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Introduction to Spectroscopic methodsIntroduction to Spectroscopic methods
Spectroscopy:Spectroscopy:
Study of interaction between Study of interaction between radiation (or other radiation (or other forms of energy)forms of energy) and and matter matter (a branch of (a branch of science). science).
Spectrometry:Spectrometry:
Analytical methodsAnalytical methods based on atomic and based on atomic and molecular spectroscopymolecular spectroscopy
2
Types of Analytical Types of Analytical SpectroscopySpectroscopy
AbsorptionAbsorption Fluoresence and PhosphoresenceFluoresence and Phosphoresence Emission (atomic with flames, Emission (atomic with flames,
arcs, sparks, and palsmas)arcs, sparks, and palsmas) Chemilumenesence and Chemilumenesence and
BiolumenesenceBiolumenesence ReflectionReflection
The Electromagnetic The Electromagnetic SpectrumSpectrum
= c / E = h
4
What about E?What about E?
= c / E = h
5
Kinds of Kinds of SpectroscopySpectroscopy
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
6
LIGHTLIGHT
Electro-Electro-magnetic magnetic radiationradiation
7
Light as a WaveLight as a Wave
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
8
Light as a WaveLight as a Wave
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
9
Light as a WaveLight as a Wave
Frequency = Frequency = Velocity of propagation = Velocity of propagation = vv = = Speed of light in a vacuum = c = 3.00 x 10Speed of light in a vacuum = c = 3.00 x 1088 m/s m/sWavenumber (reciprocal of Wavenumber (reciprocal of ) = ) = = = kk = = //vv
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
10
Effect of the Medium on a Light WaveEffect of the Medium on a Light Wave
• Frequency remains the same.Frequency remains the same.
• Velocity and Wavelength change.Velocity and Wavelength change.
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
11
Mathematic Description of a WaveMathematic Description of a Wave
Y = A sin(Y = A sin(t + t + ))
A = Amplitude A = Amplitude
= angular frequency = 2= angular frequency = 2 = =v2v2
= phase angle= phase angle
Y = A sin(2Y = A sin(2t + t + ))
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
12
Mathematic Description of a WaveMathematic Description of a Wave
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
Sine waves with different amplitudes and with a phase different of 90 degree
13
If two plane-polarized waves overlap in space, the If two plane-polarized waves overlap in space, the resulting electromagnetic disturbance is the resulting electromagnetic disturbance is the algebraic algebraic sum of the two waves.sum of the two waves.
CoherenceCoherence: : When two waves have an initial phase When two waves have an initial phase difference of zero or it is constant for a long time they difference of zero or it is constant for a long time they are considered coherent.are considered coherent.
Superposition of WavesSuperposition of Waves
Y = AY = A11sin(2sin(211t + t + ) + ) + AA22sin(2sin(222t + t + ) +…….) +…….
Optical Optical Interference:Interference: The interaction of two or more The interaction of two or more light waves yielding an irradiance that is not equal to light waves yielding an irradiance that is not equal to the sum of the irradiances.the sum of the irradiances.
14
Optical InterferenceOptical Interference
Constructive InterferenceConstructive Interference1) Have identical frequency1) Have identical frequency
2)2)22 – – 11 = = = = m2m2
Destructive InterferenceDestructive Interference1) Have identical frequency1) Have identical frequency
2)2)22 – – 11 = = = (2m+1) = (2m+1)
Figure 3-4 – Ingle and Crouch, Figure 3-4 – Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
22 – – 11 = 180 deg or integer = 180 deg or integer
of multiple of 360 deg. of multiple of 360 deg.
22 – – 11 = 0, or 360 deg or = 0, or 360 deg or
integer of multiple of 360 deg. integer of multiple of 360 deg.
15
Superposition of sinusoidal wave: (a) A1 < A2, (1 - 2) = 20º, 1 = 2;(b) A1 < A2, (1 - 2) = 200º, 1 = 2
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
16Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
Superposition of tw sinusoidal wave of different frequencies but identical amplitudes.
