Topic 2 Introduction to Spectroscopy

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    SKA6014

    ADVANCED ANALYTICAL CHEMISTRY

    TOPIC 2Introduction to Spectroscopy

    Azlan Kamari, PhD

    Department of ChemistryFaculty of Science and Mathematics

    Universiti Pendidikan Sultan Idris

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    What is Spectroscopy?

    The study of the interaction between radiation

    and matter

    Analytical spectroscopy, as defined in this

    class, covers applications of spectroscopy tochemical analysis

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    History of Analytical Spectroscopy

    1666: Isaac Newton (England) shows that white light

    can be dispersed into constituent colors, and coins theterm spectrum

    Newton also produced the first spectroscope based

    on lenses, a prism, and a screen

    1800: W. Herschel and J. W. Ritter show that infrared

    (IR) and ultraviolet (UV) light are part of the spectrum

    1814:Joseph Fraunhofer noticed that the suns

    spectrum contains a number of dark lines, developedthe diffraction grating

    1859: G. Kirchoff obtains spectra of the elements,

    explains the suns spectrum

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    The Visible Spectrum of the Sun

    (Black lines are absorption by elements in the cooler outer region of the star)

    Figure from National Optical Astronomy Observatory/Association of Universities for Research in Astronomy/National Science Foundation, http://www.noao.edu/image_gallery/html/im0600.html

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    History of Analytical Spectroscopy

    1870: J. C. Maxwell formalizes and combines

    the laws of electricity and magnetism

    1900 to present: More than 25 Nobel prizes

    awarded to spectroscopists, including:

    1902: H. A. Lorentz and P. Zeeman

    1919: J. Stark

    1933: P. A. M. Dirac and E. Schrodinger

    1945: W. Pauli

    .

    1999: A. Zewail

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    Introduction to Spectroscopy

    Figures from NASA (www.nasa.gov)

    The electromagnetic

    spectrum Each color you see is a

    specific (narrow) range of

    frequencies in this

    spectrum

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    The Electromagnetic Spectrum

    Modern life (not just analytical spectroscopy) revolves

    around the EM spectrum!

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    Properties of Electromagnetic Radiation

    Wave/particle duality

    PerpendicularEand B

    components

    E = electric field

    B = magnetic field

    Wave properties:

    Wavelength (frequency) Amplitude

    Phase1 2 3 4 5

    -1

    -0.5

    0.5

    1

    1 2 3 4 5

    -1

    -0.5

    0.5

    1

    Long wavelength

    (low frequency)

    Short wavelength

    (high frequency)c = the speed of light (~3.00 x 108 m/s)

    = the frequency in cycles/second (Hz)

    = the wavelength in meters/cycle

    c

    Note this figure

    shows polarized

    radiation!

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    Interference of Radiation

    Monochromatic: radiation containing a single frequency

    Polychromatic: radiation containing multiple frequencies

    Constructive interference:

    when two waves reinforce

    each other

    Destructive interference: when

    two waves cancel each other

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    The Interaction of Radiation and Matter

    Electromagnetic radiation travels fastest in a vacuum

    When not travelling in a vacuum, radiation and matter

    can interact in a number of ways

    Some key processes (for spectroscopy):

    Diffraction

    Refraction

    Scattering

    Polarization

    Absorption

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    Transmission of Radiation

    The velocity at which radiation travels (or propagates)

    through a medium is dependent on the medium itself

    When radiation travels through a medium and does not

    undergo a frequency change, it cannot be undergoing a

    permanent energy transfer

    However, radiation can still interact with the medium

    Radiation, an EM field, polarizes the electron clouds of

    atoms in the medium

    Polarization is a temporary deformation of the electron

    clouds

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    Transmission and Refraction

    The refractive index (ni) of a medium is given by:

    i

    icn

    c = the speed of light (~3.00 x 108 m/s)

    i = the velocity of the radiation in the medium in m/sni = the refractive index at the frequency i

    Refractive index measures the degree of interaction

    between the radiation and the medium

    Liquids: ni~ 1.3 to 1.8 Solids: ni~ 1.3 to 2.5

    Refractive index can be used to identify pure liquid

    substances

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    Refraction

    When radiation passes through an interface between two

    media with different refractive indices, it can abruptly

    change direction Snells law:

    1

    2

    2

    1

    2

    1

    sin

    sin

    v

    v

    n

    n

    1 = the velocity of the radiation in medium 1 in m/s

    n1 = the refractive index in medium 1

    Snells law is a consequence

    of the change in velocity in

    the media

    Reflection always occurs at

    an interface. Its extent

    depends on the refractive

    indices of the media

    1

    2

    Medium 1

    Medium 2

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    Diffraction

    Fraunhofer diffraction:

