Jump to content

Rep:Mod:19970410

From ChemWiki

NH3

Basic properties of NH3

Calculation method:RB3LYP

Basis set:6-31G(d,p)

Final energy:-56.55776873 a.u.

RMS gradient:0.00000485 a.u.

Point group:C3v

N-H distance:1.01798 Å

The literature value of N-H distance is 1.012 Å [1]

H-N-H Bond angle:105.74115°

The literature value of H-N-H Bond angle is 106.7° [2]


Item Table of NH3

[here]


         Item               Value     Threshold  Converged?
 Maximum Force            0.000004     0.000450     YES
 RMS     Force            0.000004     0.000300     YES
 Maximum Displacement     0.000072     0.001800     YES
 RMS     Displacement     0.000035     0.001200     YES
 Predicted change in Energy=-5.986277D-10
 Optimization completed.
    -- Stationary point found.
                           ----------------------------
                           !   Optimized Parameters   !
                           ! (Angstroms and Degrees)  !
 --------------------------                            --------------------------
 ! Name  Definition              Value          Derivative Info.                !
 --------------------------------------------------------------------------------
 ! R1    R(1,2)                  1.018          -DE/DX =    0.0                 !
 ! R2    R(1,3)                  1.018          -DE/DX =    0.0                 !
 ! R3    R(1,4)                  1.018          -DE/DX =    0.0                 !
 ! A1    A(2,1,3)              105.7412         -DE/DX =    0.0                 !
 ! A2    A(2,1,4)              105.7412         -DE/DX =    0.0                 !
 ! A3    A(3,1,4)              105.7412         -DE/DX =    0.0                 !
 ! D1    D(2,1,4,3)           -111.8571         -DE/DX =    0.0                 !
 --------------------------------------------------------------------------------
 GradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGrad

Diagram of NH3

NH3 molecule

Vibrations

Mode of different vibrations

Vibration images

Mode 1

Frequency: 1089.54Hz

Intensity:145.3814

Type:Bending

Mode 2

Frequency: 1693.95Hz

Intensity:13.5533

Type:Bending

Mode 3

Frequency: 1693.95Hz

Intensity:13.5533

Type:Bending


Mode 4

Frequency: 3461.29Hz

Intensity:1.0608

Type:stretching

Mode 5

Frequency: 3589.82Hz

Intensity:0.2711

Type:stretching


Mode 6

Frequency: 3589.82Hz

Intensity:0.2711

Type:stretching



How many modes do you expect from the 3N-6 rule?

For the rule 3N-6, N represents the number of atoms which is 4 in NH3, So the expected number of modes should be 3*4-6=6.

Which modes are degenerate (ie have the same energy)?

Mode 2 and mode 3 are degenerate; Mode 5 and mode 6 are degenerate since they absorb Infrad red with the same frequency.

Which modes are "bending" vibrations and which are "bond stretch" vibrations?

Mode 1,2 and 3 are "bending" vibrations;Mode 4,5 and 6 are "bond stretch" vibrations.

Which mode is highly symmetric?

Mode 4 is highly symmetric.

One mode is known as the "umbrella" mode, which one is this?

Mode 1 is the "umbrella" mode.

How many bands would you expect to see in an experimental spectrum of gaseous ammonia?

4 bands will be expected, but from the spectrum, the band can be observed is only 2. The dipole moment of the several modes are too low, thus the intensity is quite low, so the spectrum do no show them.

Charge Distribution

The charge on the N-atom is -1.125;

The charge on the H-atom is +0.375.

Because N-atom has a bigger electronegativity than H-atom, so electrons are 'pulled' towards N-atom. The concept electronegativity is a chemical properties that means the ability to attract electrons towards itself.

H2

Basic properities of H2

Calculation method:RB3LYP

Basis set:6-31G(d,p)

Final energy:-1.17853936 a.u.

RMS gradient:0.00000017 a.u.

Point group:D∞h

H-H distance:0.74279 Å

The literature value of H-H bond distance is 0.74 Å [3]

H-H Bond angle:180 °


Item Table of H2

[here]

   Item               Value     Threshold  Converged?
 Maximum Force            0.000000     0.000450     YES
 RMS     Force            0.000000     0.000300     YES
 Maximum Displacement     0.000000     0.001800     YES
 RMS     Displacement     0.000001     0.001200     YES
 Predicted change in Energy=-1.164080D-13
 Optimization completed.
    -- Stationary point found.
                           ----------------------------
                           !   Optimized Parameters   !
                           ! (Angstroms and Degrees)  !
 --------------------------                            --------------------------
 ! Name  Definition              Value          Derivative Info.                !
 --------------------------------------------------------------------------------
 ! R1    R(1,2)                  0.7428         -DE/DX =    0.0                 !
 --------------------------------------------------------------------------------
 GradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGrad

Diagram of H2

H2 molecule

Vibrations

Mode of Vibrations

Vibration images

Mode 1

Frequency:4465.68Hz

Intensity:0

Type:stretching

Since the H2 molecule have no dipole moment, so they will not absorb IR, thus the intensity is 0.

