Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -191.856194 |
| Energy at 298.15K | |
| HF Energy | -191.599146 |
| Nuclear repulsion energy | 103.313938 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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' |
3250 |
3118 |
3.55 |
65.09 |
0.48 |
0.64 |
| 2 |
A' |
3203 |
3072 |
0.69 |
102.99 |
0.27 |
0.43 |
| 3 |
A' |
3159 |
3030 |
4.45 |
80.41 |
0.08 |
0.14 |
| 4 |
A' |
2918 |
2799 |
83.24 |
110.72 |
0.26 |
0.41 |
| 5 |
A' |
1750 |
1679 |
237.42 |
94.53 |
0.35 |
0.51 |
| 6 |
A' |
1676 |
1607 |
3.43 |
31.11 |
0.09 |
0.16 |
| 7 |
A' |
1466 |
1406 |
10.35 |
6.29 |
0.44 |
0.61 |
| 8 |
A' |
1395 |
1338 |
5.32 |
22.22 |
0.27 |
0.42 |
| 9 |
A' |
1306 |
1253 |
2.80 |
11.39 |
0.14 |
0.25 |
| 10 |
A' |
1181 |
1133 |
39.37 |
13.05 |
0.61 |
0.75 |
| 11 |
A' |
928 |
890 |
19.32 |
1.54 |
0.00 |
0.01 |
| 12 |
A' |
573 |
550 |
4.12 |
6.29 |
0.16 |
0.28 |
| 13 |
A' |
322 |
309 |
10.37 |
1.04 |
0.31 |
0.47 |
| 14 |
A" |
1043 |
1000 |
8.39 |
0.46 |
0.75 |
0.86 |
| 15 |
A" |
1034 |
992 |
8.88 |
1.60 |
0.75 |
0.86 |
| 16 |
A" |
1005 |
964 |
38.64 |
2.63 |
0.75 |
0.86 |
| 17 |
A" |
620 |
594 |
10.24 |
0.66 |
0.75 |
0.86 |
| 18 |
A" |
170 |
163 |
4.59 |
0.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13499.7 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 12947.6 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.149 |
-0.741 |
0.000 |
| C2 |
0.000 |
0.719 |
0.000 |
| C3 |
1.210 |
1.279 |
0.000 |
| O4 |
-1.214 |
-1.320 |
0.000 |
| H5 |
0.803 |
-1.303 |
0.000 |
| H6 |
-0.909 |
1.304 |
0.000 |
| H7 |
1.348 |
2.349 |
0.000 |
| H8 |
2.100 |
0.665 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4675 | 2.4337 | 1.2123 | 1.1055 | 2.1810 | 3.4326 | 2.6522 |
C2 | 1.4675 | | 1.3327 | 2.3732 | 2.1758 | 1.0803 | 2.1145 | 2.1011 | C3 | 2.4337 | 1.3327 | | 3.5533 | 2.6133 | 2.1186 | 1.0788 | 1.0817 | O4 | 1.2123 | 2.3732 | 3.5533 | | 2.0167 | 2.6414 | 4.4744 | 3.8630 | H5 | 1.1055 | 2.1758 | 2.6133 | 2.0167 | | 3.1184 | 3.6918 | 2.3569 | H6 | 2.1810 | 1.0803 | 2.1186 | 2.6414 | 3.1184 | | 2.4867 | 3.0762 | H7 | 3.4326 | 2.1145 | 1.0788 | 4.4744 | 3.6918 | 2.4867 | | 1.8442 | H8 | 2.6522 | 2.1011 | 1.0817 | 3.8630 | 2.3569 | 3.0762 | 1.8442 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
120.630 |
|
C1 |
C2 |
H6 |
116.923 |
| C2 |
C1 |
O4 |
124.377 |
|
C2 |
C1 |
H5 |
114.751 |
| C2 |
C3 |
H7 |
122.170 |
|
C2 |
C3 |
H8 |
120.618 |
| C3 |
C2 |
H6 |
122.447 |
|
O4 |
C1 |
H5 |
120.872 |
| H7 |
C3 |
H8 |
117.211 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.008 |
|
|
|
| 2 |
C |
-0.067 |
|
|
|
| 3 |
C |
-0.887 |
|
|
|
| 4 |
O |
-0.588 |
|
|
|
| 5 |
H |
0.456 |
|
|
|
| 6 |
H |
0.377 |
|
|
|
| 7 |
H |
0.447 |
|
|
|
| 8 |
H |
0.269 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
2.571 |
2.168 |
0.000 |
3.363 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.003 |
-2.746 |
-0.006 |
| y |
-2.746 |
-24.375 |
-0.007 |
| z |
-0.006 |
-0.007 |
-25.208 |
|
| Traceless |
| | x | y | z |
| x |
-0.211 |
-2.746 |
-0.006 |
| y |
-2.746 |
0.730 |
-0.007 |
| z |
-0.006 |
-0.007 |
-0.519 |
|
| Polar |
| 3z2-r2 | -1.038 |
| x2-y2 | -0.628 |
| xy | -2.746 |
| xz | -0.006 |
| yz | -0.007 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.697 |
1.727 |
0.001 |
| y |
1.727 |
7.270 |
0.001 |
| z |
0.001 |
0.001 |
4.223 |
<r2> (average value of r
2) Å
2
| <r2> |
83.424 |
| (<r2>)1/2 |
