Jump to
S1C2
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -188.110304 |
| Energy at 298.15K | |
| HF Energy | -188.110304 |
| Nuclear repulsion energy | 86.925470 |
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/STO-3G
| 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 |
3340 |
2949 |
6.11 |
89.96 |
0.13 |
0.23 |
| 2 |
A1 |
2450 |
2164 |
375.67 |
24.69 |
0.33 |
0.49 |
| 3 |
A1 |
1887 |
1667 |
5.43 |
1.40 |
0.74 |
0.85 |
| 4 |
A1 |
1603 |
1415 |
0.64 |
24.19 |
0.68 |
0.81 |
| 5 |
A1 |
965 |
852 |
0.48 |
25.49 |
0.31 |
0.47 |
| 6 |
B1 |
1031 |
911 |
13.26 |
0.00 |
0.75 |
0.86 |
| 7 |
B1 |
630 |
556 |
7.40 |
2.73 |
0.75 |
0.86 |
| 8 |
B1 |
230 |
203 |
0.01 |
1.85 |
0.75 |
0.86 |
| 9 |
B2 |
3470 |
3064 |
0.06 |
69.85 |
0.75 |
0.86 |
| 10 |
B2 |
1136 |
1003 |
0.82 |
0.00 |
0.75 |
0.86 |
| 11 |
B2 |
378 |
333 |
8.73 |
0.61 |
0.75 |
0.86 |
| 12 |
B2 |
44i |
39i |
9.88 |
0.26 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8537.5 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 7538.6 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 B1B95/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.890 |
| C2 |
0.000 |
0.000 |
-0.572 |
| C3 |
0.000 |
0.000 |
0.711 |
| O4 |
0.000 |
0.000 |
1.936 |
| H5 |
0.000 |
0.928 |
-2.489 |
| H6 |
0.000 |
-0.928 |
-2.489 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3180 | 2.6012 | 3.8261 | 1.1041 | 1.1041 |
C2 | 1.3180 | | 1.2832 | 2.5081 | 2.1293 | 2.1293 | C3 | 2.6012 | 1.2832 | | 1.2249 | 3.3315 | 3.3315 | O4 | 3.8261 | 2.5081 | 1.2249 | | 4.5208 | 4.5208 | H5 | 1.1041 | 2.1293 | 3.3315 | 4.5208 | | 1.8556 | H6 | 1.1041 | 2.1293 | 3.3315 | 4.5208 | 1.8556 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
180.000 |
|
C2 |
C1 |
H5 |
122.827 |
| C2 |
C1 |
H6 |
122.827 |
|
C2 |
C3 |
O4 |
180.000 |
| H5 |
C1 |
H6 |
114.346 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.118 |
|
|
|
| 2 |
C |
-0.090 |
|
|
|
| 3 |
C |
0.139 |
|
|
|
| 4 |
O |
-0.123 |
|
|
|
| 5 |
H |
0.096 |
|
|
|
| 6 |
H |
0.096 |
|
|
|
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 |
-1.488 |
1.488 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.275 |
0.000 |
0.000 |
| y |
0.000 |
-20.301 |
0.000 |
| z |
0.000 |
0.000 |
-19.938 |
|
| Traceless |
| | x | y | z |
| x |
-0.156 |
0.000 |
0.000 |
| y |
0.000 |
-0.195 |
0.000 |
| z |
0.000 |
0.000 |
0.351 |
|
| Polar |
| 3z2-r2 | 0.701 |
| x2-y2 | 0.026 |
| 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 |
0.643 |
0.000 |
0.000 |
| y |
0.000 |
1.130 |
0.000 |
| z |
0.000 |
0.000 |
7.240 |
<r2> (average value of r
2) Å
2
| <r2> |
83.123 |
| (<r2>)1/2 |
9.117 |
Jump to
S1C1
Energy calculated at B1B95/STO-3G
| | hartrees |
| Energy at 0K | -188.110318 |
| Energy at 298.15K | |
| HF Energy | -188.110318 |
| Nuclear repulsion energy | 86.937241 |
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/STO-3G
| 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' |
3473 |
3067 |
0.15 |
69.15 |
0.74 |
0.85 |
| 2 |
A' |
3342 |
2951 |
6.54 |
87.12 |
0.13 |
0.23 |
| 3 |
A' |
2428 |
2144 |
367.34 |
25.44 |
0.33 |
0.50 |
| 4 |
A' |
1885 |
1664 |
7.03 |
1.29 |
0.72 |
0.84 |
| 5 |
A' |
1602 |
1414 |
0.83 |
24.20 |
0.68 |
0.81 |
| 6 |
A' |
1133 |
1001 |
2.06 |
0.27 |
0.15 |
0.25 |
| 7 |
A' |
968 |
854 |
0.34 |
24.63 |
0.29 |
0.45 |
| 8 |
A' |
383 |
338 |
8.64 |
0.81 |
0.67 |
0.80 |
| 9 |
A' |
64 |
57 |
10.06 |
0.86 |
0.75 |
0.86 |
| 10 |
A" |
1030 |
910 |
13.48 |
0.03 |
0.75 |
0.86 |
| 11 |
A" |
643 |
567 |
6.66 |
2.96 |
0.75 |
0.86 |
| 12 |
A" |
235 |
208 |
0.09 |
2.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 8592.5 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 7587.2 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/STO-3G
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.402 |
-1.841 |
0.000 |
| C2 |
0.000 |
-0.584 |
0.000 |
| C3 |
-0.120 |
0.698 |
0.000 |
| O4 |
-0.357 |
1.898 |
0.000 |
| H5 |
1.467 |
-2.133 |
0.000 |
| H6 |
-0.303 |
-2.689 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
O4 |
H5 |
H6 |
| C1 | | 1.3192 | 2.5913 | 3.8154 | 1.1045 | 1.1032 |
C2 | 1.3192 | | 1.2874 | 2.5082 | 2.1333 | 2.1266 | C3 | 2.5913 | 1.2874 | | 1.2242 | 3.2449 | 3.3916 | O4 | 3.8154 | 2.5082 | 1.2242 | | 4.4249 | 4.5878 | H5 | 1.1045 | 2.1333 | 3.2449 | 4.4249 | | 1.8557 | H6 | 1.1032 | 2.1266 | 3.3916 | 4.5878 | 1.8557 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
167.586 |
|
C2 |
C1 |
H5 |
123.081 |
| C2 |
C1 |
H6 |
122.522 |
|
C2 |
C3 |
O4 |
174.130 |
| H5 |
C1 |
H6 |
114.397 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.119 |
|
|
|
| 2 |
C |
-0.090 |
|
|
|
| 3 |
C |
0.140 |
|
|
|
| 4 |
O |
-0.123 |
|
|
|
| 5 |
H |
0.095 |
|
|
|
| 6 |
H |
0.097 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.504 |
-1.384 |
0.000 |
1.473 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.241 |
-0.284 |
0.000 |
| y |
-0.284 |
-20.036 |
0.000 |
| z |
0.000 |
0.000 |
-20.283 |
|
| Traceless |
| | x | y | z |
| x |
-0.081 |
-0.284 |
0.000 |
| y |
-0.284 |
0.226 |
0.000 |
| z |
0.000 |
0.000 |
-0.145 |
|
| Polar |
| 3z2-r2 | -0.289 |
| x2-y2 | -0.204 |
| xy | -0.284 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.379 |
-1.103 |
0.000 |
| y |
-1.103 |
6.988 |
0.000 |
| z |
0.000 |
0.000 |
0.650 |
<r2> (average value of r
2) Å
2
| <r2> |
82.838 |
| (<r2>)1/2 |
9.102 |