CH 3 NC to CH 3 CN
Transition state 0 K relative E¼ 173 Product 0 K relative E¼# 120
Ea¼DH{þRT¼DH{þ2.48¼174.0O107.2
107.2, sic120.3120.3, sic1.082
1.090
1.504
1.5031.188
1.223Cs–153.22222 + 0.04951
= –153.17271, rel. E = 236 kJ- 153.22564 + 0.04983
= – 153.17581, rel. E = 233 kJ mol–1
–153.34454 + 0.05474
= –153.28980, rel. E = –71.6 kJ- 153.34692 + 0.05507
= –153.29185, rel. E = –71.7, sic kJ mol–1
–93.12310 + 0.01557- 93.12554 + 0.01520
= – 93.11034, rel. E = 0 kJ mol–1
–93.06713 + 0.01061
= –93.05652, rel. E = 134 kJ- 93.06747 + 0.01063
= – 93.05684, rel. E = 140 kJ mol–1
–93.15452 + 0.01643
= –93.13809, rel. E = -80.3 kJ- 93.15894 + 0.01540
= – 93.14354, rel. E = – 87.2 kJ mol–1
–132.22339 + 0.04191
= –132.18148, rel. E = 168 kJ- 132.22493 + 0.04236
–132.29008 + 0.04450–132.29289 + 0.04463–132.33371 + 0.04466
= –132.28905, rel. E = –114 kJ- 132.33825 + 0.04445
579i
C
C C1.386
1.40696.1
92.2
41.8
43.61.380
1.3892.057
2.01442.144.2
CC 1.478 C
1.4821.4961.50259.2
59.1
60.460.4 CCCD2d1.296
1.313–116.12337 + 0.05303
= –116.07034, rel. E = 0 kJ mol–1- 116.12370 + 0.05321
= – 116.07049, rel. E = 0 kJ mol–1
–116.11229 + 0.05246
= –116.05983, rel. E = 27.6 kJ- 116.11330 + 0.05260
= –116.06070, rel. E = 25.7 kJ mol–1
(rel. E = 70.3 kJ mol–1)
OH
Cs117.7117.5
110.7
110.31.318
1.3371.3471.3690.9490.974HF geom
MP2 geomN C
1.135
1.180
1.468
1.463H OC 1112.6114.0 1.420
1.406 119.2118.41.252
1.2951.2931.234
1.519
1.5212574 i HF freq
2345i MP2 freq1227 i
1310i
H N C
1.0020.9851.1541.187CivC3vC2vC3vCs CivCsC 1H
N1.455
1.4091.155
1.177
50.8
53.077.5
72.8N C H
1.1331.177 1.0591.069N C
1.422
1.426
1.153
1.189
NCC
64.2
65.9 75.875.3
1.174
1.2061.8581.896 1.742
1.753468 i
444i–116.23306 + 0.05430
= –116.17876, rel. E = –285 kJ- 116.23413 + 0.05393
= –116.18020, rel. E = – 288 kJ mol–1
HF optimization–153.31831 + 0.05578
= –153.26253, rel. E = 0 kJ mol–1- 153.32005 + 0.05546
= – 153.26459, rel. E = 0 kJ mol–1
MP2 single point on HF geomMP2 optimizationC548 i(rel. E = 0 kJ mol–1) (rel. E = 294 kJ mol–1) (rel. E = –73.8 kJ mol–1)(rel. E = 0 kJ mol–1) (rel. E = 153 kJ mol–1) (rel. E = –50.4 kJ mol–1)(rel. E = 0 kJ mol–1) (rel. E = 184 kJ mol–1) (rel. E = –86.7 kJ mol–1)
= – 132.18257, rel. E = 173 kJ mol–1 =^ – 132.29380, rel. E =^ – 120 kJ mol–1= –132.24558, rel. E = 0 kJ mol–1
= – 132.24826, rel. E = 0 kJ mol–1= –93.10753, rel. E = 0 kJ mol–1(rel. E = 0 kJ mol–1) (rel. E = –243 kJ mol–1)Fig. 5.21 Calculated geometries and energies for four reactions (most H’s are omitted, for
clarity). The purpose of the figure is the compare the single-point energies with energies from
optimization at a higher level. Geometries are HF/6–31G and MP2/6–31G. Energies are MP2/
6–31G//HF/6–31G (i.e. single-point) with HF ZPE, MP2/6–31G//MP2//6–31G with MP2/
6–31G ZPE, and (only relative energies shown,in parentheses) HF/6–31G//HF/6–31G* with
HF ZPE. Ab initioE(hartrees)þZPE (hartrees)¼corrected ab initioE; relativeE(strictly
speaking, 0 K enthalpy differences):Edifference in hartrees' 2626 ¼kJ mol#^1 ). The ZPEs
shown are the ab initio ZPEs multiplied by 0.9135 (HF) or 0.967 (MP2) [ 80 ]. For a discussion of
experimental measurements on these reactions, see [ 92 ]; available experimental activation and
reaction energies (kJ mol#^1 ) are shown here. Calculations here are by the author
268 5 Ab initio Calculations