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NH3

Interactive structure of NH3

Properties

Molecule NH3
Calculation method RB3LYP
Basis set 6-31G(D,P)
Final energy (au) -56.55776
RMS gradient 0.00000485
Point group C3V
N-H bond length (Å) 1.02 ± 0.01
H-N-H bond angle 105.7° ± 1°
         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

Vibrational Modes

The vibrational modes of NH3
Wavenumber (cm-1) 1090 1694 1694 3461 3590 3590
Symmetry A1 E E A1 E E
Intensity (arbitrary units) 145 14 14 1 0 0
Image

Using the 3N-6 rule, the expected number of vibrational modes is 3 x 4 - 6 = 6 modes. The modes at 1694 cm-1 are degenerate, as well as the modes at 3590 cm-1. The bending modes are the ones at 1090 cm-1 and 1694 cm-1, and the stretching modes are the ones at 3461 cm-1 and 3590 cm-1. The modes that are highly symmetric are the ones at 1090 cm-1 and 3461 cm-1. In an experimental spectrum of gaseous ammonia, the expected number of bands would be 4, because 4 modes are actually pairs of degenerate modes. In reality, it would be very difficult to make out the degenerate vibrational modes at 3461 cm-1 and 3590 cm-1 on a spectrum, because their intensity is so low.

Gaussian job file of NH3



Charge Distribution

Considering the electronegativity of nitrogen is higher than that of hydrogen, the expected charge distribution would be a negative charge on nitrogen and a positive charge on the hydrogens. The calculated charge distribution is on the image below.

The distribution of charges in NH3













N2

Interactive structure of N2

Properties

Molecule N2
Calculation method RB3LYP
Basis set 6-31G(D,P)
Final energy (au) -109.52412
RMS gradient 0.00000060
Point group D∞h
N-N bond length (Å) 1.11 ± 0.01
         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

Vibrational Modes

The vibrational modes of N2
Wavenumber (cm-1) 2457
Symmetry SGG
Intensity (arbitrary units) 0
Image

Using the 3N-5 rule, the expected number of vibrational modes is 3 x 2 - 5 = 1 mode, which is at 2457 cm-1. It is a stretching mode and since it is symmetric, there is no change in dipole, and it is not IR active. In an experimental spectrum of nitrogen gas, the expected number of bands would be 0, because because there are no modes with a change in dipole.

Gaussian job file of N2



Charge Distribution

Since a nitrogen molecule consists of 2 nitrogen atoms with the same electronegativity, the overall charge is 0 and the charge on each atom is also 0. The calculated charge distribution is on the image below.

The distribution of charges in N2













H2

Interactive structure of H2

Properties

Molecule H2
Calculation method RB3LYP
Basis set 6-31G(D,P)
Final energy (au) -1.17853
RMS gradient 0.00000023
Point group D∞h
H-H bond length (Å) 0.74 ± 0.01
         Item               Value     Threshold  Converged?
 Maximum Force            0.000000     0.000450     YES
 RMS     Force            0.000000     0.000300     YES
 Maximum Displacement     0.000001     0.001800     YES
 RMS     Displacement     0.000001     0.001200     YES

Vibrational Modes

The vibrational modes of H2
Wavenumber (cm-1) 4466
Symmetry SGG
Intensity (arbitrary units) 0
Image

Using the 3N-5 rule, the expected number of vibrational modes is 3 x 2 - 5 = 1 mode, which is at 4466 cm-1. It is a stretching mode and since it is symmetric, there is no change in dipole, and it is not IR active. In an experimental spectrum of hydrogen gas, the expected number of bands would be 0, because because there are no modes with a change in dipole.

Gaussian job file of H2



Charge Distribution

Since a hydrogen molecule consists of 2 hydrogen atoms with the same electronegativity, the overall charge is 0 and the charge on each atom is also 0. The calculated charge distribution is on the image below.

