Silber spiegel - SwissEduc
Silber spiegel - SwissEduc
Silber spiegel - SwissEduc
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42<br />
3/04<br />
Mechanisms<br />
Mechanism 1:<br />
ΔV Δ (I (I1<br />
) = V (I ) - V (R)<br />
1<br />
ΔV Δ (TS (TS1<br />
) = V (TS ) - V (R)<br />
1<br />
ΔV Δ A V A V = V (TS (TS1<br />
) - V (I1 )<br />
ΔV Δ (I (I2<br />
) = V (I ) - V (R)<br />
2<br />
ΔV° Δ = V (P) - V (R)<br />
Mechanism 2:<br />
ΔV Δ (TS (TS1<br />
) = V (TS ) - V (R) = ΔV<br />
1 ΔV A ΔV A<br />
ΔV Δ (I (I1<br />
) = V (I ) - V (R)<br />
1<br />
ΔV Δ (TS (TS2<br />
) = V (TS ) - V (R)<br />
2<br />
ΔV Δ A VA V = V (TS ) - V (I )<br />
2 2 1<br />
ΔV Δ (I (I2<br />
) = V (I ) - V (R)<br />
2<br />
ΔV Δ (TS (TS3<br />
) = V (TS ) - V (R)<br />
3<br />
ΔV Δ A VA V = V (TS ) - V (I )<br />
3 3 2<br />
ΔV Δ (I (I3<br />
) = V (I ) - V (R)<br />
3<br />
ΔV Δ (TS (TS4<br />
) = V (TS ) - V (R)<br />
4<br />
ΔV Δ A VA V = V (TS ) - V (I )<br />
4 4 3<br />
ΔV Δ (I (I4<br />
) = V (I ) - V (R)<br />
4<br />
ΔV° Δ = V (P) - V (R)<br />
Mechanism 3:<br />
ΔV Δ (I (I1<br />
) = V (I ) - V (R)<br />
1<br />
ΔV Δ (TS (TS1<br />
) = V (TS ) - V (R)<br />
1<br />
ΔV Δ A V A V = V (TS (TS1<br />
) - V (I1 )<br />
ΔV Δ (I (I2<br />
) = V (I ) - V (R)<br />
2<br />
ΔV° Δ = V (P) - V (R)<br />
V 1<br />
2. Theoretical Background<br />
An introduction to quantum chemistry is<br />
probably best reserved for students having a<br />
background equivalent to at least two or three<br />
semesters of physical chemistry. With help from<br />
the instructor, it should be straightforward to<br />
persuade the students that quantum chemistry<br />
methods can offer important support for<br />
proposing mechanisms. Examples for carrying<br />
out quantum chemical calculations like those<br />
presented here can be found in reference [4].<br />
3. Computational Details<br />
All calculations were carried out at the Restricted Hartree–Fock (RHF) level<br />
and the standard double–zeta 6-31G basis set was used through the Gaussian 98<br />
package on an Athlon processor using the Windows 98 Second Edition operating<br />
system. Full geometry optimizations were calculated on all of the structures<br />
without symmetry restrictions.<br />
Transition states were found using the QST3 algorithm by means of searching<br />
one and only one imaginary frecuency. In order to rationalize the isomerization<br />
process the property considered in this work was the electronic potential energy,<br />
V. V The energy values are given in atomic units called hartrees, so to obtain results<br />
in kcal mol -1 , energy values must be multiplied by 627.5095.<br />
© c+b 3/04