Jump to
S1C2
Energy calculated at B1B95/6-31G(2df,p)
| hartrees |
Energy at 0K | -209.060333 |
Energy at 298.15K | -209.066385 |
Nuclear repulsion energy | 117.915124 |
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(2df,p)
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 |
3868 |
3705 |
84.25 |
|
|
|
2 |
A |
3169 |
3035 |
9.97 |
|
|
|
3 |
A |
3115 |
2983 |
15.07 |
|
|
|
4 |
A |
3050 |
2921 |
17.72 |
|
|
|
5 |
A |
1764 |
1690 |
0.77 |
|
|
|
6 |
A |
1477 |
1415 |
9.39 |
|
|
|
7 |
A |
1448 |
1386 |
13.51 |
|
|
|
8 |
A |
1390 |
1331 |
19.46 |
|
|
|
9 |
A |
1289 |
1234 |
51.43 |
|
|
|
10 |
A |
1153 |
1104 |
4.39 |
|
|
|
11 |
A |
1054 |
1009 |
154.09 |
|
|
|
12 |
A |
918 |
879 |
4.27 |
|
|
|
13 |
A |
568 |
544 |
12.42 |
|
|
|
14 |
A |
318 |
305 |
3.21 |
|
|
|
15 |
A |
3113 |
2982 |
12.80 |
|
|
|
16 |
A |
1471 |
1409 |
7.02 |
|
|
|
17 |
A |
1074 |
1029 |
0.53 |
|
|
|
18 |
A |
916 |
877 |
7.20 |
|
|
|
19 |
A |
422 |
405 |
122.97 |
|
|
|
20 |
A |
291 |
278 |
0.64 |
|
|
|
21 |
A |
213 |
204 |
0.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16040.2 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 15361.7 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(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.293 |
1.294 |
0.000 |
C2 |
0.000 |
0.561 |
0.000 |
N3 |
0.011 |
-0.708 |
0.000 |
O4 |
1.306 |
-1.202 |
0.000 |
H5 |
1.167 |
-2.151 |
0.000 |
H6 |
-2.125 |
0.590 |
0.000 |
H7 |
-1.375 |
1.940 |
0.879 |
H8 |
-1.375 |
1.940 |
-0.879 |
H9 |
0.939 |
1.118 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4865 | 2.3893 | 3.6040 | 4.2341 | 1.0896 | 1.0940 | 1.0940 | 2.2393 |
C2 | 1.4865 | | 1.2693 | 2.1945 | 2.9533 | 2.1249 | 2.1362 | 2.1362 | 1.0916 | N3 | 2.3893 | 1.2693 | | 1.3866 | 1.8498 | 2.4989 | 3.1152 | 3.1152 | 2.0482 | O4 | 3.6040 | 2.1945 | 1.3866 | | 0.9597 | 3.8708 | 4.2230 | 4.2230 | 2.3487 | H5 | 4.2341 | 2.9533 | 1.8498 | 0.9597 | | 4.2840 | 4.8966 | 4.8966 | 3.2773 | H6 | 1.0896 | 2.1249 | 2.4989 | 3.8708 | 4.2840 | | 1.7774 | 1.7774 | 3.1089 | H7 | 1.0940 | 2.1362 | 3.1152 | 4.2230 | 4.8966 | 1.7774 | | 1.7581 | 2.6080 | H8 | 1.0940 | 2.1362 | 3.1152 | 4.2230 | 4.8966 | 1.7774 | 1.7581 | | 2.6080 | H9 | 2.2393 | 1.0916 | 2.0482 | 2.3487 | 3.2773 | 3.1089 | 2.6080 | 2.6080 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
120.022 |
|
C1 |
C2 |
H9 |
119.812 |
C2 |
C1 |
H6 |
110.196 |
|
C2 |
C1 |
H7 |
110.838 |
C2 |
C1 |
H8 |
110.838 |
|
C2 |
N3 |
O4 |
111.357 |
N3 |
C2 |
H9 |
120.166 |
|
N3 |
O4 |
H5 |
102.537 |
H6 |
C1 |
H7 |
108.975 |
|
H6 |
C1 |
H8 |
108.975 |
H7 |
C1 |
H8 |
106.934 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.454 |
|
|
|
2 |
C |
0.075 |
|
|
|
3 |
N |
-0.075 |
|
|
|
4 |
O |
-0.411 |
|
|
|
5 |
H |
0.317 |
|
|
|
6 |
H |
0.151 |
|
|
|
7 |
H |
0.143 |
|
|
|
8 |
H |
0.143 |
|
|
|
9 |
H |
0.112 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.283 |
0.442 |
0.000 |
0.525 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-24.565 |
-2.078 |
0.000 |
y |
-2.078 |
-18.352 |
0.000 |
z |
0.000 |
0.000 |
-24.534 |
|
Traceless |
| x | y | z |
x |
-3.122 |
-2.078 |
0.000 |
y |
-2.078 |
6.197 |
0.000 |
z |
0.000 |
0.000 |
-3.075 |
|
Polar |
3z2-r2 | -6.150 |
x2-y2 | -6.212 |
xy | -2.078 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.331 |
-1.404 |
0.000 |
y |
-1.404 |
6.792 |
0.000 |
z |
0.000 |
0.000 |
3.360 |
<r2> (average value of r
2) Å
2
<r2> |
90.577 |
(<r2>)1/2 |
9.517 |
Jump to
S1C1
