Jump to
S1C2
Energy calculated at B1B95/6-31G
| hartrees |
Energy at 0K | -231.023434 |
Energy at 298.15K | -231.029221 |
Nuclear repulsion energy | 157.655527 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/6-31G
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
3321 |
3168 |
8.64 |
|
|
|
2 |
A1 |
3224 |
3075 |
2.68 |
|
|
|
3 |
A1 |
3189 |
3041 |
29.64 |
|
|
|
4 |
A1 |
1777 |
1695 |
5.21 |
|
|
|
5 |
A1 |
1472 |
1403 |
0.31 |
|
|
|
6 |
A1 |
1393 |
1328 |
5.28 |
|
|
|
7 |
A1 |
1196 |
1140 |
18.26 |
|
|
|
8 |
A1 |
853 |
813 |
1.66 |
|
|
|
9 |
A1 |
517 |
493 |
0.29 |
|
|
|
10 |
A1 |
226 |
216 |
0.13 |
|
|
|
11 |
A2 |
989 |
943 |
0.00 |
|
|
|
12 |
A2 |
917 |
875 |
0.00 |
|
|
|
13 |
A2 |
719 |
686 |
0.00 |
|
|
|
14 |
A2 |
109 |
104 |
0.00 |
|
|
|
15 |
B1 |
1001 |
955 |
46.67 |
|
|
|
16 |
B1 |
921 |
878 |
156.19 |
|
|
|
17 |
B1 |
690 |
658 |
3.36 |
|
|
|
18 |
B1 |
89 |
85 |
4.05 |
|
|
|
19 |
B2 |
3321 |
3168 |
3.56 |
|
|
|
20 |
B2 |
3224 |
3074 |
0.35 |
|
|
|
21 |
B2 |
3184 |
3037 |
5.09 |
|
|
|
22 |
B2 |
1726 |
1646 |
381.55 |
|
|
|
23 |
B2 |
1457 |
1390 |
36.43 |
|
|
|
24 |
B2 |
1360 |
1297 |
2.37 |
|
|
|
25 |
B2 |
1215 |
1159 |
421.46 |
|
|
|
26 |
B2 |
1046 |
998 |
15.23 |
|
|
|
27 |
B2 |
483 |
460 |
5.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19808.2 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 18891.1 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/6-31G
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
0.000 |
0.000 |
0.322 |
C2 |
0.000 |
1.196 |
-0.383 |
C3 |
0.000 |
-1.196 |
-0.383 |
C4 |
0.000 |
2.367 |
0.245 |
C5 |
0.000 |
-2.367 |
0.245 |
H6 |
0.000 |
1.090 |
-1.465 |
H7 |
0.000 |
-1.090 |
-1.465 |
H8 |
0.000 |
3.288 |
-0.321 |
H9 |
0.000 |
2.426 |
1.325 |
H10 |
0.000 |
-3.288 |
-0.321 |
H11 |
0.000 |
-2.426 |
1.325 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
O1 | | 1.3877 | 1.3877 | 2.3680 | 2.3680 | 2.0927 | 2.0927 | 3.3500 | 2.6253 | 3.3500 | 2.6253 |
C2 | 1.3877 | | 2.3911 | 1.3289 | 3.6172 | 1.0872 | 2.5285 | 2.0932 | 2.1050 | 4.4837 | 4.0041 | C3 | 1.3877 | 2.3911 | | 3.6172 | 1.3289 | 2.5285 | 1.0872 | 4.4837 | 4.0041 | 2.0932 | 2.1050 | C4 | 2.3680 | 1.3289 | 3.6172 | | 4.7336 | 2.1340 | 3.8563 | 1.0810 | 1.0818 | 5.6828 | 4.9130 | C5 | 2.3680 | 3.6172 | 1.3289 | 4.7336 | | 3.8563 | 2.1340 | 5.6828 | 4.9130 | 1.0810 | 1.0818 | H6 | 2.0927 | 1.0872 | 2.5285 | 2.1340 | 3.8563 | | 2.1794 | 2.4779 | 3.0934 | 4.5245 | 4.4882 | H7 | 2.0927 | 2.5285 | 1.0872 | 3.8563 | 2.1340 | 2.1794 | | 4.5245 | 4.4882 | 2.4779 | 3.0934 | H8 | 3.3500 | 2.0932 | 4.4837 | 1.0810 | 5.6828 | 2.4779 | 4.5245 | | 1.8580 | 6.5756 | 5.9462 | H9 | 2.6253 | 2.1050 | 4.0041 | 1.0818 | 4.9130 | 3.0934 | 4.4882 | 1.8580 | | 5.9462 | 4.8521 | H10 | 3.3500 | 4.4837 | 2.0932 | 5.6828 | 1.0810 | 4.5245 | 2.4779 | 6.5756 | 5.9462 | | 1.8580 | H11 | 2.6253 | 4.0041 | 2.1050 | 4.9130 | 1.0818 | 4.4882 | 3.0934 | 5.9462 | 4.8521 | 1.8580 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C4 |
