Wave Properties of Electromagnetic Radiation

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Wave Properties of Electromagnetic Radiation Two options are available for analytical utility when an analyte interacts with a beam of electromagnetic radiation in an instrument 1. We can monitor the changes that occur in the radiation after the interaction, or In this case, wave properties of the electromagnetic radiation is useful in understanding analytical interpretations Upon interaction with matter, electromagnetic radiation can undergo: diffraction, transmission, refraction, reflection, scattering, etc. 2. We can study the changes that occur in the analyte itself Such changes are quantized, and are utilized in most Spectrochemical methods

Wave Properties of Electromagnetic Radiation plane-polarized wave Oscillation of only the electric field The electric field is responsible for most phenomena that are of interest in chemical instrumentation The magnetic field is responsible for radio frequency absorption in NMR spectroscopy

Diffraction of Radiation

Transmission of Radiation Interactions involved in transmission is attributed to periodic of atoms or molecular species that make up the medium polarization polarization refers to temporal deformation of electron clouds associated with atoms and molecules that is brought about the alternation electromagnetic field The energy required for the polarization is momentarily retained (10-15 seconds) by the species involved, and is re-emitted as the substance returns to it s original state No energy is absorbed, but the rate of propagation of the radiation is slowed by the time needed for retention and re-emission to occur.

Transmission of Radiation Refractive Index (n i ): n i = C v i n i = refractive index at specific frequency, i v i =velocity of the radiation in the medium c = velocity in vacuum Dispersion variation of refractive index with frequency or wavelength Normal Dispersion: gradual increase in n i with frequency Anomalous Dispersion: sharp changes in n i with frequency At such frequencies, permanent energy transfer occur, and absorption of the beam is observed Instrumental Significance A material that exhibit normal dispersion is good for the manufacturing of lenses A material that exhibit anormalous dispersion is highly frequency dependent, and is selected for fabrication of prisms

Refraction of Radiation Refraction: The change in direction as a beam passes one medium to the other is a consequence of differences in velocity (v) of the radiation n the two media that have different densities (n) Snell s law: sinθ 1 sinθ 2 = n 1 n 2 = v 1 v 2 n vac = 1.0027n air

Reflection of Radiation I r = (n 2 n 1 ) 2 I o (n 2 + n 1 ) 2 Reflection always occurs when a beam crosses an interface between media that differ in refractive index The fraction of reflected radiation increases with increasing differences in refractive index

Scattering of Radiation Transmission of radiation momentary retention of the radiant energy by matter, followed by reemission of the radiation in all directions For small molecules path of beam appears to be unchanged as a consequence of destructive interference For large molecules destructive interference is incomplete, and small fraction of the emitted radiation is transmitted at all angles. Intensity of the scattered beam increases with particle size. Rayleigh Scattering: o Scattering of light by molecules significantly smaller than the wavelength of the radiation Mie Scattering: o With large molecules, scattering can be different in different directions. o Measurement of type of scattered radiation is used to determine the size and shape of large molecules, including colloidal particles Raman Scattering: o The Raman scattering effect differs from ordinary scattering in that part of the scattered radiation suffers quantized frequency changes o These changes are the result of vibrational energy level transitions that occur in the molecule as a consequence of the polarization

Spectrochemical method Focuses on the measurement of the amount of radiation produced or absorbed by molecular or atomic species of interest Classified according to the region of the electromagnetic spectrum involved: X-ray, ultraviolet (UV), visible, infrared (IR), microwave, and radio frequency (RF) The absorbed or emitted radiation is quantized! Type of quantum change: Type spectroscopy:

UV-Visible Spectroscopy Principle Required radiation wavelength: 200 700 Electrons in bonds within the molecule under electronic transitions to occupy higher energy states through absorption of the UV-Vis radiation Loosely bound electrons (lone pairs and π-electrons) are most susceptible to this radiation these types of compounds are usually colored Strengths Sensitive Easy to use, cheap and robust, good for quantitation Routine method for many industrial applications Limitation Moderately selective Not specific Not applicable for mixture analysis

Infrared (IR) Spectroscopy Principle Required radiation wavelength: 500 4000 cm -1 Bonds within the molecule under vibrational transitions through stretching and bending modes Strengths Provides complete fingerprint unique to compound under investigation Applicable to solids, liquids and gases Limitation Not quantitative Requires extensive sample preparation Not sensitive Technique is lacking mainly because sample handling has huge effect on the resulting spectrum Main Applications Authentication of raw materials Used as preliminary check for the presence or absence of a particular functional group

Atomic Absorption Spectroscopy (AAS) Principle Ground state gaseous atoms are produced by vaporization The atoms are exposed to specific line radiations generated by a lamp made from the particular metal under investigation Change is intensity of the light from the lamp is measured Strengths Highly specific Quantitative Limitation Applicable to only metals Each element requires a different lamp for its determination

Fluorescence Spectroscopy Principle Certain molecules containing chromophore and rigid structure can be excited by UV/vis radiation, and will then emit the radiation absorbed at a longer wavelength The emitted radiation can be measured Strengths Selective detection Very sensitive due to high signal-to-noise ratio Quantitative Widely used in bioanalysis Limitation Applicable to only limited number of molecules Subject to interference including the presence of heavy metal ions, UV absorbing species, and temperature changes

General Instrumentation for Spectrochemical Methods Source of Radiation Wavelength Selector Sample Containers Transducers Measurement Systems