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INTRODUCTION TO
SPECTROSCOPIC METHODS OF
ANALYSIS
LECTURE 11
WHAT IS SPECTROSCOPY?
The study of the interaction between
ELECTROMAGNETIC (EM) RADIATION and
MATTER
2
SPECTROSCOPIC ANALYSIS
covers
ATOMIC
SPECTROSCOPY
MOLECULAR
SPECTROSCOPY
3
TO UNDERSTAND SPECTROSCOPY WE
MUST UNDERSTAND ELECTROMAGNETIC
RADIATION
What is Electromagnetic Radiation?
 is a form of energy that has both Wave and Particle
Properties.
 For example: Ultraviolet, visible, infrared,
microwave, radio wave.
4
WAVE PROPERTIES
 EM radiation is conveniently modeled as waves
consisting of perpendicularly oscillating electric and
magnetic fields, as shown below.
x
y
z Electric Field
Magnetic Field
Direction of
propagation
5
o At 90° to the direction of propagation is an oscillation in
the ELECTRIC FIELD.
o At 90° to the direction of propagation and 90° from the
electric field oscillation (orthagonal) is the MAGNETIC
FIELD oscillation.
6
WAVE PARAMETERS
We Use Symbols to Designate the Various
Properties of Waves
  is the wavelength of the waves
 V is the frequency of the waves
 c is the speed of light
Time or Distance-
+
ElectricField
0
Amplitude (A)
Wavelength ()
7
DEFINITIONS:
 Period (p) – the time required for one cycle to pass a fixed point in
space.
 Frequency (V) – the number of cycles which pass a fixed point in
space per second.
 Amplitude (A) – The maximum length of the electric vector in the
wave (Maximum height of a wave).
 Wavelength () – The distance between two identical adjacent points
in a wave (usually maxima or minima).
 Wavenumber () - The number of waves per cm in units of cm-1. 8
 Radiant Power ( P ) - The amount of energy reaching a given area
per second. Unit in watts (W)
 Intensity ( I ) - The radiant power per unit solid angle.
9
DEFINITIONS:
RELATIONSHIP BETWEEN THESE VARIABLES
Speed of light = Wavelength x Frequency
 c = V
  = c/V
 V = c/
For Electromagnetic Waves the Speed (c) is a Constant
c = 3.00 x 108 m/sec = 3.00 x 1010 cm/sec
10
 This Constant Speed Means a Direct, Inverse
Relationship Between Wavelength and Frequency
 ∝ 1/V
 The Higher the Frequency the Shorter the
Wavelength . The Longer the Wavelength the Lower
the Frequency.
11
THE RELATIONSHIP BETWEEN
FREQUENCY AND WAVELENGTH
Wavelength is inversely proportional to frequency
12
800 nm
Infrared radiation
V = 3.75 x 1014 s-1
Ultraviolet radiation
V = 7.50 x 1014 s-1
PARTICLE PROPERTIES OF LIGHT: PHOTONS
• Wave theory failed to explain phenomena associated with the
absorption and emission of radiation of radiant energy.
• Thus, EM is viewed as a stream of discrete particles, or wave
packets, of energy called photons.
• We can relate the energy of photon to its wavelength,
frequency and wavenumber by
E = hV V - frequency
= h c  - wavelength
 υ - wavenumber
= hcυ
 h – Planck’s constant =6.63x10-34 J·s 13
THE ELECTROMAGNETIC SPECTRUM
14
REGIONS OF THE UV, VISIBLE AND IR SPECTRUM
Region Wavelength Range
UV 180 – 380 nm
Visible 380 – 780 nm
Near-IR 0.78 – 2.5 μm
Mid-IR 2.5 – 50 μm
15
PREFIXES FOR UNITS
Prefix Symbols Multiplier
giga- G 109
mega- M 106
kilo- k 103
deci- d 10-1
centi- c 10-2
milli- m 10-3
micro- µ 10-6
nano- n 10-9
pico- p 10-12
femto- f 10-15
atto- a 10-18 16
WAVELENGTH UNITS FOR VARIOUS SPECTRAL REGION
Region Unit Definition (m)
X-ray Angstrom unit, Å 10-10 m
Ultraviolet/visible Nanometer, nm 10-9 m
Infrared Micrometer, μm 10-6 m
17
INTERACTION OF ELECTROMAGNETIC RADIATION
WITH MATTER
Infrared primarily acts to set molecules into vibration.
UV and visible light primarily acts to elevate electrons to higher energy levels.
