Jump to
S1C2
Energy calculated at HF/daug-cc-pVTZ
| hartrees |
Energy at 0K | -153.699175 |
Energy at 298.15K | -153.702539 |
HF Energy | -153.699175 |
Nuclear repulsion energy | 99.876989 |
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 HF/daug-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 |
Ag |
3402 |
3077 |
0.00 |
|
|
|
2 |
Ag |
1746 |
1579 |
0.00 |
|
|
|
3 |
Ag |
1206 |
1091 |
0.00 |
|
|
|
4 |
Ag |
1024 |
927 |
0.00 |
|
|
|
5 |
Au |
1014 |
917 |
0.00 |
|
|
|
6 |
Au |
597 |
540 |
0.00 |
|
|
|
7 |
B1g |
1015 |
918 |
0.00 |
|
|
|
8 |
B1u |
3391 |
3068 |
11.39 |
|
|
|
9 |
B1u |
1767 |
1599 |
15.92 |
|
|
|
10 |
B1u |
1149 |
1039 |
0.01 |
|
|
|
11 |
B2g |
703 |
636 |
0.00 |
|
|
|
12 |
B2u |
3368 |
3047 |
8.81 |
|
|
|
13 |
B2u |
1392 |
1259 |
41.90 |
|
|
|
14 |
B2u |
802 |
725 |
14.55 |
|
|
|
15 |
B3g |
3352 |
3032 |
0.00 |
|
|
|
16 |
B3g |
1298 |
1174 |
0.00 |
|
|
|
17 |
B3g |
923 |
835 |
0.00 |
|
|
|
18 |
B3u |
675 |
611 |
176.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14411.0 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 13036.2 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 HF/daug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.658 |
0.781 |
C2 |
0.000 |
0.658 |
-0.781 |
C3 |
0.000 |
-0.658 |
0.781 |
C4 |
0.000 |
-0.658 |
-0.781 |
H5 |
0.000 |
1.416 |
1.536 |
H6 |
0.000 |
1.416 |
-1.536 |
H7 |
0.000 |
-1.416 |
1.536 |
H8 |
0.000 |
-1.416 |
-1.536 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.5626 | 1.3158 | 2.0428 | 1.0699 | 2.4385 | 2.2070 | 3.1101 |
C2 | 1.5626 | | 2.0428 | 1.3158 | 2.4385 | 1.0699 | 3.1101 | 2.2070 | C3 | 1.3158 | 2.0428 | | 1.5626 | 2.2070 | 3.1101 | 1.0699 | 2.4385 | C4 | 2.0428 | 1.3158 | 1.5626 | | 3.1101 | 2.2070 | 2.4385 | 1.0699 | H5 | 1.0699 | 2.4385 | 2.2070 | 3.1101 | | 3.0728 | 2.8319 | 4.1787 | H6 | 2.4385 | 1.0699 | 3.1101 | 2.2070 | 3.0728 | | 4.1787 | 2.8319 | H7 | 2.2070 | 3.1101 | 1.0699 | 2.4385 | 2.8319 | 4.1787 | | 3.0728 | H8 | 3.1101 | 2.2070 | 2.4385 | 1.0699 | 4.1787 | 2.8319 | 3.0728 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C4 |
90.000 |
|
C1 |
C2 |
H6 |
134.890 |
C1 |
C3 |
C4 |
90.000 |
|
C1 |
C3 |
H7 |
135.110 |
C2 |
C1 |
C3 |
90.000 |
|
C2 |
C1 |
H5 |
134.890 |
C2 |
C4 |
C3 |
90.000 |
|
C3 |
C1 |
H5 |
135.110 |
C4 |
C2 |
H6 |
135.110 |
|
C4 |
C3 |
H7 |
134.890 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.819 |
|
|
|
2 |
C |
-0.819 |
|
|
|
3 |
C |
-0.819 |
|
|
|
4 |
C |
-0.819 |
|
|
|
5 |
H |
0.819 |
|
|
|
6 |
H |
0.819 |
|
|
|
7 |
H |
0.819 |
|
|
|
8 |
H |
0.819 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-27.426 |
0.000 |
0.000 |
y |
0.000 |
-20.637 |
0.000 |
z |
0.000 |
0.000 |
-22.769 |
|
Traceless |
| x | y | z |
x |
-5.724 |
0.000 |
0.000 |
y |
0.000 |
4.461 |
0.000 |
z |
0.000 |
0.000 |
1.263 |
|
Polar |
3z2-r2 | 2.526 |
x2-y2 | -6.789 |
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 |
4.970 |
0.000 |
0.000 |
y |
0.000 |
7.672 |
0.000 |
z |
0.000 |
0.000 |
6.942 |
<r2> (average value of r
2) Å
2
<r2> |
57.247 |
(<r2>)1/2 |
7.566 |
Jump to
S1C1
Energy calculated at HF/daug-cc-pVTZ
