Chapter 18 Fundamentals of Spectrophotometry Properties of Light

Chapter 18 Fundamentals of Spectrophotometry Properties of Light

Chapter 18 Fundamentals of Spectrophotometry Properties of Light Electromagnetic Radiation – energy radiated in the form of a WAVE caused by an electric field interacting with a magnetic field – result of the acceleration of a charged particle – does not require a material medium and can travel through a vacuum 1 Properties of Electromagnetic Radiation ν λ vi = i where vi => velocity ν => frequency λ i => wavelength Properties of Electromagnetic Radiation in vacuum, velocity is independent of frequency, maximum value 8 c = νλ = 2.998 10 m/s 2 Properties of Electromagnetic Radiation Fig. 19-1, pg. 511 ”Plane-polarized electromagnetic radiation of wavelength λ, propagating along the x axis. The electric field of the plane-polarized light is confined to a single plane. Ordinary, unpolarized light has electric field components in all planes." Regions of Electromagnetic Spectrum 3 Line Spectrum A spectrum produced by a luminous gas or vapor and appearing as distinct lines characteristic of the various elements constituting the gas. 4 Emission Spectrum The spectrum of bright lines, bands, or continuous radiation characteristic of and determined by a specific emitting substance subjected to a specific kind of excitation. Ground State The state of least possible energy in a physical system, as of elementary particles. Also called ground level. 5 Excited State Being at an energy level higher than the ground state. 6 Absorption Spectrum • Light shinning on a sample causes electrons to be excited from the ground state to an excited state • wavelengths of that energy are removed from transmitted spectra Absorption and Emission of Light Energy Absorption Emission 7 Absorption Methods, Transmittance T = P/Po where T => transmittance P => power of transmitted radiation Po => power of incident radiation %T = (P/Po)*100 where %T => percent transmittance Absorption Methods, Absorbance A = - log10T = - log10 (P/Po) where A => absorbance 8 Relation Between Transmittance and Absorbance P/Po %T A 11000 0.1 10 1 0.01 1 2 Colors of Visible Light Wavelength Absorbed Observed 380-420 violet green-yellow 420-440 violet-blue yellow 440-470 blue orange 470-500 blue-green red 500-520 green purple 520-550 yellow-green violet 550-580 yellow violet-blue 580-620 orange blue 620-680 red blue-green 680-780 purple green 9 Components of Optical Instruments Rotating mirror Semitransparent mirror P Signal Processor Source Wavelength Selector Sample Detector Readout Po mirrorReference mirror Absorption Spectrometer Emission Flame Photometer Flame Atomic Absorption Spectrometer Fluorescence and/or Scattering Spectrometer Absorption Methods, Beer’s Law A = abc = εbc where a => absorptivity b => path length c => concentration ε => molar absorptivity 10 Beer’s Law A = abc = εbc A c Attenuation of Light 11 Beer’s Law A = abc Path Length Dependence, b Readout Absorbance 0.82 Source Detector 12 Beer’s Law A = abc Path Length Dependence, b Readout Absorbance 0.62 Source b Detector Sample Beer’s Law A = abc Path Length Dependence, b Readout Absorbance 0.42 Source Detector Samples 13 Beer’s Law A = abc Path Length Dependence, b Readout Absorbance 0.22 Source Detector Samples Beer’s Law A = abc Concentration Dependence, c Readout Absorbance 0.82 Source Detector 14 Beer’s Law A = abc Concentration Dependence, c Readout Absorbance 0.62 Source b Detector Sample Beer’s Law A = abc Concentration Dependence, c Readout Absorbance 0.42 Source b Detector Sample 15 Beer’s Law A = abc Wavelength Dependence, a Readout Absorbance 0.82 Source Detector Beer’s Law A = abc Wavelength Dependence, a Readout Absorbance 0.30 Source b Detector 16 Beer’s Law A = abc Wavelength Dependence, a Readout Absorbance 0.80 Source b Detector 17 Simple Spectrometer Relationship of Transmittance and Absorpbance transmittance scale is linear absorbance scale is exponential thus, read transmittance, then calculate absorbance 18 19 20 21.

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