9.134 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -191.852516 |
| Energy at 298.15K | |
| HF Energy | -191.595331 |
| Nuclear repulsion energy | 104.790248 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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' |
3261 |
3127 |
1.24 |
53.00 |
0.59 |
0.74 |
| 2 |
A' |
3191 |
3061 |
9.36 |
140.06 |
0.19 |
0.32 |
| 3 |
A' |
3167 |
3038 |
4.62 |
54.14 |
0.12 |
0.22 |
| 4 |
A' |
2945 |
2824 |
126.13 |
176.53 |
0.28 |
0.44 |
| 5 |
A' |
1757 |
1685 |
95.83 |
16.16 |
0.65 |
0.79 |
| 6 |
A' |
1665 |
1597 |
75.76 |
71.09 |
0.14 |
0.25 |
| 7 |
A' |
1449 |
1390 |
42.66 |
7.80 |
0.46 |
0.63 |
| 8 |
A' |
1434 |
1375 |
1.29 |
10.25 |
0.11 |
0.20 |
| 9 |
A' |
1321 |
1267 |
2.67 |
21.33 |
0.25 |
0.39 |
| 10 |
A' |
1076 |
1032 |
3.79 |
3.42 |
0.68 |
0.81 |
| 11 |
A' |
939 |
900 |
61.53 |
6.37 |
0.07 |
0.13 |
| 12 |
A' |
684 |
656 |
12.09 |
0.67 |
0.75 |
0.86 |
| 13 |
A' |
286 |
275 |
6.86 |
3.39 |
0.31 |
0.47 |
| 14 |
A" |
1047 |
1004 |
4.93 |
3.48 |
0.75 |
0.86 |
| 15 |
A" |
1031 |
989 |
33.57 |
0.55 |
0.75 |
0.86 |
| 16 |
A" |
1018 |
976 |
9.69 |
1.36 |
0.75 |
0.86 |
| 17 |
A" |
566 |
543 |
10.20 |
0.74 |
0.75 |
0.86 |
| 18 |
A" |
146 |
140 |
6.51 |
0.23 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 13490.8 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 12939.1 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.885 |
-0.291 |
0.000 |
| C2 |
0.000 |
0.893 |
0.000 |
| C3 |
1.327 |
0.779 |
0.000 |
| O4 |
-0.495 |
-1.440 |
0.000 |
| H5 |
-1.966 |
-0.074 |
0.000 |
| H6 |
-0.480 |
1.862 |
0.000 |
| H7 |
1.970 |
1.645 |
0.000 |
| H8 |
1.786 |
-0.199 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.4788 | 2.4577 | 1.2127 | 1.1028 | 2.1907 | 3.4501 | 2.6727 |
C2 | 1.4788 | | 1.3322 | 2.3851 | 2.1910 | 1.0810 | 2.1088 | 2.0936 | C3 | 2.4577 | 1.3322 | | 2.8713 | 3.4020 | 2.1071 | 1.0788 | 1.0803 | O4 | 1.2127 | 2.3851 | 2.8713 | | 2.0075 | 3.3014 | 3.9492 | 2.5969 | H5 | 1.1028 | 2.1910 | 3.4020 | 2.0075 | | 2.4397 | 4.2953 | 3.7543 | H6 | 2.1907 | 1.0810 | 2.1071 | 3.3014 | 2.4397 | | 2.4602 | 3.0632 | H7 | 3.4501 | 2.1088 | 1.0788 | 3.9492 | 4.2953 | 2.4602 | | 1.8535 | H8 | 2.6727 | 2.0936 | 1.0803 | 2.5969 | 3.7543 | 3.0632 | 1.8535 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
121.840 |
|
C1 |
C2 |
H6 |
116.848 |
| C2 |
C1 |
O4 |
124.489 |
|
C2 |
C1 |
H5 |
115.371 |
| C2 |
C3 |
H7 |
121.658 |
|
C2 |
C3 |
H8 |
120.054 |
| C3 |
C2 |
H6 |
121.312 |
|
O4 |
C1 |
H5 |
120.140 |
| H7 |
C3 |
H8 |
118.289 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.086 |
|
|
|
| 2 |
C |
-0.054 |
|
|
|
| 3 |
C |
-0.791 |
|
|
|
| 4 |
O |
-0.616 |
|
|
|
| 5 |
H |
0.462 |
|
|
|
| 6 |
H |
0.358 |
|
|
|
| 7 |
H |
0.389 |
|
|
|
| 8 |
H |
0.336 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.205 |
2.755 |
0.000 |
2.763 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.550 |
-0.691 |
-0.004 |
| y |
-0.691 |
-26.796 |
-0.007 |
| z |
-0.004 |
-0.007 |
-25.180 |
|
| Traceless |
| | x | y | z |
| x |
5.438 |
-0.691 |
-0.004 |
| y |
-0.691 |
-3.931 |
-0.007 |
| z |
-0.004 |
-0.007 |
-1.507 |
|
| Polar |
| 3z2-r2 | -3.014 |
| x2-y2 | 6.246 |
| xy | -0.691 |
| xz | -0.004 |
| yz | -0.007 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.784 |
0.612 |
0.000 |
| y |
0.612 |
6.665 |
0.002 |
| z |
0.000 |
0.002 |
4.208 |
<r2> (average value of r
2) Å
2
| <r2> |
75.239 |
| (<r2>)1/2 |
8.674 |