Should be
17
Diffraction: The Bending of Light as It Diffraction: The Bending of Light as It Passes Through an Aperture or Around Passes Through an Aperture or Around
a Small Objecta Small Object
Fraunhofer Fraunhofer DiffractionDiffractionNarrow SlitNarrow SlitDiffractionDiffraction
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
Diffraction is a consequence of interference
18Eugene Hecht, Eugene Hecht, OpticsOptics, Addison-Wesley, Reading, MA, 1998., Addison-Wesley, Reading, MA, 1998.
Diffraction increases as Diffraction increases as aperture size aperture size
Diffraction of Waves in a LiquidDiffraction of Waves in a Liquid
19
Diffraction Pattern From Diffraction Pattern From Multiple SlitsMultiple Slits
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
20
Diffraction Pattern From Diffraction Pattern From Multiple SlitsMultiple Slits
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
21
Diffraction Pattern From Diffraction Pattern From Multiple SlitsMultiple Slits
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
CF = BC sin = nn is an integer called order of interference
22
Coherent RadiationCoherent Radiation
Conditions for coherent of
two sources of radiation are:
1.Identical frequencies and wavelength
2.Phase relationship remains constant with time
23
Eugene Hecht, Eugene Hecht, OpticsOptics, Addison-Wesley, , Addison-Wesley, Reading, MA, 1998.Reading, MA, 1998.
Conservation LawConservation Law
TT = 1 = 1
= Fraction Absorbed= Fraction Absorbed
= Fraction Reflected= Fraction Reflected
TT = Fraction = Fraction TransmittedTransmitted
What happens when light What happens when light hits a boundary between hits a boundary between two media?two media?
RefractionRefraction: : change in direction change in direction of radiation as it passes from of radiation as it passes from one medium to another with one medium to another with different densitydifferent density
Physics of RefractionPhysics of Refraction
24
Refractive index (Refractive index (nn))
the velocity (v) of EM radiation the velocity (v) of EM radiation depends on the medium depends on the medium through which it travelsthrough which it travels
nnii = c/v = c/vii (>1). (>1). the ratio of the velocity in vacuum the ratio of the velocity in vacuum
over the velocity in the medium over the velocity in the medium nn depends on the frequency of depends on the frequency of
the lightthe light
25
RefractionRefraction
nn11sinsin11 = = nn22sinsin22
Snell’s LawSnell’s Law
vv22sinsin1 = v1 = v11sinsin22
Douglas A. Skoog, Douglas A. Skoog, et al.et al. Principles of Instrumental Analysis, Principles of Instrumental Analysis, ThomsonThomson, , 20072007
26
RefractionRefraction
27
Transmission: The Refractive IndexTransmission: The Refractive Index
Eugene Hecht, Eugene Hecht, OpticsOptics, Addison-Wesley, Reading, MA, 1998., Addison-Wesley, Reading, MA, 1998.
vn
c v
nc
n is wavelength (frequency) n is wavelength (frequency) dependent.dependent.
In glass n increases as In glass n increases as decreases.decreases.
28
Dispersion and PrismsDispersion and Prisms
iv
c iv
c
DispersionThe variation in refractive index of a substance with wavelength or frequency
29
Dispersion and PrismsDispersion and Prisms
Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007Douglas A. Skoog, et al. Principles of Instrumental Analysis, Thomson, 2007
30
A ray of single-wavelength incident on a prismA ray of single-wavelength incident on a prism
12 3
: angle of deviation
Cai® 2007
31
A ray of white-wavelength incident on a prismA ray of white-wavelength incident on a prism
RB
White light
Cai® 2007
32
33
Reflection of RadiationReflection of Radiation
212
212
0 )(
)(
nn
nn
I
I r
I0: intensity of incident lightIr: reflected intensity
For monochromatic For monochromatic light hitting a flat light hitting a flat surface at 90surface at 9000
34
Reflection of RadiationReflection of Radiation
35
Specular reflection: Reflection of light from a Specular reflection: Reflection of light from a smooth surfacesmooth surface
Diffuse reflection: Reflection of light from a rough Diffuse reflection: Reflection of light from a rough surfacesurface
Smooth or rough surface ???????