Charge Distribution

The charge on the N-atom is 0.00;

The charge on the H-atom is 0.00.

Because H-atom has a same electronegativity with the H-atom, so electrons are 'pulled' equally towards themselves. The concept electronegativity is a chemical properities that means the ability to attract electrons towards itself.


N2

Basic properties of N2

Calculation method:RB3LYP

Basis set:6-31G(d,p)

Final energy:-109.52412868 a.u.

RMS gradient:0.00000060 a.u.

Point group:C∞h

N-N distance:1.10550 Å

N-N Bond angle:105.74115 °


Item Table of N2

[here]

 Item               Value     Threshold  Converged?
 Maximum Force            0.000001     0.000450     YES
 RMS     Force            0.000001     0.000300     YES
 Maximum Displacement     0.000000     0.001800     YES
 RMS     Displacement     0.000000     0.001200     YES
 Predicted change in Energy=-3.401031D-13
 Optimization completed.
    -- Stationary point found.
                           ----------------------------
                           !   Optimized Parameters   !
                           ! (Angstroms and Degrees)  !
 --------------------------                            --------------------------
 ! Name  Definition              Value          Derivative Info.                !
 --------------------------------------------------------------------------------
 ! R1    R(1,2)                  1.1055         -DE/DX =    0.0                 !
 --------------------------------------------------------------------------------
 GradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGrad

Diagram of N2

N2 molecule

Vibrations

Mode of different vibrations


Vibration images

Mode 1

Frequency:2457.33Hz

Intensity:0

Type: stretching

Since the N2 molecule have no dipole moment, so they will not absorb IR, thus the intensity is 0.

Charge Distribution

The charge on the N-atom is 0.00;

The charge on the H-atom is 0.00.

Because N-atom has a same electronegativity with the N-atom, so electrons are 'pulled' equally towards themselves. The concept electronegativity is a chemical properities that means the ability to attract electrons towards itself.


Molecular Orbitals of N2

MO diagram

[4]

MO images

Type of orbital: 1s-1s bonding orbital

Energy of orbital:-14.44676 a.u.

Description:This is the 1s-1s bonding orbital. From the diagram, there is little overlap of 1s-1s AOs and has a very low energy. These 2 features indicate the little contribution of chemical bonding. Because the 1s AOs is very close to nucleus, the electrons will be held so tightly, thus 1s AOs are very hard to overlap.

Type of orbital: 1s-1s anti-bonding π orbital

Energy of orbital:-14.44512 a.u.

Description: This is anti-bonding orbital with low contribution to the formation of chemical bonding. The energy of this MO is too low that means there is almost no contribution of bond formation.

Type of orbital: 2s-2s bonding orbital

Energy of orbital:-1.12383 a.u.

Description: This is a bonding orbital that contributes strongly to the formation of chemical bonding. From the diagram, the 2s-2s MO is a extended circular surface that shows the big overlap.

Type of orbital: 2s-2s anti-bonding orbital

Energy of orbital:-0.55342 a.u.

Description: This is anti-bonding orbital has a relatively big energy difference with 2s-2s bonding orbital which can also indicate the better overlap of 2s-2s bonding orbital.

Type of orbital: 2p-2p bonding π orbital

Energy of orbital:-0.46240 a.u.

Description: This is a pi bond which formed from the side to side overlap of 2p AOs. There are 2 pi orbital with same energy. Since the existence of 3 x 2p orbitals, two of them are perpendicular to each other resulting in the formation of 2 pi bonds.

Type of orbital: 2p-2p bonding σ orbital

Energy of orbital:-0.42688 a.u.

Description: This is a sigma bonding that formed by the back to back overlap of 2p-2p orbital. Normally, the Sigma orbital should have a lower energy than pi bonding;however, the s-p mixing create a pi orbital with lower energy. [5]

Type of orbital: 2p-2p anti-bonding π orbital

Energy of orbital:-0.02412 a.u.

Description:This is an anti-bonding orbital which is unoccupied by electrons. The energy is quiet high that will destabilise the bond formation. However, there are no electrons in this orbital, so the chemical bond formed is not destabilized by this anti-bonding orbital

Type of orbital: 2p-2p anti-bonding σ* orbital

Energy of orbital:0.41366 a.u.

Description: This is the anti-bonding orbital with positive energy. But it also do not contain any electrons, so this orbital will not destabilize the chemical bond.

