160 likes | 259 Views
Single points Opt, Freq Single points. Basis set. HF/3-21G HF/6-31G(d) HF/6-31G(d,p) HF/6-311++G(3df,2p) Collect the electronic energies. Correlation Methods. HF/3-21G MP2/3-21G MP3/3-21G MP4/3-21G QCISD/3-21G QCISD(T)/3-21G
E N D
Basis set • HF/3-21G • HF/6-31G(d) • HF/6-31G(d,p) • HF/6-311++G(3df,2p) Collecttheelectronicenergies
Correlation Methods • HF/3-21G • MP2/3-21G • MP3/3-21G • MP4/3-21G • QCISD/3-21G • QCISD(T)/3-21G Collecttheelectronicenergiesfrom output files.
Opt C2H5OH design • Gaussview • Gaussian Gaussview HF/6-31G(d) Comparision energy from Single point calcs. with optimised electronic energy
Absorption • vertical (or Frank-Condon) excitation • 0 - 0’ (or adiabatic) excitation UV-VIS IR
Translations (a) and rotations (b) of H2O. The normal vibrations of the H2O molecule. The fundamental frequencies of the three modes of motions are denoted as , (symm
In general, the 3n-6 vibrational modes can be subdivided into three types of deformations: stretch, bend and torsion (see for example Figures 1.6 and 1.11). The approximate potential energy functions associated with these three types of modes of motion are shown, again schematically, Three types of potentials associated with three types of internal modes of motion. The energy requirement is the greatest for the stretch and the smallest for the torsion. Therefore, these three types fall into three different frequency ranges, even though there is some overlap Overlapping frequency ranges for stretching, bending and torsional modes of vibration.
Characteristic stretching and bending frequencies of the most frequently occurring functional groups are shown in Table 13.3. The torsional frequencies (included in Table 13.3) are usually below 100cm-1.
Design of the Transition State • C2H5OH
Energy difference • ETS – Eeq
Reaction enthalpy • Products: H2O and C2H4