36
Reflection
Refraction
M1
M2
37Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
at different interfacesat different interfacesReflectance Reflectance is is the fraction of the incident radiant energy refelcted.the fraction of the incident radiant energy refelcted.
38
Scattering of RadiationScattering of Radiation
Rayleigh scatteringRayleigh scattering Molecules or aggregates of molecules Molecules or aggregates of molecules
smaller than smaller than Scattering by big moleculesScattering by big molecules
Used for measuring particle sizeUsed for measuring particle size Raman ScatteringRaman Scattering
Involves quntized frequency changesInvolves quntized frequency changes
The fraction of radiation transmitted at all angles from its original path
39
Serway, Physics, 4th edition, 1996
40
Light as ParticlesLight as Particles
c Eh
h
c
Eh
h
Eugene Hecht, Eugene Hecht, OpticsOptics, Addison-Wesley, Reading, MA, 1998., Addison-Wesley, Reading, MA, 1998.
hh = Planck Constant = 6.63 = Planck Constant = 6.63 10 10-34-34 Js Js
41
The Photoelectric EffectThe Photoelectric Effect
Vo: Stopping voltage (the negative voltage at which the photocurrent is zero)
eV0 = h -
: work needed to remove e-
Douglas A. Skoog, Douglas A. Skoog, et al.et al. Principles of Instrumental Analysis, Principles of Instrumental Analysis, ThomsonThomson, , 20072007
42
Cut-off
Current is Current is proportional to the proportional to the intensity of the intensity of the radiationradiation
VV00 depends on the depends on the frequency of the frequency of the radiation and the radiation and the chemical composition chemical composition of the coatingof the coating
VV00 depends on depends on the the chemical composition chemical composition of the coating on the of the coating on the photocathodephotocathode
VV00 independent of the independent of the intensity of the intensity of the radiationradiation
Douglas A. Skoog, Douglas A. Skoog, et al.et al. Principles of Instrumental Analysis, Principles of Instrumental Analysis, ThomsonThomson, , 20072007
43
Energy States of Energy States of ChemicalChemical
Quantum theory by Quantum theory by PlanckPlanck (1900) (1900)
Black body radiationBlack body radiation Atoms, ions , and Atoms, ions , and
molecules exist in molecules exist in discrete statesdiscrete states
Characterized by Characterized by definite amounts of definite amounts of energyenergy
Changes of state Changes of state involve absorption or involve absorption or emission of energyemission of energy
EE11-E-E00 = = hh = = hhc/c/
44
Interaction of Radiation Interaction of Radiation and Matterand Matter
Emission and Chemiluminescence Process
45
Interaction of Radiation Interaction of Radiation and Matterand Matter
Absorption Process
46
Interaction of Radiation Interaction of Radiation and Matterand Matter
Photoluminescence method (Fluorescence and phosphorescence)
47
Interaction of Radiation Interaction of Radiation and Matterand Matter
Inelastic Scattering in Raman Spectroscopy
48
Emission of RadiationEmission of Radiation
Douglas A. Skoog, F. James Holler and Timothy A. Nieman, Principles of Douglas A. Skoog, F. James Holler and Timothy A. Nieman, Principles of Instrumental Analysis, Saunders College Publishing, Philadelphia, 1998.Instrumental Analysis, Saunders College Publishing, Philadelphia, 1998.
EmissionEmission XX** X + h X + h
Excitation needs energy!
•Particle bombardment (e-)
•Electrical currents (V)
•Fluorescence
•Heat
49
Emission: Saltwater in Emission: Saltwater in a flamea flame
50
Line SpectraLine Spectra
Individual atoms, well separated, in a gas phase
51
Band SpectraBand Spectra
Small molecules and radicals
Vibrational levels
52
Continuum SpectraContinuum Spectra Produced when solid are heated to Produced when solid are heated to
incandescence. incandescence. Blackbody Radiation (Thermal Radiation) Blackbody Radiation (Thermal Radiation)
53
Blackbody RadiationBlackbody Radiation A A blackbodyblackbody is a theoretical is a theoretical
object, (i.e. object, (i.e. emissivityemissivity = 1.0), = 1.0), which is both a perfect absorber which is both a perfect absorber and emitter of radiation. and emitter of radiation. Common usage refers to a source Common usage refers to a source of infrared energy as a of infrared energy as a "blackbody" when it's emissivity "blackbody" when it's emissivity approaches 1.0 (usually e = 0.99 approaches 1.0 (usually e = 0.99 or better) and as a "graybody" if or better) and as a "graybody" if it has lower emissivity. it has lower emissivity.