121.297 |
|
O1 |
C2 |
H6 |
114.928 |
O1 |
C3 |
C5 |
121.297 |
|
O1 |
C3 |
H7 |
114.928 |
C2 |
O1 |
C3 |
118.972 |
|
C2 |
C4 |
H8 |
120.240 |
C2 |
C4 |
H9 |
121.329 |
|
C3 |
C5 |
H10 |
120.240 |
C3 |
C5 |
H11 |
121.329 |
|
C4 |
C2 |
H6 |
123.775 |
C5 |
C3 |
H7 |
123.775 |
|
H8 |
C4 |
H9 |
118.431 |
H10 |
C5 |
H11 |
118.431 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.541 |
|
|
|
2 |
C |
0.165 |
|
|
|
3 |
C |
0.165 |
|
|
|
4 |
C |
-0.371 |
|
|
|
5 |
C |
-0.371 |
|
|
|
6 |
H |
0.156 |
|
|
|
7 |
H |
0.156 |
|
|
|
8 |
H |
0.154 |
|
|
|
9 |
H |
0.167 |
|
|
|
10 |
H |
0.154 |
|
|
|
11 |
H |
0.167 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
-1.610 |
1.610 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-33.423 |
0.000 |
0.000 |
y |
0.000 |
-26.152 |
0.000 |
z |
0.000 |
0.000 |
-27.407 |
|
Traceless |
| x | y | z |
x |
-6.643 |
0.000 |
0.000 |
y |
0.000 |
4.263 |
0.000 |
z |
0.000 |
0.000 |
2.380 |
|
Polar |
3z2-r2 | 4.759 |
x2-y2 | -7.271 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.371 |
0.000 |
0.000 |
y |
0.000 |
12.341 |
0.000 |
z |
0.000 |
0.000 |
6.109 |
<r2> (average value of r
2) Å
2
<r2> |
149.563 |
(<r2>)1/2 |
12.230 |
Jump to
S1C1
Energy calculated at B1B95/6-31G
| hartrees |
Energy at 0K | -231.020461 |
Energy at 298.15K | -231.026507 |
HF Energy | -231.020461 |
Nuclear repulsion energy | 160.305622 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/6-31G
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A |
3328 |
3174 |
6.61 |
|
|
|
2 |
A |
3323 |
3169 |
12.25 |
|
|
|
3 |
A |
3281 |
3129 |
7.03 |
|
|
|
4 |
A |
3233 |
3084 |
2.83 |
|
|
|
5 |
A |
3227 |
3078 |
2.42 |
|
|
|
6 |
A |
3210 |
3061 |
7.75 |
|
|
|
7 |
A |
1755 |
1673 |
100.06 |
|
|
|
8 |
A |
1722 |
1643 |
139.42 |
|
|
|
9 |
A |
1471 |
1403 |
1.29 |
|
|
|
10 |
A |
1460 |
1392 |
13.94 |
|
|
|
11 |
A |
1384 |
1320 |
32.93 |
|
|
|
12 |
A |
1355 |
1293 |
4.81 |
|
|
|
13 |
A |
1248 |
1190 |
289.04 |
|
|
|
14 |
A |
1145 |
1092 |
12.78 |
|
|
|
15 |
A |
1026 |
979 |
42.34 |
|
|
|
16 |
A |
1020 |
973 |
5.08 |
|
|
|
17 |
A |
1013 |
966 |
36.50 |
|
|
|
18 |
A |
944 |
900 |
74.96 |
|
|
|
19 |
A |
926 |
883 |
87.49 |
|
|
|
20 |
A |
863 |
823 |
9.93 |
|
|
|
21 |
A |
739 |
705 |
3.77 |
|
|
|
22 |
A |
721 |
688 |
1.38 |
|
|
|
23 |
A |
591 |
564 |
2.37 |
|
|
|
24 |
A |
444 |
424 |
3.50 |
|
|
|
25 |
A |
262 |
250 |
2.49 |
|
|
|
26 |
A |
205 |
196 |
10.92 |
|
|
|
27 |
A |
92 |
88 |
0.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19994.7 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 19069.0 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/6-31G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