18
INTERACTION OF ELECTROMAGNETIC
RADIATION WITH MATTER
 The interaction of radiation with matter can cause redirection
of the radiation and/or transitions between the energy levels
of the atoms or molecules.
1. A transition from a lower level to a higher level with transfer
of energy from the radiation field to the atom or molecule is
called absorption.
2. A transition from a higher level to a lower level is called
emission if energy is transferred to the radiation field, or
nonradiative decay if no radiation is emitted.
3. Redirection of light due to its interaction with matter is called
scattering, and may or may not occur with transfer of energy,
i.e., the scattered radiation has a slightly different or the same
wavelength.
19
TYPES OF SPECTRA
1. Absorption spectrum
2.Emission spectrum
 Absorption spectrum
 A plot of the absorbance as a function of wavelength or
frequency.
 Emission spectrum
 A plot of the relative power of the emitted radiation as a
function of wavelength or frequency.
20
ATOMIC vs MOLECULAR TRANSITIONS
21
ATOMIC TRANSITION
 Atomic transitions are usually very discreet changes
of electrons from one quantum state to another
(energy levels, shells, spins, etc.).
 Only electronic transition is quantized.
 When an atom changes energy state, it absorbs or
emits energy equal to the energy difference
E = E1 – E0
 The wavelength or frequency of radiation absorbed
or emitted during a transition proportional to E
 Transitions between electronic levels produce line
spectra. 22
ATOMIC TRANSITION
 E0 – lowest energy electronic level or ground state
 E1, E2 – higher-energy electronic levels 23
MOLECULAR TRANSITION
 In molecules the electronic states are subdivided
into vibrational states.
 The energy of a band in a molecular absorption
spectrum is the sum of three different energy
components.
E = Eelectronic + Evibrational + Erotational
 Transitions between electronic-vibrational-rotational
states give rise to spectra that appear to have
bands. 24
25
Vibrational
energy level
MOLECULAR TRANSITION
Energy
ATOMIC ABSORPTION SPECTRUM
 The two peaks arise from the promotion of a 3s electron to the
two 3p states
26
Absorption Spectrum of Na
MOLECULAR ABSORPTION SPECTRA
 The sharpness of molecular
absorption spectra also depends on
the state of the sample.
 Figure (b) shows an absorption
band due to transitions between
electronic-vibrational-rotational
states
 Figure (d) shows a continuous
spectra due to the sample is in the
condensed state. In condensed
states the spectra broaden due to
molecular collisions.
27
EMISSION SPECTRUM
 Three types of
spectra:
 Lines
 Bands
 Continuum
spectra
28
Emission spectrum of a brine sample
COMPONENTS OF INSTRUMENTS FOR
OPTICAL SPECTROSCOPY
29
GENERAL DESIGN OF OPTICAL INSTRUMENTS
Absorption
Emission
30
FIVE BASIC OPTICAL INSTRUMENT COMPONENTS
1)Source - A stable source of radiant energy at the desired wavelength (or  range).
2)Sample Holder - A transparent container used to hold the sample (cells,
cuvettes, etc.).
3)Wavelength Selector - A device that isolates a restricted region of the EM
spectrum used for measurement (monochromators, prisms, & filters).
4)Photoelectric Transducer - (Detector) Converts the radiant energy into a
useable signal (usually electrical).
5)Signal Processor & Readout - Amplifies or attenuates the transduced signal
and sends it to a readout device such as a meter, digital readout, chart recorder,
computer, etc.
31
I. SOURCES OF RADIATION
• Generate a beam of radiation that is stable and has sufficient
power.
A. Continuum Sources
- emit radiation over a broad wavelength range and the intensity
of the radiation changes slowly as a function of wavelength.
This type of source is commonly used in UV, visible and IR
instruments.
• Deuterium lamp is the most common UV source.
• Tungsten lamp is the most common visible source.
• Glowing inert solids are common sources for IR instruments. 32
B. Line Sources
- Emit a limited number lines or bands of radiation at specific
wavelengths.
• Used in atomic absorption spectroscopy
• Types of line sources:
1) Hollow cathode lamps
2) Electrodeless discharge lamps
3) Lasers - Light amplification by stimulated emission of
radiation
33
II. WAVELENGTH SELECTORS
• Wavelength selectors output a limited, narrow,
continuous group of wavelengths called a band.
• Two types of wavelength selectors:
A)Filters
B)Monochromators
34
A. FILTERS
• Two types of filters:
1) Interference filters
2) Absorption Filters
B. Monochromators
• Wavelength selector that can continuously scan a broad range of
wavelengths
• Used in most scanning spectrometers including UV, visible, and IR
instruments.
