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Hydrogen Cyanide (HCN)

    The geometry optimization of 621G, 631G, and DZV are shown below for the smallest polar molecule hydrogen cyanide. There is no bond angle due to the molecule being linear making the angle 180 degrees.

Table 1: This table represents the bond lengths of each atom in hydrogen cyanide taken from the literature3.
Type of bond
Bond Length in Angstroms
C-H
1.064
C-N
1.156

    These buttons below display the bond lengths calculated from each level of theory.

    This button displays the bond length using the lowest level of optimization theory.
    This button displays the bond length using the second highest level of optimization theory.

    This button displays the bond length using the highest level of theory and gave the best optimized lengths compared to the literature. This comparison gave a 0.90% error for the H to N bond length (Total Length of HCN).

    This displays the Highest Occupied Molecular Orbital found at orbital 7.  The orbitals were calculated by adding all of electrons in the molecule and dividing it by two. 
    This displays the Lowest Unoccupied Molecular Orbital found at orbital 8. The electrons will transition to this orbital when excited with enough energy.

    This button displays the electrostatic potential. The electron cloud ranges in color from red to blue. Red being areas of high electrostatic potential and blue  being areas of low electrostatic potential. Since the nitrogen atom is more electronegative, thus pulling the electrons closer to it (Red area).

    The partial atomic charge on each atom is shown in this diagram.  They are created by the asymmetric distribution of electrons in a chemical bond. The sum of these charges equal to zero.

    Below shows the vibrations of HCN, determined from an IR-spectrum.

Table 2: The vibrations of HCN in cm^-1 taken from the literature1.
Type of vibration
Wave Length in cm^-1
C-H bend
685-995
C-N triple bond stretch
2200-2280
C-H alkyne stretch
3200-3310

IR spectrum of HCN retreived from NIST
Figure 1:
An IR-Spectrum of HCN taken from the NIST website3.


C-H bend
C-N triple bond stretch
C-H alkyne stretch

    These buttons above represent the vibrations calculated from the highest level of theory, DZV. The values calculated from the DZV optimization does not deviate with the C-H bend, but with the C-H triple bond stretch and the C-H alkyne stretch it deviates substantially. The values for those two vibrations were overestimated giving a 2.16% and 12.20% error respectively.

    A Dipole moment is present in HCN since the molecule is polar.
Table 3: This table displays the dipole moment for HCN in the gas phase taken from the literature5.
Molecule
Dipole Moment
Hydrogen Cyanide
3.06

Table 4: This table displays the dipole moments calculated from each level of theory.
Level of Geometry Optimization Theory
Dipole Moment of HCN
621G
3.028709
631G
3.271937
DZV
3.286865

    The best value for the dipole moment of HCN was calculated with the lowest level of theory, 621G. This gave a percent error of 1.04%.

Based on template by A. Herráez as modified by J. Gutow
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