Important sources of infrared, Important sources of infrared, visible, and long wavelength UV visible, and long wavelength UV for analytical instrumentsfor analytical instruments
http://www.electro-optical.com/bb_rad/bb_rad.htm
54
Wien’sWien’sDisplacement LawDisplacement Law
T
nmK 10 2.897
6
max
T
nmK 10 2.897
6
max
Eugene Hecht, Eugene Hecht, OpticsOptics, Addison-Wesley, Reading, MA, 1998., Addison-Wesley, Reading, MA, 1998.
Stefan-Boltzman LawStefan-Boltzman Law
P = P = TT44
= 5.6697 = 5.6697 10 10-12-12 Wcm Wcm-2-2KK-4-4
Blackbody RadiationBlackbody Radiation
Both max and radiation power (P) are related to TEMPERATURE and current!
55
Continuum SourceContinuum Source Line SourceLine Source
Continuum + Line SourceContinuum + Line Source
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
Al + Mg
56
Ranges of Common SourcesRanges of Common Sources
Douglas A. Skoog and James J. Leary, Douglas A. Skoog and James J. Leary, Principles of Instrumental Principles of Instrumental AnalysisAnalysis, Saunders College Publishing, Fort Worth, 1992., Saunders College Publishing, Fort Worth, 1992.
57
Optical Source CharacteristicsOptical Source Characteristics
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
58
Nernst GlowerNernst GlowerRare earth oxides formed into a Rare earth oxides formed into a cylinder (1-2 mm diameter, cylinder (1-2 mm diameter, ~20mm long).~20mm long).
Pass current to give:Pass current to give:T = 1200 – 2200 K.T = 1200 – 2200 K.
Ingle and Crouch, Ingle and Crouch, Spectrochemical Spectrochemical AnalysisAnalysis
Douglas A. Skoog and James J. Leary, Douglas A. Skoog and James J. Leary, Principles of Instrumental Principles of Instrumental AnalysisAnalysis, Saunders College Publishing, Fort Worth, 1992., Saunders College Publishing, Fort Worth, 1992.
59
GlobarGlobar
Silicon Carbide Rod (5mm diameter, 50 mm long).Silicon Carbide Rod (5mm diameter, 50 mm long).
Heated electrically to 1300 – 1500 K.Heated electrically to 1300 – 1500 K.
Positive temperature coefficient of resistancePositive temperature coefficient of resistance
Electrical contact must be water cooled to prevent arcing.Electrical contact must be water cooled to prevent arcing.
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
60
Tungsten FilamentTungsten Filament
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
Heated to 2870 K.Heated to 2870 K.
Useful Range: 350 – 2500nmUseful Range: 350 – 2500nm
61
Tungsten / HalogenTungsten / Halogen
Iodine added.Iodine added.
Reacts with gaseous W near the quartz wall to form WIReacts with gaseous W near the quartz wall to form WI22..
W is redeposited on the filament.W is redeposited on the filament.
Gives longer lifetimesGives longer lifetimes
Allows higher temperatures (~3500 K).Allows higher temperatures (~3500 K).
62
Intensity Spectrum of Intensity Spectrum of the Tungsten-Halogen the Tungsten-Halogen
LampLamp
• Weak intensity in UV range• Good intensity in visible range• Very low noise• Low drift
63
Arc LampsArc Lamps
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
Electrical discharge is Electrical discharge is sustained through a gas or sustained through a gas or metal vapor.metal vapor.
Continuous emission due to Continuous emission due to rotational/vibrational energy rotational/vibrational energy levels and pressure levels and pressure broadening.broadening.
64
HH22 or D or D22 Arc Lamps Arc Lamps
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
DD22 + E + Ee-e- D D22* * D’ + D” + h D’ + D” + h
Energetics:Energetics: EEe-e- = E = EDD22** = E = ED’D’ + E + ED”D” + h + h
Useful Range: 185 – 400 nm.Useful Range: 185 – 400 nm.
