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EX3 section

BH3

Item               Value     Threshold  Converged?
 Maximum Force            0.000007     0.000450     YES
 RMS     Force            0.000004     0.000300     YES
 Maximum Displacement     0.000028     0.001800     YES
 RMS     Displacement     0.000014     0.001200     YES

File:Ruman1 BH3 FREQ.LOG


Low frequencies ---  -38.8634  -38.8412  -18.7509   -0.0042    0.0451    0.2082
 Low frequencies ---  458.9323 1681.0420 1681.0424



Wavenumber (cm-1 Intensity (arbitrary units) symmetry IR Active? Type
1163 93 A2 Yes out-of-plane bend
1213 14 E' Very slight bend
1213 14 E' Very slight bend
2582 0 A1' No symmetric stretch
2715 126 E' Yes asymmetric stretch
2715 126 E' Yes asymmetric stretch
BH3 Molecule



NH3



Item               Value     Threshold  Converged?
 Maximum Force            0.000005     0.000450     YES
 RMS     Force            0.000003     0.000300     YES
 Maximum Displacement     0.000012     0.001800     YES
 RMS     Displacement     0.000006     0.001200     YES

File:RUUMAAAAAN NH3 FREQIII.LOG

Low frequencies ---  -11.6527  -11.6490   -0.0048    0.0332    0.1312   25.5724
Low frequencies --- 1089.6616 1694.1736 1694.1736


NH3 Molecule



NH3BH3

         Item               Value     Threshold  Converged?
 Maximum Force            0.000041     0.000450     YES
 RMS     Force            0.000014     0.000300     YES
 Maximum Displacement     0.000603     0.001800     YES
 RMS     Displacement     0.000278     0.001200     YES



E(NH3)=-56.55776863 E(BH3)=-26.61532363 E(NH3BH3)=-83.22468929

ΔE=E(NH3BH3)-[E(NH3)+E(BH3)] ΔE=-83.22468929 - (-26.61532363+-56.55776863) ΔE=-0.05159au =-135kJ/mol

This energy is quite weak for a covalent bond.

Smf115 (talk) 08:10, 17 May 2018 (BST)Good consideration of the accuracy of reported energy values and correct calculation.

BH3NH3 Molecule


BBr3

Item               Value     Threshold  Converged?
 Maximum Force            0.000008     0.000450     YES
 RMS     Force            0.000005     0.000300     YES
 Maximum Displacement     0.000036     0.001800     YES
 RMS     Displacement     0.000023     0.001200     YES


Low frequencies ---   -0.0137   -0.0064   -0.0046    2.4315    2.4315    4.8421
 Low frequencies ---  155.9631  155.9651  267.7052
BBr3 Molecule


BBr3 DOI:10042/202327

Project section

Benzene

         Item               Value     Threshold  Converged?
 Maximum Force            0.000196     0.000450     YES
 RMS     Force            0.000096     0.000300     YES
 Maximum Displacement     0.001062     0.001800     YES
 RMS     Displacement     0.000381     0.001200     YES
Low frequencies ---  -16.9577  -14.2980   -9.2699   -0.0012   -0.0005   -0.0005
Low frequencies ---  413.7998  414.4799  620.8650
Benzene


Borazine


Item               Value     Threshold  Converged?
 Maximum Force            0.000117     0.000450     YES
 RMS     Force            0.000036     0.000300     YES
 Maximum Displacement     0.000327     0.001800     YES
 RMS     Displacement     0.000104     0.001200     YES
Low frequencies ---  -11.3791    0.0008    0.0011    0.0014    9.0995   10.8730
Low frequencies ---  288.5041  290.3971  404.0139


Borazine


Benzene and Borazine MO comparison
Benzene----------------------------------------Borazine Comparison
MO 22 is similar for both structures and shows out of phase p orbitals. However, borazine’s orbitals are more distrorted than that of bezenes due to different sized p orbitals between atoms. Each atom on borazine has less contribution to the MO than that of benzene. Due to this, the MO of borazine is higher in energy 0.02422 Hartrees (64KJ/mol), whilst benzenes MO has an energy of 0.00267 Hartrees (7KJ/mol).
MO 17 is very similar for both molecules. This MO features all in phase pi orbitals bonding together, showing the delocalisation present within the structures. The Borazine MO is slightly more contracted at the nitrogen atoms, due to the higher electronegativity of nitrogen compared to borane. As we expect borazine is slightly lower in energy at -0.36130 Hartrees (-947KJ/mol). Whilst benzene has an energy of -0.35998 Hartrees (-945KJ/mol)
MO 14 for benzene and MO 15 for borazine both show out of phase sigma orbitals with lobes present at the atomic centres. MO 14 has an energy of -0.43854 Hartrees (-1151KJ/mol), whilst MO 15 on borazine is -0.43198 Hartrees (-1134KJ/mol).
For benzene the charge is symmetrical distributed, showing all the hydrogens having the same positive value of 0.239, and all carbon atoms having the same slightly negative value of +0.239.

Borazine shows an uneven distribution of charge. The nitrogen atoms (red) have the lowest charge of -1.102 with it hydrogens atoms having charges of +0.432. Whilst boron (light green) has a positive charge of 0.747 with it hydrogen molecules having a charge of -0.077. The positive charge on the boron is due to the fact that it is bonded to the highly electronegative nitrogen atom, shifting electron density onto the nitrogen, making the nitrogen more negative and the boron more positive. Furthermore, boron donates electron density towards its hydrogen atoms, thereby allowing the hydrogens to experience a slight negative charge.

Smf115 (talk) 08:15, 17 May 2018 (BST)Good attempt at the charge analysis with mention of symmetry and electronegativity. Smf115 (talk) 08:15, 17 May 2018 (BST)Nice range of MOs chosen, however, the energies of the MOs can't be compared. Good mention of electronegativity however, the overall character and mention whether they were sigma- or pi- orbitals should have been made for a better comparison.

Aromatic molecules have a ring of resonance bonds that provide more stability than similar geometric arrangements of structures containing the same set of atoms. Compounds can be classed as aromatic if they have 4n+2 pi electrons. This is known as Huckle’s rule and therefore can be used to prove that aromatic molecules do not have to be planar. For example, the aromatic compound cyclooctatetraene conforms to a non-planar ‘tub’ conformation, and has 8 pi electrons. Aromaticity is commonly thought to arise from its 6 Pz orbitals which form a pi bond, leading to the formation of a delocalised ring of electron density above and below the ring. However, sigma orbitals can contribute to this delocalisation ring, and in few cases, only some fragments from p orbitals can be thought to contribute to this system.

Smf115 (talk) 08:15, 17 May 2018 (BST)Nice cover of the basic conceptes of aromatiticty. However, the discussion is a bit brief and mention of more complex ideas, such as sigma-aromaticty, and reference to MOs is needed to develop it further.

Smf115 (talk) 08:15, 17 May 2018 (BST)Overall a good attempt at the report and project section.