35
III. RADIATION TRANSDUCERS (DETECTORS)
• Early detectors in spectroscopic instruments were the human eye,
photographic plates or films. Modern instruments contain devices that
convert the radiation to an electrical signal.
Two general types of radiation transducers:
a. Photon detectors
b. Thermal detectors
36
• Several types of photon detectors are available:
1. Vacuum phototubes
2. Photomultiplier tubes
3. Photovoltaic cells
4. Silicon photodiodes
5. Diode array transducers
6. Photoconductivity transducers
A. Photon Detectors
• Commonly useful in ultraviolet, visible, and near infrared instruments.
37
• Three types of thermal detectors :
1. Thermocouples
2. Bolometers
3. Pyroelectric transducers
B. Thermal Detectors
• Used for infrared spectroscopy because photons in the IR region lack
the energy to cause photoemission of electrons.
38
 Sample containers, usually called cells or cuvettes must have
windows that are transparent in the spectral region of interest.
 There are few types of cuvettes:
- quartz or fused silica
- silicate glass
- crystalline sodium chloride
QUARTZ OR FUSED SILICA
- REQUIRED FOR UV AND MAY BE USED IN VISIBLE REGION
SILICATE GLASS
- CHEAPER COMPARED TO QUARTZ. USED IN UV
CRYSTALLINE SODIUM CHLORIDE
- USED IN IR
IV.SAMPLE HOLDER (CONTAINER)
cuvette
39
 SPECTROMETER
- is an instrument that provides information about the intensity of
radiation as a function of wavelength or frequency
 SPECTROPHOTOMETER
- is a spectrometer equipped with one or more exit slits and
photoelectric transducers that permits the determination of the
ratio of the radiant power of two beams as a function of
wavelength as in absorption spectroscopy.
40
REGION SOURCE SAMPLE
HOLDER
DETECTOR
Ultraviolet Deuterium lamp Quartz/fused
silica
Phototube, PM
tube, diode array
Visible Tungsten lamp Glass/quartz Phototube, PM
tube, diode array
Infrared Nernst glower (rare earth
oxides or silicon carbide
glowers)
Salt crystals e.g.
crystalline
sodium chloride
Thermocouples,
bolometers
Types of source, sample holder and detector for various
EM region
SUMMARY
41

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Introduction of spectroscopy

  • 1. INTRODUCTION TO SPECTROSCOPIC METHODS OF ANALYSIS LECTURE 11
  • 2. WHAT IS SPECTROSCOPY? The study of the interaction between ELECTROMAGNETIC (EM) RADIATION and MATTER 2
  • 4. TO UNDERSTAND SPECTROSCOPY WE MUST UNDERSTAND ELECTROMAGNETIC RADIATION What is Electromagnetic Radiation?  is a form of energy that has both Wave and Particle Properties.  For example: Ultraviolet, visible, infrared, microwave, radio wave. 4
  • 5. WAVE PROPERTIES  EM radiation is conveniently modeled as waves consisting of perpendicularly oscillating electric and magnetic fields, as shown below. x y z Electric Field Magnetic Field Direction of propagation 5
  • 6. o At 90° to the direction of propagation is an oscillation in the ELECTRIC FIELD. o At 90° to the direction of propagation and 90° from the electric field oscillation (orthagonal) is the MAGNETIC FIELD oscillation. 6
  • 7. WAVE PARAMETERS We Use Symbols to Designate the Various Properties of Waves   is the wavelength of the waves  V is the frequency of the waves  c is the speed of light Time or Distance- + ElectricField 0 Amplitude (A) Wavelength () 7
  • 8. DEFINITIONS:  Period (p) – the time required for one cycle to pass a fixed point in space.  Frequency (V) – the number of cycles which pass a fixed point in space per second.  Amplitude (A) – The maximum length of the electric vector in the wave (Maximum height of a wave).  Wavelength () – The distance between two identical adjacent points in a wave (usually maxima or minima).  Wavenumber () - The number of waves per cm in units of cm-1. 8
  • 9.  Radiant Power ( P ) - The amount of energy reaching a given area per second. Unit in watts (W)  Intensity ( I ) - The radiant power per unit solid angle. 9 DEFINITIONS:
  • 10. RELATIONSHIP BETWEEN THESE VARIABLES Speed of light = Wavelength x Frequency  c = V   = c/V  V = c/ For Electromagnetic Waves the Speed (c) is a Constant c = 3.00 x 108 m/sec = 3.00 x 1010 cm/sec 10