Haber-Bosch process

Reaction equation

N2 + 3H2 -> 2NH3

This reaction was used as the major production source of fertilizer. Originally, most of the plants can only obtain the NH3 under the help of thunderstorm, but with the fertilizer, they can absorb NH3 easily, thus they can grow more quicker and stronger. The N- atom is the essential components in amino acid, thus, more N- atoms, more amino acid and more protein in the plants. Since it is an exothermic reaction, the optimized temperature used is 450 degrees with 100 a.t.m. pressures. The catalyst is Iron. Based on these conditions, this reaction is relatively highly efficient for converting nitrogen gas and hydrogen gas into fertilizer.

Reaction energies

E(NH3)=-56.55776873 a.u.=-148492.421 kJ/mol

2*E(NH3)=-113.1155375 a.u.=-296984.843 kJ/mol

E(N2)=-109.52412868 a.u.=-287555.599 kJ/mol

E(H2)=-1.17853936 a.u.=-3094.255 kJ/mol

3*E(H2)=-3.53561808 a.u.=-9282.765 kJ/mol

ΔE=2*E(NH3)-[E(N2)+3*E(H2)]=-0.5579074 a.u.= -146.48 kJ/mol

Since the reaction release energy which is exothermic reaction, the final product ( ammonia) is more stable than the gaseous reactants.

The literature value of reaction energies of Haber process is -45.7kJ/mol which much smaller than the calculated value. The difference may due to the different calculation method used. [6]

H2SiO

Basic properties of H2SiO

Calculation method:RB3LYP

Basis set:6-31G(d,p)

Final energy:-365.90001403 a.u.

RMS gradient:0.00000941 a.u.

Point group:Cs

Si-H distance:1.48652 Å

Si=O distance:1.53172 Å

H-Si=O Bond angle:124.15648 °

H-Si-H Bond angle:111.68594 °

Item Table of H2SiO

[here]

  Item               Value     Threshold  Converged?
 Maximum Force            0.000023     0.000450     YES
 RMS     Force            0.000009     0.000300     YES
 Maximum Displacement     0.000022     0.001800     YES
 RMS     Displacement     0.000017     0.001200     YES
 Predicted change in Energy=-5.109756D-10
 Optimization completed.
    -- Stationary point found.
                           ----------------------------
                           !   Optimized Parameters   !
                           ! (Angstroms and Degrees)  !
 --------------------------                            --------------------------
 ! Name  Definition              Value          Derivative Info.                !
 --------------------------------------------------------------------------------
 ! R1    R(1,2)                  1.4865         -DE/DX =    0.0                 !
 ! R2    R(1,3)                  1.4865         -DE/DX =    0.0                 !
 ! R3    R(1,4)                  1.5317         -DE/DX =    0.0                 !
 ! A1    A(2,1,3)              111.686          -DE/DX =    0.0                 !
 ! A2    A(2,1,4)              124.1565         -DE/DX =    0.0                 !
 ! A3    A(3,1,4)              124.1576         -DE/DX =    0.0                 !
 ! D1    D(2,1,4,3)            180.0            -DE/DX =    0.0                 !
 --------------------------------------------------------------------------------
 GradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGrad

Diagram of H2SiO

H2SiO molecule

Vibrations

Mode of Vibrations

Vibration images

Mode 1

Frequency:698.63Hz

Intensity:58.6111

Type:Bending


Mode 2

Frequency:712.10Hz

Intensity:61.2043

Type: Bending


Mode 3

Frequency:1037.98Hz

Intensity:55.3456

Type: Bending


Mode 4

Frequency:1219.23Hz

Intensity:64.9588

Type: stretching and bending


Mode 5

Frequency:2230.72Hz

Intensity:49.9752

Type: stretching


Mode 6

Frequency:2247.73Hz

Intensity:185.7008

Type: stretching


How many modes do you expect from the 3N-6 rule?

For the rule 3N-6, N represents the number of atoms which is 4 in H2SiO, So the expected number of modes should be 3*4-6=6.

Which modes are degenerate (ie have the same energy)?

None of the modes are degenerate since they do not absorb Infrad red with the same frequency.

Which modes are "bending" vibrations and which are "bond stretch" vibrations?

Mode 1,2 and 3 are "bending" vibrations;Mode 5 and 6 are "bond stretch" vibrations.

Which mode is highly symmetric?

Mode 5 is highly symmetric.

How many bands would you expect to see in an experimental spectrum of gaseous ammonia?

6 bands will be expected. But from the spectrum, only 4 bands were observed, since the value of frequency was quite similar, so they overlap to form a bigger band.

