4793.0−4780.7−12.30.26
1-Ethyl-3-methylimidazolium chloride−3886.2−3899.713.5−0.35
1-Ethyl-3-methylimidazolium dicyanamide−4955.4−4964.79.3−0.19
1-Ethyl-3-methylimidazolium nitrate−3697.5−3710.913.4−0.36
1-Methyl-3-pentylimidazolium chloride−5904.3−5860.1−44.20.75
1-Octyl-3-methylimidazolium bromide−7837.8−7820.5−17.30.22
1-Tetradecyl-3-methylimidazolium bromide−11,718.0−11,741.323.3−0.20
6,6-(Tetramethylene-3′-oxa)-7a-(nitroxymethyl)-3-oxoperhydroimidazo [1,5-c]oxazol-6-ium nitrate−5384.8−5376.5−8.30.15
6,6-(Tetramethylene-3′-oxa)-7a-methyl-3-oxoperhydroimidazo [1,5-c]oxazol-6-ium nitrate−5587.5−5604.817.3−0.31
6,6-Pentamethylene-7a-(nitroxymethyl)-3-oxoperhydroimidazo[1,5-c]oxazol-6-ium nitrate−6166.4−6159.0−7.40.12
Diethylammonium diethyldithiocarbamate−7639.6−7650.010.4−0.14
Diisobutylammonium diisobutyldithiocarbamate−12,891.0−12,868.4−22.60.18
Diisopropylammonium diisopropyldithiocarbamate−10,260.0−10,252.6−7.40.07
Dipropylammonium dipropyldithiocarbamate−10,252.0−10,271.719.7−0.19
N,N-Dimethylglycine bisulfate−2610.6−2604.7−5.90.23
N,N-Dimethylglycine methyl ester bisulfate−3323.2−3329.15.9−0.18
N,N-Dimethylglycine methyl ester sulfate−6765.2−6790.225.0−0.37
N,N-Dimethylglycine sulfate−5371.6−5346.6−25.00.47
Tetraethylammonium nitrate−5573.4−5590.617.2−0.31
Tetramethylammonium nitrate−2960.5−2958.5−2.00.07
Tetra-n-butylammonium nitrate−10,841.0−10,818.4−22.60.21
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Naef, R.; Acree, W.E., Jr. Revision and Extension of a Generally Applicable Group-Additivity Method for the Calculation of the Standard Heat of Combustion and Formation of Organic Molecules. Molecules 2021, 26, 6101. https://doi.org/10.3390/molecules26206101

AMA Style

Naef R, Acree WE Jr. Revision and Extension of a Generally Applicable Group-Additivity Method for the Calculation of the Standard Heat of Combustion and Formation of Organic Molecules. Molecules. 2021; 26(20):6101. https://doi.org/10.3390/molecules26206101

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Naef, Rudolf, and William E. Acree, Jr. 2021. "Revision and Extension of a Generally Applicable Group-Additivity Method for the Calculation of the Standard Heat of Combustion and Formation of Organic Molecules" Molecules 26, no. 20: 6101. https://doi.org/10.3390/molecules26206101

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