UVVIS SPECTROSCOPY PPT

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    SPECTROSCOPY

    Light interacting with matter as an

    analytical tool

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    X-ray:

    core electronexcitation

    UV:

    valanceelectronic

    excitation

    IR:

    molecularvibrations

    Radio waves:

    Nuclear spin states(in a magnetic field)

    Electronic Excitation by UV/Vis Spectroscopy :

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    Spectroscopic Techniques andChemistry they Probe

    UV-vis UV-vis region bonding electrons

    Atomic Absorption UV-vis region atomic transitions (val. e-)

    FT-IR IR/Microwave vibrations, rotations

    Raman IR/UV vibrations

    FT-NMR Radio waves nuclear spin states

    X-Ray Spectroscopy X-rays inner electrons, elemental

    X-ray Crystallography X-rays 3-D structure

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    Spectroscopic Techniques and Common Uses

    UV-vis UV-vis regionQuantitative

    analysis/Beers Law

    Atomic Absorption UV-vis regionQuantitative analysis

    Beers Law

    FT-IR IR/Microwave Functional Group Analysis

    Raman IR/UVFunctional Group

    Analysis/quant

    FT-NMR Radio waves Structure determination

    X-Ray Spectroscopy X-rays Elemental Analysis

    X-ray Crystallography X-rays 3-D structure Anaylysis

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    Different Spectroscopies

    UV-vis electronic states of valence e/d-orbital transitions for solvated transitionmetals

    Fluorescence emission of UV/vis by certainmolecules

    FT-IR vibrational transitions of molecules

    FT-NMR nuclear spin transitions X-Ray Spectroscopy electronic transitions

    of core electrons

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    Quantitative Spectroscopy

    Beers Law

    Al1 = el1bc

    e is molar absorptivity (unique for a

    given compound at l1)

    b is path length

    c concentration

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    Beers Law

    A = -logT = log(P0/P) = ebc

    T = Psolution/Psolvent = P/P0

    Works for monochromatic light

    Compound x has a unique e at different

    wavelengths

    cuvette

    source slit

    detector

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    Characteristics of

    Beers Law Plots One wavelength

    Good plots have a range of

    absorbances from 0.010 to 1.000

    Absorbances over 1.000 are not that

    valid and should be avoided

    2 orders of magnitude

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    Standard Practice

    Prepare standards of knownconcentration

    Measure absorbance at lmax Plot A vs. concentration

    Obtain slope

    Use slope (and intercept) to determinethe concentration of the analyte in theunknown

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    Typical Beers Law Plot

    y = 0.02x

    0

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    0.0 20.0 40.0 60.0

    concentration (uM)

    A

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    UV-Vis Spectroscopy

    UV- organic molecules

    Outer electron bonding transitions

    conjugation

    Visible metal/ligands in solution

    d-orbital transitions

    Instrumentation

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    Characteristics of UV-Vis spectra of

    Organic Molecules Absorb mostly in UV unless highly

    conjugated

    Spectra are broad, usually to broad forqualitative identification purposes

    Excellent for quantitative Beers Law-

    type analyses The most common detector for anHPLC

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    Molecules have quantized energy levels:

    ex. electronic energy levels.

    energy

    hv

    energy

    }= hv

    Q: Where do these quantized energy levels come from?

    A: The electronic configurations associated with bonding.

    Each electronic energy level(configuration) has

    associated with it the many

    vibrational energy levels we

    examined with IR.

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    Broad spectra

    Overlapping vibrational and rotational

    peaks Solvent effects

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    Molecular Orbital Theory

    Fig 18-10

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    2s 2s

    s

    s*

    s

    s*

    p*

    p

    2p 2pn

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    C C

    s

    s*

    hv

    s

    s*

    s s*

    C C

    H

    H

    HH

    HH

    lmax

    = 135 nm (a high energy transition)

    Absorptions havinglmax < 200 nm are difficult to observe because

    everything (including quartz glass and air) absorbs in this spectral

    region.

    Ethane

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    C C

    s

    s*

    hv

    p

    p*

    s

    s*

    p

    p*

    p p*

    Example: ethylene absorbs at longer wavelengths: lmax = 165 nm = 10,000

    = hv=hc/l

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    s

    s*

    hv

    p

    p*

    n

    s

    s*

    p

    p*

    n

    C O

    p*n

    The n to pi* transition is at even lower wavelengths but is notas strong as pi to pi* transitions. It is said to be forbidden.

    Example:

    Acetone: ns*lmax = 188 nm ; = 1860

    np* lmax = 279 nm ; = 15

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    C C

    C C

    C O

    C O

    H

    ss* 135 nm

    pp* 165 nm

    ns* 183 nm weak

    pp* 150 nm

    ns* 188 nmnp* 279 nm weak

    l

    A

    180 nm

    279 nm

    C O

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    C C

    HOMO

    LUMO

    Conjugated systems:

    Preferred transition is between Highest Occupied Molecular Orbital(HOMO) and Lowest Unoccupied Molecular Orbital (LUMO).

    Note: Additional conjugation (double bonds) lowers the HOMO-

    LUMO energy gap:

    Example:

    1,3 butadiene: lmax = 217 nm ; = 21,000

    1,3,5-hexatriene lmax = 258 nm ; = 35,000

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    O

    O

    O

    Similar structures have similar UV spectra:

    lmax = 238, 305 nmlmax = 240, 311 nm lmax = 173, 192 nm

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    Lycopene:

    lmax = 114 + 5(8) + 11*(48.0-1.7*11) = 476 nm

    lmax(Actual) = 474.

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    Metal ion transitions

    Degenerate

    D-orbitals

    of naked Co

    D-orbitalsof hydrated Co2+

    Octahedral Configuration

    E

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    Co2+

    H2O

    H2O

    H2O

    H2O

    H2O

    H2

    O

    Octahedral Geometry

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    Instrumentation

    Fixed wavelength instruments

    Scanning instruments

    Diode Array Instruments

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    Fixed Wavelength Instrument

    LED serve as source

    Pseudo-monochromatic light source

    No monochrometer necessary/ wavelength selection

    occurs by turning on the appropriate LED 4 LEDs to choose from

    photodyode

    sample

    beam of light

    LEDs

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    Scanning Instrument

    cuvette

    Tungsten

    Filament (vis)

    slit

    Photomultiplier

    tube

    monochromator

    Deuterium lamp

    Filament (UV)

    slit

    Scanning Instrument

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    sources

    Tungten lamp (350-2500 nm)

    Deuterium (200-400 nm)

    Xenon Arc lamps (200-1000 nm)

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    Monochromator

    Braggs law, nl = d(sin i + sin r)

    Angular dispersion, dr/dl = n / d(cos r)

    Resolution, R = l/l=nN, resolution is

    extended by concave mirrors to refocus

    the divergent beam at the exit slit

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    Sample holder

    Visible; can be plastic or glass

    UV; you must use quartz

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    Single beam vs. double beam

    Source flicker

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    Diode array Instrument

    cuvette

    Tungsten

    Filament (vis)

    slit

    Diode array detector

    328 individual detectors

    monochromator

    Deuterium lampFilament (UV)

    slit

    mirror

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    Advantages/disadvantages

    Scanning instrument High spectral resolution (63000),l/l

    Long data acquisition time (severalminutes)

    Low throughput

    Diode array

    Fast acquisition time (a couple of

    seconds), compatible with on-lineseparations

    High throughput (no slits)

    Low resolution (2 nm)

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    HPLC-UV

    Mobile

    phase

    HPLC

    Pump

    syringe

    6-port

    valveSample

    loop

    HPLC

    column

    UV

    detector

    Solvent

    waste