Energy calculated at B1B95/6-31G(2df,p)
| hartrees |
Energy at 0K | -209.056833 |
Energy at 298.15K | -209.062805 |
HF Energy | -209.056833 |
Nuclear repulsion energy | 120.625091 |
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(2df,p)
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' |
3892 |
3728 |
88.80 |
|
|
|
2 |
A' |
3210 |
3074 |
5.44 |
|
|
|
3 |
A' |
3184 |
3049 |
7.86 |
|
|
|
4 |
A' |
3069 |
2939 |
11.13 |
|
|
|
5 |
A' |
1780 |
1705 |
6.91 |
|
|
|
6 |
A' |
1477 |
1414 |
16.46 |
|
|
|
7 |
A' |
1404 |
1344 |
35.53 |
|
|
|
8 |
A' |
1386 |
1328 |
26.70 |
|
|
|
9 |
A' |
1349 |
1292 |
30.11 |
|
|
|
10 |
A' |
1147 |
1098 |
9.60 |
|
|
|
11 |
A' |
989 |
947 |
136.45 |
|
|
|
12 |
A' |
930 |
890 |
5.77 |
|
|
|
13 |
A' |
679 |
651 |
13.11 |
|
|
|
14 |
A' |
306 |
293 |
1.26 |
|
|
|
15 |
A" |
3130 |
2998 |
9.87 |
|
|
|
16 |
A" |
1484 |
1421 |
7.90 |
|
|
|
17 |
A" |
1061 |
1016 |
0.23 |
|
|
|
18 |
A" |
872 |
835 |
11.12 |
|
|
|
19 |
A" |
513 |
492 |
34.72 |
|
|
|
20 |
A" |
395 |
378 |
78.42 |
|
|
|
21 |
A" |
37 |
35 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16146.1 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 15463.1 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(2df,p)
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-1.441 |
0.480 |
0.000 |
C2 |
0.000 |
0.857 |
0.000 |
N3 |
1.008 |
0.085 |
0.000 |
O4 |
0.656 |
-1.254 |
0.000 |
H5 |
1.510 |
-1.688 |
0.000 |
H6 |
-1.563 |
-0.599 |
0.000 |
H7 |
-1.940 |
0.897 |
0.878 |
H8 |
-1.940 |
0.897 |
-0.878 |
H9 |
0.267 |
1.909 |
0.000 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.4891 | 2.4807 | 2.7210 | 3.6621 | 1.0863 | 1.0928 | 1.0928 | 2.2268 |
C2 | 1.4891 | | 1.2700 | 2.2102 | 2.9596 | 2.1359 | 2.1298 | 2.1298 | 1.0859 | N3 | 2.4807 | 1.2700 | | 1.3838 | 1.8427 | 2.6603 | 3.1818 | 3.1818 | 1.9696 | O4 | 2.7210 | 2.2102 | 1.3838 | | 0.9582 | 2.3135 | 3.4842 | 3.4842 | 3.1869 | H5 | 3.6621 | 2.9596 | 1.8427 | 0.9582 | | 3.2602 | 4.4002 | 4.4002 | 3.8066 | H6 | 1.0863 | 2.1359 | 2.6603 | 2.3135 | 3.2602 | | 1.7758 | 1.7758 | 3.1049 | H7 | 1.0928 | 2.1298 | 3.1818 | 3.4842 | 4.4002 | 1.7758 | | 1.7556 | 2.5817 | H8 | 1.0928 | 2.1298 | 3.1818 | 3.4842 | 4.4002 | 1.7758 | 1.7556 | | 2.5817 | H9 | 2.2268 | 1.0859 | 1.9696 | 3.1869 | 3.8066 | 3.1049 | 2.5817 | 2.5817 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
N3 |
127.904 |
|
C1 |
C2 |
H9 |
118.882 |
C2 |
C1 |
H6 |
111.096 |
|
C2 |
C1 |
H7 |
110.215 |
C2 |
C1 |
H8 |
110.215 |
|
C2 |
N3 |
O4 |
112.712 |
N3 |
C2 |
H9 |
113.214 |
|
N3 |
O4 |
H5 |
102.251 |
H6 |
C1 |
H7 |
109.160 |
|
H6 |
C1 |
H8 |
109.160 |
H7 |
C1 |
H8 |
106.893 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.471 |
|
|
|
2 |
C |
0.058 |
|
|
|
3 |
N |
-0.077 |
|
|
|
4 |
O |
-0.421 |
|
|
|
5 |
H |
0.321 |
|
|
|
6 |
H |
0.169 |
|
|
|
7 |
H |
0.148 |
|
|
|
8 |
H |
0.148 |
|
|
|
9 |
H |
0.127 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.608 |
0.077 |
0.000 |
0.613 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.419 |
-3.750 |
0.000 |
y |
-3.750 |
-20.663 |
0.000 |
z |
0.000 |
0.000 |
-24.542 |
|
Traceless |
| x | y | z |
x |
0.184 |
-3.750 |
0.000 |
y |
-3.750 |
2.818 |
0.000 |
z |
0.000 |
0.000 |
-3.002 |
|
Polar |
3z2-r2 | -6.003 |
x2-y2 | -1.756 |
xy | -3.750 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.750 |
-1.177 |
0.000 |
y |
-1.177 |
5.884 |
0.000 |
z |
0.000 |
0.000 |
3.344 |
<r2> (average value of r
2) Å
2
<r2> |
77.836 |
(<r2>)1/2 |
8.822 |