Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p

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Introduction to Spectroscopy (Chapter 6) Electromagnetic radiation (wave) description: Wavelength λ Velocity v Electric Field Strength 0 Amplitude A Time t or Distance x Period p Frequency ν time for 1 λ to pass fixed point # of λ passing per s ν= 1 p Wavenumber ν Velocity v In a vacuum: # of λ per cm ν = 1 λ Distance point on wave travels per second v =ν λ v vacuum = c = 2.99782x10 8 m/s A set of waves with identical (a) freqency (b) phase are called coherent. CEM 333 page 2.1

Frequency is always fixed but velocity can vary! Waves slow down in medium (gas, liquid, solid) so v<c v =ν λ Implies λ decreases in medium Refractive index η= c v 1.00 Equation for Wave E = Asin(ωt +φ) where ω=2πν electric field frequency amplitude phase angular frequency time Wave description explains certain EM radiation phenomena: transmission reflection and refraction diffraction interference scattering polarization CEM 333 page 2.2

Particle Description of Light: Based on quantum mechanics Energy of EM photon: E = hυ = hc λ Postulates of QM: Planck's Constant=6.626x10-34 J s 1. Atoms, ions and molecules exist in discrete energy states only E 0 = ground state E 1,E 2,E 3... = excited states Excitation can be electronic, vibrational or rotational Energy levels for atoms, ions or molecules different. Measuring energy levels gives means of identification - spectroscopy 2. When an atom, ion or molecule changes energy state, it absorbs or emits energy equal to the energy difference E = E 1 E 0 3. The wavelength or frequency of radiation absorbed or emitted during a transition proportional to E E = h ν = h c λ CEM 333 page 2.3

Emission Spectra Plot of emission intensity vs. ν or λ called emission spectrum Atom: Atomic Excitation E 2 Atomic Emission Lifetime~1-100 ns E 1 Energy E 0 line emission spectra E=202.8 kj/mol 14 ν=5.08x10 Hz λ=590 nm E=362.5 kj/mol 14 ν=9.08x10 Hz λ=330 nm Inner shell (core) electrons (1s 2p) - x-rays photons Outer shell (valence) electrons (3d 4p) - UV/vis photons Molecule: Molecular Excitation E 2 Molecular Emission E 1 Energy R 10 V 3 R 0 E 0 Band 1 Band 2 V 2 V 1 V 0 Lifetime 1-100 fs vibrational and rotational transitions - band emission spectra CEM 333 page 2.4

Emission spectrum of brine (Fig. 6-15): CEM 333 page 2.5

Ballpark Energy Level Spacings: E (Electronic) >100 MJ/mol (x-ray) to <100 kj/mol (UV-vis) E (Vibrational) <1 to <100 kj/mol (IR) E (Rotational) 10-100 J/mol (microwave) Continuum Spectra: Very broad band spectra in emission from solids Produced by blackbody radiation - thermal excitation and relaxation of many vibrational (and rotational) levels. Blackbody Spectrum (Fig 6-18) CEM 333 page 2.6

Absorption Spectra Plot of Absorbance vs. ν or λ called absorption spectrum Just as in emisson spectra an atom, ion or molecule can only absorb radiation if energy matches separation between two energy states Atoms: No vibrational or rotational energy levels - sharp line spectra with few features For example: Na 3s 3p 589.0, 589.6 nm (yellow) Na 3s 5p 285.0, 285.1 nm (UV) Visible enough energy for valence (bonding) excitations UV and x-ray enough energy for core (inner) excitations Molecules: Electronic, vibrational and rotational energy levels - broad band spectra with many features E = E electronic + E vibrational + E rotational For each electronic state - many vibrational states For each vibrational state - many rotational states many features Absorption spectra affected by (1) number of atoms in molecule (2) solvent molecules more features blurred features CEM 333 page 2.7

Effect of Chemical State (Fig 6-19): CEM 333 page 2.8

Relaxation Processes: Lifetime of excited state is short (fs ms) - relaxational processes return excited species to ground state Nonradiative relaxation many small collisional relaxations tiny temperature rise of surrounding species Radiative relaxation (emission) fluorescence (<10-5 s) and phosphorescence (>10-5 s) Resonance fluorescence produces emission at same energy/frequency/wavelength as absorption common for atoms (no V or R levels) Non-resonance fluorescence produces emission at lower energy (lower frequency/longer wavelength) than absorption (Stokes shift) common in molecules - vibrational relaxation occurs before fluorescence Phosphorescence Produced by long-lived electronic state (up to hours) CEM 333 page 2.9

Absorption Nonradiative relaxation Fluorescence E 2 Vis UV Resonance Non-resonance E 1 IR E 0 Excitation methods: (i) (ii) EM radiation spark/discharge/arc (iii) particle bombardment (electrons, ions... ) (iv) chemiluminescence (exothermic chemical reaction generates excited products) CEM 333 page 2.10