  • 11.  This Constant Speed Means a Direct, Inverse Relationship Between Wavelength and Frequency  ∝ 1/V  The Higher the Frequency the Shorter the Wavelength . The Longer the Wavelength the Lower the Frequency. 11
  • 12. THE RELATIONSHIP BETWEEN FREQUENCY AND WAVELENGTH Wavelength is inversely proportional to frequency 12 800 nm Infrared radiation V = 3.75 x 1014 s-1 Ultraviolet radiation V = 7.50 x 1014 s-1
  • 13. PARTICLE PROPERTIES OF LIGHT: PHOTONS • Wave theory failed to explain phenomena associated with the absorption and emission of radiation of radiant energy. • Thus, EM is viewed as a stream of discrete particles, or wave packets, of energy called photons. • We can relate the energy of photon to its wavelength, frequency and wavenumber by E = hV V - frequency = h c  - wavelength  υ - wavenumber = hcυ  h – Planck’s constant =6.63x10-34 J·s 13
  • 15. REGIONS OF THE UV, VISIBLE AND IR SPECTRUM Region Wavelength Range UV 180 – 380 nm Visible 380 – 780 nm Near-IR 0.78 – 2.5 μm Mid-IR 2.5 – 50 μm 15
  • 16. PREFIXES FOR UNITS Prefix Symbols Multiplier giga- G 109 mega- M 106 kilo- k 103 deci- d 10-1 centi- c 10-2 milli- m 10-3 micro- µ 10-6 nano- n 10-9 pico- p 10-12 femto- f 10-15 atto- a 10-18 16
  • 17. WAVELENGTH UNITS FOR VARIOUS SPECTRAL REGION Region Unit Definition (m) X-ray Angstrom unit, Å 10-10 m Ultraviolet/visible Nanometer, nm 10-9 m Infrared Micrometer, μm 10-6 m 17
  • 18. INTERACTION OF ELECTROMAGNETIC RADIATION WITH MATTER Infrared primarily acts to set molecules into vibration. UV and visible light primarily acts to elevate electrons to higher energy levels. 18
  • 19. INTERACTION OF ELECTROMAGNETIC RADIATION WITH MATTER  The interaction of radiation with matter can cause redirection of the radiation and/or transitions between the energy levels of the atoms or molecules. 1. A transition from a lower level to a higher level with transfer of energy from the radiation field to the atom or molecule is called absorption. 2. A transition from a higher level to a lower level is called emission if energy is transferred to the radiation field, or nonradiative decay if no radiation is emitted. 3. Redirection of light due to its interaction with matter is called scattering, and may or may not occur with transfer of energy, i.e., the scattered radiation has a slightly different or the same wavelength. 19
  • 20. TYPES OF SPECTRA 1. Absorption spectrum 2.Emission spectrum  Absorption spectrum  A plot of the absorbance as a function of wavelength or frequency.  Emission spectrum  A plot of the relative power of the emitted radiation as a function of wavelength or frequency. 20
  • 21. ATOMIC vs MOLECULAR TRANSITIONS 21
  • 22. ATOMIC TRANSITION  Atomic transitions are usually very discreet changes of electrons from one quantum state to another (energy levels, shells, spins, etc.).  Only electronic transition is quantized.  When an atom changes energy state, it absorbs or emits energy equal to the energy difference E = E1 – E0  The wavelength or frequency of radiation absorbed or emitted during a transition proportional to E  Transitions between electronic levels produce line spectra. 22
  • 23. ATOMIC TRANSITION  E0 – lowest energy electronic level or ground state  E1, E2 – higher-energy electronic levels 23
  • 24. MOLECULAR TRANSITION  In molecules the electronic states are subdivided into vibrational states.  The energy of a band in a molecular absorption spectrum is the sum of three different energy components. E = Eelectronic + Evibrational + Erotational  Transitions between electronic-vibrational-rotational states give rise to spectra that appear to have bands. 24
  • 26. ATOMIC ABSORPTION SPECTRUM  The two peaks arise from the promotion of a 3s electron to the two 3p states 26 Absorption Spectrum of Na
  • 27. MOLECULAR ABSORPTION SPECTRA  The sharpness of molecular absorption spectra also depends on the state of the sample.  Figure (b) shows an absorption band due to transitions between electronic-vibrational-rotational states  Figure (d) shows a continuous spectra due to the sample is in the condensed state. In condensed states the spectra broaden due to molecular collisions. 27
  • 28. EMISSION SPECTRUM  Three types of spectra:  Lines  Bands  Continuum spectra 28 Emission spectrum of a brine sample
