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Spectroscopy
| Front | Back |
|---|---|
| Interaction of light and matter | light is made of photons when dealing with the interaction of light and matter we treat light as a wave electromagnetic (EM) radiation has both a frequency and wavelength |
| frequency (v) | number of waves produced by a source each second measured in Hertz (Hz) or s-1 |
| wavelength (λ) | distance between a point on one wave and the same point on the next wave measured in metres (m) wavenumber (cm-1) = 1/λ (cm) |
| equation | velocity (c) = frequency (v) x wavelength (λ) |
| equation | energy (E) = frequency (v) x Planck's constant (h) |
| infrared and raman spectroscopy | wavelength will be in the range from 400nm to 100,000nm this covers the visible and infrared regions of the electromagnetic spectrum |
| motion in molecules | 3 diff ways molecules move: - translation (movement in 3 dimensions) - rotation (movement about an axis) - vibration (movement on a bond) |
| atoms in molecules | all molecules have 3N degrees of freedom, where N is the number of atoms - translation uses 3 - rotation 2 or 3 - vibration uses the rest |
| vibrational modes | linear molecules e.g. H2 and CO2 have 3N - 5 vibrational modes Non-linear molecules e.g. H2O have 3N - 6 vibrational modes |
| Motion requires energy | Translation requires the least (kinetic) Rotation requires more (equivalent to microwave wavelength) Vibration requires even more (equivalent to infrared wavelength) |
| vibration in molecules | absorption of infrared radiation causes covalent bonds within molecules to vibrate a molecule is only able to absorb radiation whose energy corresponds to the energy difference: E1 - E0 |
| vibration in molecules | most molecules have many covalent bonds hence infrared and raman spectra provide detailed info on molecular structure bond vibrations that result in absorption of infrared radiation are either stretching or bending vibrations |
| modes of vibration in molecules | - symmetric stretch - asymmetric stretch - twisting - wagging - scissoring - rocking |
| IR active or inactive? | not all vibrations in molecules can be seen by IR spectroscopy only those termed as IR active will be visible |
| selection rules for IR | gross selection rule - vibration must result in a change in the molecular dipole moment specific selection rule - the change in vibrational energy level must be Δν = ±1 |
| examples of ir active or inactive | symmetric stretch - not infrared active symmetric stretch - not infrared active assymetric stretch - infrared active |
| absorption | large change in dipole moment e.g. C=O results in an intense absorption small change in dipole moment e.g. C=C results in a weak absorption |
| interpreting IR spectra | the structure of an unknown molecule is not determined just by using IR IR can be used for identifying certain functional groups but is complimentary to other techniques |
| advantages of IR spectroscopy | - little sample prep required - can handle any state of sample - identifies functional groups |
| disadvantages of IR spectroscopy | - not usually quantitative - low sensitivity - cannot detect IR inactive impurities |
| raman spectroscopy | when radiation passes through a transparent medium, most of it is elastically scattered (Rayleigh scattering) - this is where light is scattered at same frequency to the incident radiation |
| raman spectroscopy | one in a million photons are inelastically scattered (Raman scattering) - light is scattered at different frequency to the incident radiation - use high-powered lasers |
| stokes emission | - decrease in frequency = stokes emission - increase in frequency = anti-stokes emission typically we see stokes emission since anti requires the molecule to be in an excited state initially |