The distribution of charges in H2













Mono-Metallic Transition Metal Complex Incorporating H2

There is a complex that coordinates H2, where the bond length between the hydrogens is different than in hydrogen gas. The complex is Chloro-(dihydrogen-H,H')-hydrido-tris(triphenylphosphine)-osmium, with the identifier CEFCAS. The H-H bond distance in the complex is 1.482 Å.
The reason for the increased bond length is the that the d orbitals of the osmium atom overlap with the bonding and antibonding orbitals of the two hydrogens, increasing the antibonding character in the H-H bond, weakening it and elongating it. Eventually, this H-H bond gets cleaved, leaving 2 hydride ligands.[1] Also, when calculating the bond lengths with software, some approximations have to be made, which changes the result. Experimentally obtained values may also be affected by external factors.

Interactive structure of the metal complex


Energy of Formation of Ammonia

The formation of ammonia from hydrogen and nitrogen gas goes as follows:
N2 + 3H2 -> 2NH3
The energy change of this reaction can be found by calculating the energies of each reactant and products, then subtracting the energy of the reactants from the energy of the products. The energies of the reactants and products have been determined in the previus sections.

  • E(NH3) = -56.55776 au
  • 2 * E(NH3) = -113.11553 au
  • E(N2) = -109.52412 au
  • E(H2) = -1.17853 au
  • 3 * E(H2) = -3.53561 au
  • ΔE = 2 * E(NH3) - [E(N2) + 3 * E(H2)]= -113.11553 - (-109.52412 -3.53561) = -0.0557 au

In kJ/mol that value is approximately -146.8. Since ΔE is negative, ammonia must be more stable than the gaseous reactants.

PF3Cl2

Interactive structure of PF3Cl2

Properties

Molecule PF3Cl2
Calculation method RB3LYP
Basis set 6-31G(D,P)
Final energy (au) -1561.34405
RMS gradient 0.00000295
Point group D3H
P-Cl bond length (Å) 2.10 ± 0.01
P-F bond length (Å) 1.58 ± 0.01
F-P-F bond angle 180°
F-P-Cl bond angle 90°
Cl-P-Cl bond angle 120°
         Item               Value     Threshold  Converged?
 Maximum Force            0.000008     0.000450     YES
 RMS     Force            0.000003     0.000300     YES
 Maximum Displacement     0.000046     0.001800     YES
 RMS     Displacement     0.000014     0.001200     YES

Vibrational Modes

The vibrational modes of PF3Cl2
Wavenumber (cm-1) Symmetry Intensity Image IR Activity Mode
117 E' 0 Yes Bending
117 E' 0 Yes Bending
348 A''2 13 Yes Bending
348 A''2 13 Yes Bending
353 A'1, A'2, or A''11) 0 No Stretching
371 A'1, A'2, or A''1 0 No Bending
371 A'1, A'2, or A''1 0 No Bending
451 A2 2 Yes Stretching
589 A''2 683 Yes Stretching
707 A'1 0 No Stretching
985 E' 189 Yes Stretching
985 E' 189 Yes Stretching

1)Note: for the modes at 353 cm-1 and 371 cm-1, Gaussian was unable to determine symmetry.

Using the 3N-6 rule, the expected number of vibrational modes is 3 x 6 - 6 = 12 modes. There are degenerate pairs of vibrational modes at 116 cm-1, 349cm-1, 371 cm-1, and 985 cm-1. The vibrational modes are the first 7 (up to 371 cm-1), excluding the mode at 353 cm-1. The rest of them are stretching modes. The modes that are highly symmetric are the ones at 353 cm-1 and 707 cm-1. In an experimental spectrum of PF3Cl2, the expected number of bands would be 5, because 6 modes are actually pairs of degenerate modes and 4 modes are IR inactive. In reality, it would be very difficult to make out the degenerate vibrational modes at 117 cm-1 and 451 cm-1 on a spectrum, because their intensity is so low.

Gaussian job file of PF3Cl2

Charge Distribution

Considering the electronegativity of fluorine is the highest, chlorine the second highest, and phosphorus the lowest, the expected charge distribution would be a high negative charge on the fluorine atoms, a weaker negative charge on the chlorine atoms, and a positive charge on the phosphorus atom. The calculated charge distribution is on the image below.