  • 29. COMPONENTS OF INSTRUMENTS FOR OPTICAL SPECTROSCOPY 29
  • 30. GENERAL DESIGN OF OPTICAL INSTRUMENTS Absorption Emission 30
  • 31. FIVE BASIC OPTICAL INSTRUMENT COMPONENTS 1)Source - A stable source of radiant energy at the desired wavelength (or  range). 2)Sample Holder - A transparent container used to hold the sample (cells, cuvettes, etc.). 3)Wavelength Selector - A device that isolates a restricted region of the EM spectrum used for measurement (monochromators, prisms, & filters). 4)Photoelectric Transducer - (Detector) Converts the radiant energy into a useable signal (usually electrical). 5)Signal Processor & Readout - Amplifies or attenuates the transduced signal and sends it to a readout device such as a meter, digital readout, chart recorder, computer, etc. 31
  • 32. I. SOURCES OF RADIATION • Generate a beam of radiation that is stable and has sufficient power. A. Continuum Sources - emit radiation over a broad wavelength range and the intensity of the radiation changes slowly as a function of wavelength. This type of source is commonly used in UV, visible and IR instruments. • Deuterium lamp is the most common UV source. • Tungsten lamp is the most common visible source. • Glowing inert solids are common sources for IR instruments. 32
  • 33. B. Line Sources - Emit a limited number lines or bands of radiation at specific wavelengths. • Used in atomic absorption spectroscopy • Types of line sources: 1) Hollow cathode lamps 2) Electrodeless discharge lamps 3) Lasers - Light amplification by stimulated emission of radiation 33
  • 34. II. WAVELENGTH SELECTORS • Wavelength selectors output a limited, narrow, continuous group of wavelengths called a band. • Two types of wavelength selectors: A)Filters B)Monochromators 34
  • 35. A. FILTERS • Two types of filters: 1) Interference filters 2) Absorption Filters B. Monochromators • Wavelength selector that can continuously scan a broad range of wavelengths • Used in most scanning spectrometers including UV, visible, and IR instruments. 35
  • 36. III. RADIATION TRANSDUCERS (DETECTORS) • Early detectors in spectroscopic instruments were the human eye, photographic plates or films. Modern instruments contain devices that convert the radiation to an electrical signal. Two general types of radiation transducers: a. Photon detectors b. Thermal detectors 36
  • 37. • Several types of photon detectors are available: 1. Vacuum phototubes 2. Photomultiplier tubes 3. Photovoltaic cells 4. Silicon photodiodes 5. Diode array transducers 6. Photoconductivity transducers A. Photon Detectors • Commonly useful in ultraviolet, visible, and near infrared instruments. 37
  • 38. • Three types of thermal detectors : 1. Thermocouples 2. Bolometers 3. Pyroelectric transducers B. Thermal Detectors • Used for infrared spectroscopy because photons in the IR region lack the energy to cause photoemission of electrons. 38
  • 39.  Sample containers, usually called cells or cuvettes must have windows that are transparent in the spectral region of interest.  There are few types of cuvettes: - quartz or fused silica - silicate glass - crystalline sodium chloride QUARTZ OR FUSED SILICA - REQUIRED FOR UV AND MAY BE USED IN VISIBLE REGION SILICATE GLASS - CHEAPER COMPARED TO QUARTZ. USED IN UV CRYSTALLINE SODIUM CHLORIDE - USED IN IR IV.SAMPLE HOLDER (CONTAINER) cuvette 39
  • 40.  SPECTROMETER - is an instrument that provides information about the intensity of radiation as a function of wavelength or frequency  SPECTROPHOTOMETER - is a spectrometer equipped with one or more exit slits and photoelectric transducers that permits the determination of the ratio of the radiant power of two beams as a function of wavelength as in absorption spectroscopy. 40
  • 41. REGION SOURCE SAMPLE HOLDER DETECTOR Ultraviolet Deuterium lamp Quartz/fused silica Phototube, PM tube, diode array Visible Tungsten lamp Glass/quartz Phototube, PM tube, diode array Infrared Nernst glower (rare earth oxides or silicon carbide glowers) Salt crystals e.g. crystalline sodium chloride Thermocouples, bolometers Types of source, sample holder and detector for various EM region SUMMARY 41