O1 |
-0.047 |
-0.780 |
0.048 |
C2 |
1.310 |
-0.501 |
0.012 |
C3 |
-0.950 |
0.252 |
0.285 |
C4 |
1.870 |
0.696 |
-0.148 |
C5 |
-2.189 |
0.199 |
-0.187 |
H6 |
1.870 |
-1.418 |
0.124 |
H7 |
-0.567 |
1.047 |
0.916 |
H8 |
2.946 |
0.787 |
-0.148 |
H9 |
1.296 |
1.600 |
-0.304 |
H10 |
-2.903 |
0.970 |
0.066 |
H11 |
-2.516 |
-0.617 |
-0.817 |
Atom - Atom Distances (Å)
|
O1 |
C2 |
C3 |
C4 |
C5 |
H6 |
H7 |
H8 |
H9 |
H10 |
H11 |
O1 | | 1.3862 | 1.3916 | 2.4274 | 2.3671 | 2.0218 | 2.0888 | 3.3841 | 2.7559 | 3.3495 | 2.6212 |
C2 | 1.3862 | | 2.3979 | 1.3315 | 3.5746 | 1.0801 | 2.5959 | 2.0882 | 2.1253 | 4.4630 | 3.9168 | C3 | 1.3916 | 2.3979 | | 2.8868 | 1.3271 | 3.2813 | 1.0851 | 3.9561 | 2.6851 | 2.0923 | 2.1025 | C4 | 2.4274 | 1.3315 | 2.8868 | | 4.0895 | 2.1322 | 2.6816 | 1.0803 | 1.0817 | 4.7850 | 4.6265 | C5 | 2.3671 | 3.5746 | 1.3271 | 4.0895 | | 4.3806 | 2.1371 | 5.1691 | 3.7586 | 1.0805 | 1.0812 | H6 | 2.0218 | 1.0801 | 3.2813 | 2.1322 | 4.3806 | | 3.5559 | 2.4687 | 3.1023 | 5.3373 | 4.5568 | H7 | 2.0888 | 2.5959 | 1.0851 | 2.6816 | 2.1371 | 3.5559 | | 3.6797 | 2.2950 | 2.4869 | 3.0935 | H8 | 3.3841 | 2.0882 | 3.9561 | 1.0803 | 5.1691 | 2.4687 | 3.6797 | | 1.8461 | 5.8556 | 5.6790 | H9 | 2.7559 | 2.1253 | 2.6851 | 1.0817 | 3.7586 | 3.1023 | 2.2950 | 1.8461 | | 4.2622 | 4.4396 | H10 | 3.3495 | 4.4630 | 2.0923 | 4.7850 | 1.0805 | 5.3373 | 2.4869 | 5.8556 | 4.2622 | | 1.8564 | H11 | 2.6212 | 3.9168 | 2.1025 | 4.6265 | 1.0812 | 4.5568 | 3.0935 | 5.6790 | 4.4396 | 1.8564 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
O1 |
C2 |
C4 |
126.536 |
|
O1 |
C2 |
H6 |
109.502 |
O1 |
C3 |
C5 |
121.059 |
|
O1 |
C3 |
H7 |
114.429 |
C2 |
O1 |
C3 |
119.369 |
|
C2 |
C4 |
H8 |
119.587 |
C2 |
C4 |
H9 |
123.122 |
|
C3 |
C5 |
H10 |
120.347 |
C3 |
C5 |
H11 |
121.288 |
|
C4 |
C2 |
H6 |
123.959 |
C5 |
C3 |
H7 |
124.432 |
|
H8 |
C4 |
H9 |
117.274 |
H10 |
C5 |
H11 |
118.360 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
O |
-0.548 |
|
|
|
2 |
C |
0.141 |
|
|
|
3 |
C |
0.141 |
|
|
|
4 |
C |
-0.376 |
|
|
|
5 |
C |
-0.358 |
|
|
|
6 |
H |
0.180 |
|
|
|
7 |
H |
0.170 |
|
|
|
8 |
H |
0.160 |
|
|
|
9 |
H |
0.162 |
|
|
|
10 |
H |
0.157 |
|
|
|
11 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.432 |
1.060 |
0.285 |
1.180 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.911 |
-1.805 |
0.570 |
y |
-1.805 |
-29.412 |
0.907 |
z |
0.570 |
0.907 |
-32.183 |
|
Traceless |
| x | y | z |
x |
4.887 |
-1.805 |
0.570 |
y |
-1.805 |
-0.365 |
0.907 |
z |
0.570 |
0.907 |
-4.522 |
|
Polar |
3z2-r2 | -9.043 |
x2-y2 | 3.501 |
xy | -1.805 |
xz | 0.570 |
yz | 0.907 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
10.325 |
0.408 |
0.639 |
y |
0.408 |
6.106 |
0.295 |
z |
0.639 |
0.295 |
3.169 |
<r2> (average value of r
2) Å
2
<r2> |
132.617 |
(<r2>)1/2 |
11.516 |