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All results from a given calculation for C4H5N ((Z)-2-Butenenitrile)

using model chemistry: LSDA/6-31G

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 yes CS 1A'
Energy calculated at LSDA/6-31G
 hartrees
Energy at 0K-208.890440
Energy at 298.15K-208.894970
Nuclear repulsion energy141.795679
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 LSDA/6-31G
Mode Number Symmetry Frequency
(cm-1)
Scaled Frequency
(cm-1)
IR Intensities
(km mol-1)
Raman Act
4/u)
Dep P Dep U
1 A 3144 3080 3.41      
2 A 3117 3054 7.08      
3 A 3084 3021 1.11      
4 A 2976 2916 4.59      
5 A 2255 2209 17.75      
6 A 1686 1652 16.27      
7 A 1461 1431 25.03      
8 A 1408 1379 19.10      
9 A 1387 1359 10.55      
10 A 1247 1222 1.22      
11 A 1125 1102 0.39      
12 A 986 966 21.75      
13 A 935 916 3.80      
14 A 672 658 2.03      
15 A 389 381 0.30      
16 A 152 149 4.15      
17 A 3048 2986 4.83      
18 A 1456 1426 17.56      
19 A 1055 1033 0.57      
20 A 972 952 0.73      
21 A 756 741 47.25      
22 A 532 521 6.80      
23 A 279 274 2.92      
24 A 163 160 0.47      

Unscaled Zero Point Vibrational Energy (zpe) 17141.1 cm-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 16793.1 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.
Rotational Constants (cm-1) from geometry optimized at LSDA/6-31G
ABC
0.39761 0.11763 0.09234

See section I.F.4 to change rotational constant units
Geometric Data calculated at LSDA/6-31G

Point Group is Cs

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
C1 -1.200 0.255 0.000
N2 -2.204 -0.367 0.000
C3 0.000 0.997 0.000
H4 -0.095 2.089 0.000
C5 1.217 0.414 0.000
H6 2.097 1.070 0.000
C7 1.455 -1.045 0.000
H8 0.508 -1.611 0.000
H9 2.045 -1.352 0.884
H10 2.045 -1.352 -0.884

Atom - Atom Distances (Å)
  C1 N2 C3 H4 C5 H6 C7 H8 H9 H10
C11.18161.41092.14122.42183.39622.95552.52953.72703.7270
N21.18162.59253.23763.50914.53533.72132.98394.45044.4504
C31.41092.59251.09581.34952.09842.50712.65773.23773.2377
H42.14123.23761.09582.12772.41713.49583.74924.14744.1474
C52.42183.50911.34952.12771.09821.47762.14572.14142.1414
H63.39624.53532.09842.41711.09822.21033.11732.57932.5793
C72.95553.72132.50713.49581.47762.21031.10371.10661.1066
H82.52952.98392.65773.74922.14573.11731.10371.79201.7920
H93.72704.45043.23774.14742.14142.57931.10661.79201.7684
H103.72704.45043.23774.14742.14142.57931.10661.79201.7684

picture of (Z)-2-Butenenitrile state 1 conformation 1
More geometry information
Calculated Bond Angles
atom1 atom2 atom3 angle atom1 atom2 atom3 angle
C1 C3 H4 116.783 C1 C3 C5 122.625
N2 C1 C3 179.986 C3 C5 H6 117.658
C3 C5 C7 124.890 H4 C3 C5 120.591
C5 C7 H8 111.635 C5 C7 H9 111.107
C5 C7 H10 111.107 H6 C5 C7 117.452
H8 C7 H9 108.347 H8 C7 H10 108.347
H9 C7 H10 106.082
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G Charges (e)
Number Element Mulliken CHELPG AIM ESP
1 C 0.002      
2 N -0.235      
3 C -0.111      
4 H 0.207      
5 C -0.066      
6 H 0.171      
7 C -0.574      
8 H 0.204      
9 H 0.200      
10 H 0.200      


Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section VII.A.3)
  x y z Total
  4.057 1.175 0.000 4.224
CHELPG        
AIM        
ESP        


Electric Quadrupole moment
Quadrupole components in D Å
Primitive
 xyz
x -34.801 -2.833 0.000
y -2.833 -26.854 0.000
z 0.000 0.000 -30.583
Traceless
 xyz
x -6.083 -2.833 0.000
y -2.833 5.839 0.000
z 0.000 0.000 0.244
Polar
3z2-r20.489
x2-y2-7.948
xy-2.833
xz0.000
yz0.000


Polarizabilities
Components of the polarizability tensor.
Units are Å3 (Angstrom cubed)
Change units.
  x y z
x 10.195 0.039 0.000
y 0.039 6.399 0.000
z 0.000 0.000 3.515


<r2> (average value of r2) Å2
<r2> 0.000
(<r2>)1/2 0.000