    Also known as far-field diffraction, parallel beamdiffraction

    Important in optical microscopy

    Fresnel diffraction

    Also known as near-field diffraction

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    Diffraction

    Diffraction gratings:

    Widely used in

    spectroscopic instruments

    to separate frequencies(can be made precisely)

    sin2dn

    https://reader009.{domain}/reader009/html5/0420/5ad979fdc2507/5ad97a0797aa6.jpg

    Bragg diffraction multiple slit Fraunhofer diffraction:

    Important for instrument design, crystallography

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    Scattering

    Rayleigh scattering (an elastic process): Scattering of small amounts of radiation by molecules

    and atoms (whose size is near to the wavelength of

    the radiation)

    Mie scattering: applies to large particles, involvesscattering in different directions.

    Practical use in particle size analysis

    4

    1

    scattering

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    Polarization

    Polarization of EM radiation a simple classical picture:

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    Coherent Radiation

    Coherent radiation fulfils two

    conditions: (1) it has the

    same frequency or set offrequencies, and (2) it has a

    well-defined and constant

    phase relationship

    Coherent radiation is cross-correlated in that the

    properties of one beam can be

    used to predict those of the

    other beam

    Examples of coherent

    radiation:

    Lasers

    Microwave sources (masers)

    Coherent radiation: different

    frequencies (colors) with a defined

    phase relationship interfere to produce

    a pulse

    Diagram from wikipedia.org (public domain)

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    Incoherent Radiation

    Produced by random

    emission, e.g. individual

    atoms in a large sampleemitting photons

    Actually is coherent, but just

    to a tiny (undetectable)

    extent Also known as continuous

    radiation

    Examples of incoherent

    radiation: Incandescent light bulbs

    Filament sources

    Deuterium lamps

    Incoherent radiation: differentfrequencies (colors) combined to

    produce continuous radiation with

    varying phase, frequency and

    amplitude

    Diagram from wikipedia.org (public domain)

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    More Properties of Electromagnetic Radiation

    Wave and particle behaviour: photons behave asboth waves and particles

    Quantum mechanics developed around the concept of

    the photon, the elementary unit of radiation

    Plancks law:

    Eis the energy of the photon in joules

    h is Planck's constant (6.624 x 10-34 joule seconds)

    is the frequency of the radiation

    hE

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    Absorption and Emission

    Absorption is a process accompanied by an energy

    change involves energy transfer of EM radiation to a

    substance, usually at specific frequencies

    corresponding to natural atomic or molecular energies

    Emission occurs when matter releases energy in the form

    of radiation (photons)

    E= h

    Higher energy

    Lower energy

    Absorption Emission

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    Energy Levels

    Several types of quantum-mechanical energy

    levels occur in nature: Electronic

    Rotational

    Vibrational (including phonons and heat)

    Nuclear

    For each of these, a discrete quantum state and

    energy-driven transitions between these states can be

    studied (as opposed to a continuous range of energies)

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    The Uncertainty of Measurements

    Because the lifetimes of quantum states canpersist for short periods, it can be difficult to

    measure their energies accurately

    This is usually stated in the form of an energy-

    time uncertainty:

    tE

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    The Uncertainty Principle

    The uncertainty principle: it is not possible to know both

    the location and the momentum of a particle exactly afundamental limit on all measurements

    In Heisenbergs terms, the act of measuring a particles

    position affects its momentum, andvice versa

    In equation form:

    In other words, if you know the position of a particle to within x,

    then you can specify its momentum alongxto px

    As the uncertainty inxincreases (x), that ofpxdecreases (x

    ), and vice versa

    px x 21

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    Spectra and Spectrometers

    Spectra are usually plotted as frequency vs. amplitude

    Instead of energy, wavelength or energy (related

    properties) can also be used

    The choice of x- and y-axes is often dependent on the

    particular technique, its history, etc

    Key parameter is frequency/energy/wavelength

    resolution

    Spectrometers:

    instruments that measure the interaction

    of radiation with matter, so the properties of such

    interactions can be studied

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    Spectroscopy in Analytical Chemistry

    Widely used approach for characterizing systems ranging

    from chemical physics to biology, from individual atoms tothe largest molecules

    Some of the most common techniques are:

    UV-Visible spectroscopy

    IR spectroscopy

    Raman spectroscopy

    X-ray spectroscopy NMR spectroscopy

    EPR spectroscopy