| hartrees |
Energy at 0K | -153.648507 |
Energy at 298.15K | |
HF Energy | -153.648507 |
Nuclear repulsion energy | 100.491418 |
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 HF/daug-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 |
Ag |
3474 |
3143 |
0.00 |
|
|
|
2 |
Ag |
3308 |
2993 |
0.00 |
|
|
|
3 |
Ag |
1368 |
1237 |
0.00 |
|
|
|
4 |
Ag |
1033 |
935 |
0.00 |
|
|
|
5 |
B1g |
1218 |
1102 |
0.00 |
|
|
|
6 |
B1u |
3464 |
3134 |
20.33 |
|
|
|
7 |
B1u |
1564 |
1415 |
140.62 |
|
|
|
8 |
B1u |
1026 |
928 |
237.85 |
|
|
|
9 |
B2g |
427i |
387i |
0.00 |
|
|
|
10 |
B2u |
3314 |
2998 |
50.47 |
|
|
|
11 |
B2u |
1399 |
1265 |
174.25 |
|
|
|
12 |
B2u |
1036 |
938 |
27.14 |
|
|
|
13 |
B3g |
7509 |
6792 |
0.00 |
|
|
|
14 |
B3g |
1326 |
1200 |
0.00 |
|
|
|
15 |
B3g |
1139 |
1030 |
0.00 |
|
|
|
16 |
B3u |
1064 |
963 |
3.01 |
|
|
|
17 |
B3u |
601 |
543 |
150.30 |
|
|
|
18 |
B3u |
375i |
339i |
196.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16520.1 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 14944.1 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 HF/daug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.959 |
0.000 |
C2 |
0.000 |
0.000 |
1.052 |
C3 |
0.000 |
0.000 |
-1.052 |
C4 |
0.000 |
-0.959 |
0.000 |
H5 |
0.000 |
2.037 |
0.000 |
H6 |
0.000 |
0.000 |
2.114 |
H7 |
0.000 |
0.000 |
-2.114 |
H8 |
0.000 |
-2.037 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
C4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.4238 | 1.4238 | 1.9182 | 1.0776 | 2.3212 | 2.3212 | 2.9958 |
C2 | 1.4238 | | 2.1046 | 1.4238 | 2.2925 | 1.0615 | 3.1660 | 2.2925 | C3 | 1.4238 | 2.1046 | | 1.4238 | 2.2925 | 3.1660 | 1.0615 | 2.2925 | C4 | 1.9182 | 1.4238 | 1.4238 | | 2.9958 | 2.3212 | 2.3212 | 1.0776 | H5 | 1.0776 | 2.2925 | 2.2925 | 2.9958 | | 2.9353 | 2.9353 | 4.0734 | H6 | 2.3212 | 1.0615 | 3.1660 | 2.3212 | 2.9353 | | 4.2275 | 2.9353 | H7 | 2.3212 | 3.1660 | 1.0615 | 2.3212 | 2.9353 | 4.2275 | | 2.9353 | H8 | 2.9958 | 2.2925 | 2.2925 | 1.0776 | 4.0734 | 2.9353 | 2.9353 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C4 |
84.697 |
|
C1 |
C2 |
H6 |
137.652 |
C1 |
C3 |
C4 |
84.697 |
|
C1 |
C3 |
H7 |
137.652 |
C2 |
C1 |
C3 |
95.303 |
|
C2 |
C1 |
H5 |
132.348 |
C2 |
C4 |
C3 |
95.303 |
|
C3 |
C1 |
H5 |
132.348 |
C4 |
C2 |
H6 |
137.652 |
|
C4 |
C3 |
H7 |
137.652 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/daug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.250 |
|
|
|
2 |
C |
-1.912 |
|
|
|
3 |
C |
-1.912 |
|
|
|
4 |
C |
0.250 |
|
|
|
5 |
H |
0.914 |
|
|
|
6 |
H |
0.749 |
|
|
|
7 |
H |
0.749 |
|
|
|
8 |
H |
0.914 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-28.383 |
0.000 |
0.000 |
y |
0.000 |
-18.000 |
0.000 |
z |
0.000 |
0.000 |
-26.486 |
|
Traceless |
| x | y | z |
x |
-6.140 |
0.000 |
0.000 |
y |
0.000 |
9.435 |
0.000 |
z |
0.000 |
0.000 |
-3.295 |
|
Polar |
3z2-r2 | -6.589 |
x2-y2 | -10.384 |
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 |
6.000 |
0.000 |
0.000 |
y |
0.000 |
7.234 |
0.000 |
z |
0.000 |
0.000 |
9.366 |
<r2> (average value of r
2) Å
2
<r2> |
56.729 |
(<r2>)1/2 |
7.532 |