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All results from a given calculation for C2H4N2O2 (Oxalamide)

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 C2H 1Ag
Energy calculated at LSDA/6-31G*
 hartrees
Energy at 0K-336.866619
Energy at 298.15K-336.873030
Nuclear repulsion energy234.529995
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 Ag 3629 3561 0.00      
2 Ag 3444 3380 0.00      
3 Ag 1834 1800 0.00      
4 Ag 1542 1513 0.00      
5 Ag 1381 1355 0.00      
6 Ag 1080 1060 0.00      
7 Ag 772 757 0.00      
8 Ag 533 523 0.00      
9 Ag 382 375 0.00      
10 Au 715 702 6.66      
11 Au 520 510 313.17      
12 Au 354 347 207.44      
13 Au 120 117 2.81      
14 Bg 800 785 0.00      
15 Bg 712 699 0.00      
16 Bg 409 401 0.00      
17 Bu 3630 3562 196.46      
18 Bu 3446 3381 137.17      
19 Bu 1813 1779 482.59      
20 Bu 1528 1500 420.80      
21 Bu 1307 1283 30.07      
22 Bu 1080 1060 30.88      
23 Bu 551 541 14.75      
24 Bu 278 273 50.06      

Unscaled Zero Point Vibrational Energy (zpe) 15928.6 cm-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 15630.7 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.
Rotational Constants (cm-1) from geometry optimized at LSDA/6-31G*
ABC
0.18562 0.12925 0.07620

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

Point Group is C2h

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
C1 -0.061 0.762 0.000
C2 0.061 -0.762 0.000
O3 -1.154 1.322 0.000
O4 1.154 -1.322 0.000
N5 1.154 1.319 0.000
N6 -1.154 -1.319 0.000
H7 1.278 2.329 0.000
H8 1.939 0.658 0.000
H9 -1.278 -2.329 0.000
H10 -1.939 -0.658 0.000

Atom - Atom Distances (Å)
  C1 C2 O3 O4 N5 N6 H7 H8 H9 H10
C11.52851.22832.41231.33672.35052.06112.00283.32152.3548
C21.52852.41231.22832.35051.33673.32152.35482.06112.0028
O31.22832.41233.50992.30802.64122.63233.16363.65282.1306
O42.41231.22833.50992.64122.30803.65282.13062.63233.1636
N51.33672.35052.30802.64123.50521.01711.02614.38423.6713
N62.35051.33672.64122.30803.50524.38423.67131.01711.0261
H72.06113.32152.63233.65281.01714.38421.79615.31274.3903
H82.00282.35483.16362.13061.02613.67131.79614.39034.0959
H93.32152.06113.65282.63234.38421.01715.31274.39031.7961
H102.35482.00282.13063.16363.67131.02614.39034.09591.7961

picture of Oxalamide state 1 conformation 1
More geometry information
Calculated Bond Angles
atom1 atom2 atom3 angle atom1 atom2 atom3 angle
C1 C2 O4 121.718 C1 C2 N6 110.064
C1 N5 H7 121.660 C1 N5 H8 115.286
C2 C1 O3 121.718 C2 C1 N5 110.064
C2 N6 H9 121.660 C2 N6 H10 115.286
O3 C1 N5 128.218 O4 C2 N6 128.218
H7 N5 H8 123.054 H9 N6 H10 123.054
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 0.465      
2 C 0.465      
3 O -0.466      
4 O -0.466      
5 N -0.740      
6 N -0.740      
7 H 0.362      
8 H 0.378      
9 H 0.362      
10 H 0.378      


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
 xyz
x -31.136 11.577 0.000
y 11.577 -30.043 0.000
z 0.000 0.000 -34.904
Traceless
 xyz
x 1.338 11.577 0.000
y 11.577 2.977 0.000
z 0.000 0.000 -4.315
Polar
3z2-r2-8.629
x2-y2-1.093
xy11.577
xz0.000
yz0.000


Polarizabilities
Components of the polarizability tensor.
Units are Å3 (Angstrom cubed)
Change units.
  x y z
x 7.739 0.676 0.000
y 0.676 6.501 0.000
z 0.000 0.000 2.588


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