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ZQR01333824

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Small molecules

BH3 Molecule

Basic Information

Calculation method:RB3LYP

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

Summary table

Summary table of optimised BH3 molecule















Item table

        Item               Value     Threshold  Converged?
Maximum Force            0.000011     0.000450     YES
RMS     Force            0.000006     0.000300     YES
Maximum Displacement     0.000043     0.001800     YES
RMS     Displacement     0.000022     0.001200     YES



Frequency log file

Media:ZQR-BH3_FERQ.LOG


Low frequency table

Low frequencies ---  -14.6858  -14.6818  -11.0436   -0.0009    0.0165    0.3415

Low frequencies --- 1162.9492 1213.1220 1213.1222

J mol file

BH Molecule


Vibrational spectrum for BH3

wavenumber (cm-1) Intensity (arbitrary units) symmetry IR active? type
1163 92 A2 Yes out-of-plane bend
1213 14 E' Yes bend
1213 14 E' Yes bend
2583 0 A1 no symmetric stretch
2716 126 E' Yes asymmetric stretch
2716 126 E' Yes asymmetric stretch

IR spectrum of BH3

IR spectrum of BH3























Question

A: There are only three peaks on IR spectrum, which represents mode 1, mode 2 & 3 and mode 5 & 6. Mode 1 is IR active because there is change in dipole moment. Mode 2 and mode 3 are degenerate so they show as one peak. Same for mode 5 and 6 since they are also degenerate. Mode 4 is IR inactive because there is no net change in dipole moment.


MO diagram of BH3

MO diagram of BH3






























Reference: Hunt P. Lecture_4_Tut_MO_diagram_BH3. Inorganic Lecture Course; 2019.

Question

Q1 A: The real Mo is calculated by computer, it shows the real size, fragmentation of orbitals and the exact way they mix. LCAO is formed by combination of atomic orbitals, the exact size cannot be predicted accurately.

Q2 A: Qualitative Mos are only useful to predict the size and shape orbitals for small molecules, For more complex Mos, calculation is needed to get the accurate prediction.


Correct inclusion of the calculated MOs on to the MO diagram. Your evaluation of the usefulness of the LCAO approach is ok but to improve, you could have discussed the similarities and differences in more detail, for example, consider the differences in orbital contributions in the 3a1' or 2e' MOs. Smf115 (talk) 14:46, 2 June 2019 (BST)

NH3 Molecule

Basic Information

Calculation method:RB3LYP

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

Summary table

Summary table of optimised frequency NH3 molecule

















Item table

         Item               Value     Threshold  Converged?
 Maximum Force            0.000006     0.000450     YES
 RMS     Force            0.000003     0.000300     YES
 Maximum Displacement     0.000013     0.001800     YES
 RMS     Displacement     0.000007     0.001200     YES

Frequency log file

Media:ZQR_NH3_1_OPT_FREQ2.LOG


Low frequency table

Low frequencies ---   -0.0129   -0.0018    0.0001    7.0724    8.1020    8.1023
Low frequencies --- 1089.3849 1693.9369 1693.9369

J mol file

NH Molecule

NH3BH3 Molecule

Basic Information

Calculation method:RB3LYP

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

Summary table

Summary table of optimised NH3BH3 molecule
















Item table

         Item               Value     Threshold  Converged?
 Maximum Force            0.000350     0.000450     YES
 RMS     Force            0.000112     0.000300     YES
 Maximum Displacement     0.001347     0.001800     YES
 RMS     Displacement     0.000450     0.001200     YES


frequency log file

Media:ZQRNH3BH3_FREQUENCY.LOG

Low frequency table

Low frequencies ---   -0.0265   -0.0066   -0.0053   10.4126   10.4592   38.3629
Low frequencies ---  265.3603  634.4262  639.2330

J mol file

BH Molecule



Association energy

E of BH3 = -26.61532 a.u.

E of NH3 = -56.55777 a.u.

E of NH3BH3 = -83.22469 a.u.