Charge Distribution

The charge on the Si-atom is +1.472;

The charge on the H-atom is -0.236.

The charge on the O-atom is -1.001.

Because O-atom has the biggest electronegativity value, so electrons are 'pulled' towards O-atom. For H-atom and Si-atom, H-atom has a bigger electronegativity than Si-atom, so H-atom is more negative charged since more electrons were pulled towards H-atom. The concept electronegativity is a chemical properties that means the ability to attract electrons towards itself.

MO orbitals

Coordinates

The Si=O bond is in z direction

The molecule is a trigonal planar structure and in z-y phase.

MO image:

Type of orbital: 2s-2pz bonding orbital

Energy of orbital:-0.92465 a.u.

Description:This MO comes from the overlap of 2s orbital form o-atom and 2pz orbital from Si-atom. Since 2s orbital can only have one phase, but 2p orbital have 2 different phase, thus only part of the orbital will overlap. This MO orbital is occupied by electrons and will positively contribute to the chemical bond formation.

Type of orbital: 1s(H)-2s(Si)-1s(H) bonding orbital with a mixture of 2ps(Si)-2pz(H) anti-bonding orbital

Energy of orbital:-0.52699 a.u.

Description: This orbital is a mixture of bonding and anti-bonding orbital. The bonding orbital comes from the overlap of 1s(H)-2s(Si)-1s(H) AOs in the same phase, thus at the bottom the diagram, there is a big overlap area. The discontinuous of Si-O bond comes form the overlap of 2s(Si)-2pz(H) in the out-of-phase. Thus, there is no overlap orbitals between Si-O. This orbital is also occupied by electrons and will weaken the Si-O bond but strengthen the Si-H bond.

Type of orbital: 1s(H)(+)-2py(Si)(+)-2py(O)(+) bonding orbital

Energy of orbital:-0.39697 a.u.

Description: This orbital comes from a big overlap of 1s(H)-2py(Si)-2py(O), since the 2py orbitals has different phase, the 1s orbital for left hand side should have a different phase with the right hand side. Meanwhile, the phase of s and p orbitals all should be the same phase for each of the side. This orbital is also occupied by electrons and will stabilize the chemical bond formation

Type of orbital: 1s(H)-1s(H) bonding orbital and 2pz(Si)-2pz</sub(O) anti-bonding orbital and 2pz</sub(Si)-1s(H) anti-bonding orbitals

Energy of orbital:-0.35346 a.u.

Description: This orbitals is a mixture of bonding and anti-bonding orbitals. The 1s(H)-1s(H) overlap to form a bonding orbital but the 1s-1s system has a different phase with the 2pz</sub(Si), thus there is an overlap between Si and H atoms. The other anti-bonding orbital is the cancellation of the 2s(O)-2pz</sub(Si) AOs. The 2pz</sub orbital from O-atom also has a different phase with the 2pz</sub(Si), thus the 2pz</sub orbital from O-atom cancel with 2pz</sub orbital from Si-atom to create the discontinuities. Since the 2pz</sub(Si) orbital was cancelled by the s orbital from upwards and downwards, it become smaller. This orbital is occupied by electrons and will partially destabilize the bond formation.

Type of orbital: 2px-2px bonding π orbital

Energy of orbital:-0.31773 a.u.

Description: This a pi bond which formed from the side to side overlap of 2px AOs. Since the 2 x 2px are perpendicular to 2pz resulting in formation of pi bond. This orbital is occupied by electrons and will stabilize the bond formation.

Reaction energies

E(H2SiO)=-365.90001403 a.u.

E(O2)=-150.25742434 a.u.

0.5*(O2)=-75.12871217 a.u.

E(H2)=-1.17853936 a.u.

2*E(H2)=-2.35707872

2*ΔE= 2*E(H2SiO)-[(O2)+2*E(H2)]=-579.185525 a.u.

ΔE=-289.5927625 a.u. = -7.60*105 kJ/mol

Reference

  1. Revore, M., & Mccarthy, M. I. (1996). Surfaces. Molecules, 3654(95), 7610–7616.
  2. Revore, M., & Mccarthy, M. I. (1996). Surfaces. Molecules, 3654(95), 7610–7616.
  3. Liang, T., Devine, B., Phillpot, S. R., & Sinnott, S. B. (2012). Variable charge reactive potential for hydrocarbons to simulate organic-copper interactions. Journal of Physical Chemistry A, 116(30), 7976–7991. doi:10.1021/jp212083t
  4. Mo, D., Bond, P., & Bond, D. (n.d.). MO Diagram for CO.
  5. MO theory for diatomic molecules. (2012).
  6. Modak, J. M. (2002). Haber Process for Ammonia Synthesis Jayant M Modak. Resonance, 7(8), 69–77.