The distribution of charges in PF3Cl2















Molecular Orbitals

Molecular Orbital Number Image Atomic Orbitals Involved Bonding or Antibonding Energy Filled or Empty
38 Fluorine 2pz orbitals and chlorine 3px orbitals Antibonding -0.33759 au (HOMO) Filled with 2 electrons
30 Fluorine 2pz orbitals and chlorine 3px orbitals Bonding (bonding equivalent of HOMO) -0.51680 au Filled with 2 electrons
39 Fluorine 2px orbitals, chlorine 3pz orbitals, phosphorus 3s orbital Antibonding -0.07701 au (LUMO) Empty
40 Fluorine 2pz orbitals, chlorine 3pz orbitals, phosphorus 3pz orbital Antibonding 0.03013 au Empty
27 Fluorine 2pz orbitals, chlorine 3pz orbitals, phosphorus 3pz orbital Bonding (bonding equivalent of molecular orbital 40) -0.56466 au Empty

Bond Lengths of PCl3F2

Interactive structure of PCl3F2

The bond lengths for PCl3F2 are different , because of the equatorial and axial positions are in different environments. The P-F bond length in PCl3F2 is 1.62 Å, compared to 1.58 Å for PF3Cl2. The P-Cl bond length in PCl3F2 is 2.05 Å, compared to 2.10 Å in PF3Cl2. The equatorial P-Cl bond length is shorter than the axial P-Cl bond length, just as the equatorial P-F bond length is shorter than the axial P-F bond length. The reason is that the axial bonds are formed from the overlap with an unhybridized phosphorus 3p orbital, while the equatorial bonds are formed from overlap with sp2 hybridized phosphorus orbitals, which have more s character.

References

  1. Angew.Chem.Int.Ed. 2005, 44,7227–7230, DOI: 10.1002/anie.200502297

Marking

Note: All grades and comments are provisional and subject to change until your grades are officially returned via blackboard. Please do not contact anyone about anything to do with the marking of this lab until you have received your grade from blackboard.

Wiki structure and presentation 1/1

Is your wiki page clear and easy to follow, with consistent formatting?

YES

I'm not going to mark you down for this but it is completely inappropriate to write "testosterone420" as the title of your page in work that is handed in to be marked. You should only write things relevant to the subject at hand in any piece of academic work.

Do you effectively use tables, figures and subheadings to communicate your work?

YES

NH3 0.5/1

Have you completed the calculation and given a link to the file?

YES

Have you included summary and item tables in your wiki?

YES

Have you included a 3d jmol file or an image of the finished structure?

YES

Have you included the bond lengths and angles asked for?

YES

Have you included the “display vibrations” table?

YES

Have you added a table to your wiki listing the wavenumber and intensity of each vibration?

YES

Did you do the optional extra of adding images of the vibrations?

YES

Have you included answers to the questions about vibrations and charges in the lab script?

YES, most answers are correct. However there are only 2 visible peaks in the spectra of NH3, due to the low intensity of the other 2 peaks. (See infrared column in vibrations table.)

N2 and H2 0.5/0.5

Have you completed the calculations and included all relevant information? (summary, item table, structural information, jmol image, vibrations and charges)

YES

Crystal structure comparison 0.5/0.5

Have you included a link to a structure from the CCDC that includes a coordinated N2 or H2 molecule?

YES

Have you compared your optimised bond distance to the crystal structure bond distance?

YES

Haber-Bosch reaction energy calculation 1/1

Have you correctly calculated the energies asked for? ΔE=2*E(NH3)-[E(N2)+3*E(H2)]

YES

Have you reported your answers to the correct number of decimal places?

YES

Do your energies have the correct +/- sign?

YES

Have you answered the question, Identify which is more stable the gaseous reactants or the ammonia product?

YES

Your choice of small molecule 4/5

Have you completed the calculation and included all relevant information?

YES

Have you added information about MOs and charges on atoms?

YES - especially good discussion of the charges well done! You could have improved by adding more detail on the MOs - for example the LUMO is antibonding (as you stated) but does not affect the P-X bonding as it is unoccupied.

Independence 0.5/1

If you have finished everything else and have spare time in the lab you could:

Check one of your results against the literature, or

Do an extra calculation on another small molecule, or

YES - you did an extra calculation on PCl3F2 and discussed your results. It would have been good for you to include a link to the log file of the independent calculation.

Do some deeper analysis on your results so far