ΔE= -83.22469-(-26.61532-56.55777) = -0.05160 a.u. = -135 kJ/mol

B-N dative bond is relatively weak compared to C-C bond which is equal to 346 KJ/mol

Correct calculation, good consideration given to the accuracy of the final reported energy values and ok comparison made. To improve, you could have considered why the C-C bond is a good comparison and always include a reference for literature values! Smf115 (talk) 14:48, 2 June 2019 (BST)

NI3 Molecule

Basic Information

Calculation method:RB3LYP

Basis set:Gen

Summary table

Summary table of optimised BH3 molecule















Item table

Item               Value     Threshold  Converged?
 Maximum Force            0.000096     0.000450     YES
 RMS     Force            0.000075     0.000300     YES
 Maximum Displacement     0.000860     0.001800     YES
 RMS     Displacement     0.000613     0.001200     YES

frequency log file

Media:23NI3FREQ3.LOG


Low frequency table

Low frequencies ---  -12.7408  -12.7347   -6.4001   -0.0039    0.0188    0.0622
Low frequencies ---  101.0654  101.0662  147.4490

J mol file

NH Molecule


Correct implementation of the pseudopotential and good structure information, however, you are missing the bond length for the molecule. Smf115 (talk) 14:51, 2 June 2019 (BST)

Mini Projects: Ionic liquids

[N(CH3)4]+ Molecule

Basic Information

Calculation method:RB3LYP

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

Summary table

Summary table of optimised [N(CH3)4]+ molecule















Item table

         Item               Value     Threshold  Converged?
 Maximum Force            0.000030     0.000450     YES
 RMS     Force            0.000018     0.000300     YES
 Maximum Displacement     0.000201     0.001800     YES
 RMS     Displacement     0.000116     0.001200     YES

Frequency log file

Media:ZQROPTNCH34_FREQ1.LOG

Low frequency table

Low frequencies ---   -0.0013   -0.0011   -0.0008   21.4310   21.4310   21.4310
 Low frequencies ---  188.2136  292.4076  292.4076


J mol file

BH Molecule

[P(CH3)4]+ Molecule

Basic Information

Calculation method:RB3LYP

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

Summary table

Summary table of optimised [P(CH3)4]+ molecule















Item table

         Item               Value     Threshold  Converged?
 Maximum Force            0.000046     0.000450     YES
 RMS     Force            0.000031     0.000300     YES
 Maximum Displacement     0.000507     0.001800     YES
 RMS     Displacement     0.000448     0.001200     YES

Frequency log file

Media:ZQRPCH3411FREQUENCY.LOG

Low frequency table

Low frequencies ---   -0.0022    0.0013    0.0025   26.7152   26.7152   26.7152
 Low frequencies ---  161.3609  195.7728  195.7728

J mol file

NH Jmol

Charge distribution

Charge distribution of [P(CH3)4]+ Colour range -0.50 t0 0.50
Charge distribution of [N(CH3)4]+ Colour range -0.50 t0 0.50



Charge on [P(CH3)4]+: P=+1.666, C=-1.050, H=+0.298.

Charge on [N(CH3)4]+: N=-0.295, C=-0.483, H=+0.269.


For [P(CH3)4]+, phosphorous is more electropositive than carbon hence most of the positive charges are concentrated on phosphorous.Therefore, the negative charges are concentrated on carbon atoms.



For [N(CH3)4]+, nitrogen is more electronegative than carbon. Therefore, the negative charge density is concentrated around nitrogen. Since carbon is also electron negative than hydrogen, the positive charge is concentrated on hydrogen atoms.

Correct NBO charges calculated and good use of a uniform colour range across both ILs, however, it should have been larger to properly show the differences between the charges. Your analysis of the charge distributions is minimal and you haven't considered the question about the +1 formal charge on the N in the traditional picture. Smf115 (talk) 20:49, 4 June 2019 (BST)

MO diagrams

Good construction of the FOs and the corresponding LCAOs, however, the last LCAO could have been drawn consistently with the other two. To improve, you could have made some attempt to consider the character of each of the MOs chosen to illustrate the range chosen. Smf115 (talk) 20:53, 4 June 2019 (BST) Overall, an ok report which could be improved by more analysis in the project section. Smf115 (talk) 20:53, 4 June 2019 (BST)
Real MO LCAO
No.9 MO
LCAO of No.9
No.10 MO
LCAO of No.10
No.17 MO
LCAO of No.17