Analysis of spectroscopic and theoretical results of compounds with intermolecular hydrogen bonding
Supervisor: prof. Aleksander Filarowski
Gabriela Drabik SUMMER STUDENT PRACTICE JINR 2014
Jagiellonian University in Krakow Poland
Analysis of spectroscopic and theoretical results of compounds with - - PowerPoint PPT Presentation
Analysis of spectroscopic and theoretical results of compounds with intermolecular hydrogen bonding Supervisor : prof. Aleksander Filarowski Gabriela Drabik Jagiellonian University in Krakow Poland SUMMER STUDENT PRACTICE JINR 2014 The
Supervisor: prof. Aleksander Filarowski
Jagiellonian University in Krakow Poland
The hydrogen bond definition: The hydrogen bond is an attractive interaction between a hydrogen atom from a molecule or a molecular fragment X–H in which X is more electronegative than H, and an atom or a group of atoms in the same or a different molecule, in which there is evidence of bond formation.
Pure Appl. Chem., Vol. 83, No. 8, pp. 1637–1641, 2011
,,The hydrogen bond is the most important of all directional intermolecular interactions. It is operative in determining molecular conformation, molecular aggregation, and the function of a vast number of chemical systems ranging from inorganic to biological”.
.2 .4 .6 .8 Absorbance 3000 2000 1000 Wavenumber (cm-1) .2 .4 .6 .8 Absorbance 3000 2000 1000 Wavenumber (cm-1)
IR spectra: Left: 2,4,6-tri-Cl-phenol (no hydrogen bond); right: 2,4,6-tri-Cl-phenol + N-benzyldenomethylamine (hydrogen bonding occurence). Asterix: stretching mode of the X-H bonding.
* * IR
Example
Selection rules:
In general, molecular vibrations symmetric with regard to the centre of symmetry are forbidden in the infrared spectrum, whereas molecular vibrations which are antisymmetric to the centre
exclusion.
Example
Selection rules:
dipole momentum µ in a molecule is changed during the normal vibration. The intensity of an infrared absorption band IIR depends on the change of the dipole moment µ during this vibration where q is the normal coordinate.
Example
Selection rules:
polarizability a in a molecule is changed during the normal vibration. The intensity of a Raman active band IRaman depends on the change
where q is the normal coordinate.
The main contribution to the incoherent neutron scattering comes from the interaction of the atom and neutron spins and from the random isotope distribution in the sample
Ei, Ef – energy of the incident and scattered neutrons ki, kf – wave vectors of the incident and scattered neutrons
Cross sections [b]:
Double differential crossection: describes the density of the probability, that the incident neutron with energy: is scattered by an angle: θ, within the solid angle element: dΩ=2sinπθdθ, and into the energy range: from hω’ to h(ω’+dω’). Fourier transform of the correlation function of the nuclei pairs and describes the collective motion of atoms and molecules Fourier transform of the autocorrelation function of atomic nuclei and describes individual atomic and molecular movements
The S(Q,w) function is named the scattering law. It depends only on structural and dynamical properties of a system. Where: Mean square displacement:
SAMPLE
Inverted geometry time-of-flight spectrometer NERA at the IBR-2 high flux pulsed reactor in Dubna
I.Natkaniec, S.I.Bragin, J.Brankowski and J.Mayer, in Proc. ICANS XII Meeting, Abington 1993, RAL Report 94-025, vol.I.,p.89- (1994).
Energy of the unscattered neutron beam (Ei) Change of the neutron energy upon inelastic scattering
Lf1 Lf2
Change of the momentum upon inelastic scattering
Lf1 Lf2
INS IR and Raman
the molecule
and on the amplitude of the vibration of an particular atom
low frequency internal modes
(hydrogen bonding dynamics)
1000 2000 3000
wavenumber, cm
1000 2000 3000 1000 2000 3000
absorbance
1000 2000 3000
IR SPECTRA (GAZ) IR SPECTRA (GAZ)
B3LYP/6-31G(d,p) MP2/6-31G(d,p)
O H N C H CH3 O D N C H CH3
100 200 300 400 500 600 700 250 500 750 1000 1250 , cm-1 Q( ) [a. u.]
O H N C CH3 CH3 O D N C CD3 CH3
100 200 300 400 250 500 750 1000 1250 , cm-1 Q( ) [a. u.]
O H N C H CH3 O D N C H CH3
IINS IR and QM
Antigen – antibody recognition DNA structure Protein structure
(Chalmers J., Griffiths P. R. eds), J. Wiley & Sons Ltd, 2002, Vol. 1, pp 838-852
1993, Vol. 1, p.89
molecular vibrations, Trends in Applied Spectroscopy Vol. 5 , 2004
materii, WN UAM 2013