e10 Infrared

Embed Size (px)

Citation preview

  • 7/29/2019 e10 Infrared

    1/5

    E10 INFRARED & RAMAN SPECTROMETRY : Principles &

    INSTRUMENTATION

    KEY NOTES

    Principal:-Vibrational Transition In Molecules Cause Absorption In The Infrared

    Region Of The Electromagnetic Spectrum. They may also be studied using the

    technique of raman spectrometry, where they scatter exciting radiation with an

    accompanying shift in its wavelength.

    Group Frequencies:- Vibrational Spectra Give Information About The

    Functional Groups In Molecules, And The Observed Group Frequencies Are

    Affected By Molecular Interactions Such As Hydrogen Bonding.

    Instrumentation:- Infrared And Raman Instruments Include A Radiation Source, A

    Means Of Analyzing The Radiation And Detection And Data Processing System.

    Additionally, sampling methods to deal with gases, liquids, solids, micro samples

    and mixtures are available.

    Related topics :-Infrared And Raman Spectrometry

    Applications (E 11)

    Gas chromatography infrared

    Spectrometry (F4)

    Principles:- The vibrational levels of molecules are separated by energies in the

    infrared (1R) region of the electromagnetic spectrum. That is, in the wavenumberrange from 13000 to 10 cm, or between0.8 and 1000 um on the wavelength scale

    .For convenience, this large region is divided into near IR, or NIR (13000-4000cm-

    1), mid IR(4000-400cm-1) and far IR (400-10cm-1).

  • 7/29/2019 e10 Infrared

    2/5

    Molecules contain bonds of specific spatial orientation and energy. These bonds

    are seldom completely rigid, and when energy is supplied, they may bend, distort

    or stretch. A very approximate model compares the vibration to that of a

    harmonic oscillator, such as an ideal spring. If the spring has a force constant, k,

    and masses m at the ends, then the theoretical vibration frequency v is given by:

    V=(1/2n) (k/)

    Where =m m /(m + m ) is called the reduced mass.

    Each type of molecular vibration is characterized by a vibrational quantum

    number, v. For a simple stretching vibration, there is a series of levels whose

    energy is given approximately by

    E=hv ,(v+1/2)

    This means there is a set of levels spaced in energy by hv or in wavenumber by v .

    The selection rule for an ideal harmonic oscillator allows transitions where

    Av =+_1, giving a single, fundamental vibrational absorption peak.

    However, when bonds are stretched they weaken, so a better model takes this

    into account, and the molecules are treated as anharmonic oscillators. This where

    high energies are involved, large energy transition may occur, where v = +2, +3,etc, giving the first overtone at a wavenumber approximately

    double that of the fundamental, & so on.

    The electrical field associated with the electromagnetic radiation will interact with

    the molecules to change its electrical properties. Some molecules (for example,

    HCI) have a dipole moment due to change separation & will interact with the field

    others may acquire a dipole when they vibrate, for example, molecules, CH4 HAS

    No Dipole, But When One Of The Ch Bonds Stretched, The molecules will develop

    a temporary dipole.

    even if the molecules does not have a dipole, the electric fields ,E, may distort the

    electron distribution and polarize the molecules

    =a E

  • 7/29/2019 e10 Infrared

    3/5

    where is the dipole induced by fields ,E and a is the polarizability of the

    molecules

    The rules governing transitions in the infrared region of the spectrum require that

    ,in order to absorb, the dipole of molecule must change during the vibration.Such vibrations said to be IR active. For transitions to be active in the Raman

    region, it is required that the polarizability must change using the vibration. The

    transitions are then Raman active, or R active (fig. 1).

    Consider two simple diatomic molecules, nitrogen and carbon monoxide. These

    molecules have only one fundamental vibration frequency, vo. For nitrogen it is

    2360 cm-1, and for carbon monoxide 2168 cm-1.

    Since carbon monoxide has a permanent dipole, which will increase and decrease

    as he molecule stretches and compresses, the vibration will interact with IR

    radiation, and an absorption peak will be observed close to 2168 cm-1. Nitrogen

    has no dipole, and vibration does not produce one. Therefore, it will not absorb IR

    radiation. This is of great importance, since IR spectra may be recorded in air

    without interference.

    However, when the nitrogen molecule vibrates, he bonding electrons are

    distorted and the polarizability is changed. Therefore, it will give a spectrum usingthe Raman technique.

    In order to excite Raman transitions, energy comparable to the difference

    between electronic energy levels must be supplied. This may be visible laser light

  • 7/29/2019 e10 Infrared

    4/5

    or NIR radiation. If the exciting wavelength matches the energy difference

    between the electronic levels of the sample, the Raman signal is greatly

    enhanced by the resonance Raman effect. Rayleigh scattering re-emits the

    exciting line. There ore intense emission due to fluorescence effects may mask

    the weak Raman signal, but with NIR radiation fluorescent interference is much

    less.

    As molecules become more complex. The number of possible vibrations

    increases. For example, carbon monoxide, co2 , has three atoms arranged in a

    line: O=C=O. this molecule does not have a dipole and may vibrate in three ways.

    I. The symmetric stretch, denoted by v is where both oxygen are equidistantfrom the central carbon, but the C-O bonds lengthen and contact together.

    The dipole does not change, but the polarizability does . so this vibration is

    IR inactive, but R active.

    II. The antisymmetric stretch, v has one C-O bond stretching, while the othercontact. The carbon atom moves as well so that the centre of mass of the

    molecules remains stationary. The dipole changes but the polarizability

    does not so this is IR active but R active

    III. The bending vibrations may be resolved into two identical and mutuallyperpendicular components corresponding to two transitions of the sameenergy ( degenerate ). It is necessary to think in three dimension:

    considering the page as plane, then if the two oxygen go equally down the

    page while the carbon goes up the page to balance this is in plane bending

    .if the oxygen go into the page the carbon out of the page this is out of

    plane bending. These changes will be reversed as the vibration progresses .

    This vibration is IR active R inactive

    The triangular molecule of water HO also has three different vibration

    corresponding to the same vibrational types. However each involved change in

    dipole so all three are IR active. The Raman spectrum shows only one line due

    to the symmetric stretch. These vibrations are shown schematically in figure 2.

    It is possible to extend these arguments to more complex molecules, but this is

  • 7/29/2019 e10 Infrared

    5/5

    only of value for student of structural parameters such as the length and