65
Intensity Spectrum of Intensity Spectrum of the Xenon Lampthe Xenon Lamp
• High intensity in UV range• High intensity in visible range• Medium noise
66
Hg Arc LampHg Arc Lamp
Continuum + Line SourceContinuum + Line Source
High Power Source.High Power Source.
Often used in photoluminescence.Often used in photoluminescence.
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
67Douglas A. Skoog and James J. Leary, Douglas A. Skoog and James J. Leary, Principles of Instrumental Principles of Instrumental AnalysisAnalysis, Saunders College Publishing, Fort Worth, 1992., Saunders College Publishing, Fort Worth, 1992.
Hollow Cathode Discharge Tube.Hollow Cathode Discharge Tube.
Apply ~300 V across Apply ~300 V across electrodes.electrodes.
ArAr++ or Ne or Ne++ travel toward the travel toward the cathode.cathode.
If potential is high enough If potential is high enough cations will sputter metal off cations will sputter metal off the electrode.the electrode.
Metal emits photons at Metal emits photons at characteristic atomic lines as characteristic atomic lines as the metal returns to the the metal returns to the ground state.ground state.
68
Hollow Cathode Discharge Tube.Hollow Cathode Discharge Tube.
Line Widths are typically 0.01 – 0.02 Line Widths are typically 0.01 – 0.02 Å.Å.
Ingle and Crouch, Ingle and Crouch, Spectrochemical AnalysisSpectrochemical Analysis
69
Absorption of Absorption of RRadiationadiation
Is a quantized process???Is a quantized process??? The energy absorbed is released, although The energy absorbed is released, although
not necessarily all as light energy (e.g. heat)not necessarily all as light energy (e.g. heat) Results in excitation of a molecule to a Results in excitation of a molecule to a
higher energy statehigher energy state E= E E= E electronicelectronic + E + E vibrationalvibrational + E + E rotationalrotational
70
Absorption of Absorption of RadiationRadiation
Douglas A. Skoog, F. James Holler and Timothy A. Nieman, Principles of Douglas A. Skoog, F. James Holler and Timothy A. Nieman, Principles of Instrumental Analysis, Saunders College Publishing, Philadelphia, 1998.Instrumental Analysis, Saunders College Publishing, Philadelphia, 1998.
71
Atomic absorption
72
Rotational energy levels associated with each vibrational level not shown
73
Relaxation Resonance fluorescence
F = A
Non- Resonance fluorescence F A
Stokes shift F > A
74
Quantitative Aspects of Quantitative Aspects of Spectrochemical Spectrochemical MeasurementsMeasurements
Radiation power PRadiation power P The energy of the a beam of The energy of the a beam of
radiation that reaches a given radiation that reaches a given area per secondarea per second
S =kPS =kP
S is an electrical signalS is an electrical signal Dark currentDark current
Response of the detector in the Response of the detector in the absence of radiationabsence of radiation
S =kP + S =kP + kkdd
75
Quantitative Aspects of Quantitative Aspects of Spectrochemical Spectrochemical MeasurementsMeasurements
TransmittanceTransmittance T = P/PT = P/Po o (definition)(definition)
PPoo - incident light power - incident light power P - transmitted light powerP - transmitted light power
%T = P/P%T = P/Po o x 100 %x 100 % AbsorbanceAbsorbance
A = - log T A = - log T (definition)(definition) Beer’s Law Beer’s Law (physical law applicable under (physical law applicable under
certain conditions)certain conditions) A = A = b c b c (basis of quantitation)(basis of quantitation)
- molar absorptivity (L mol- molar absorptivity (L mol-1-1 cm cm-1-1)) b - pathlength (cm)b - pathlength (cm) c - concentration (mol Lc - concentration (mol L-1-1))
76
Non-radiative Non-radiative relaxationrelaxation
Vibrational Relaxation:Vibrational Relaxation: A molecule can give off some of its energy from A molecule can give off some of its energy from
absorbed light (usually uv-vis) by jumping to a lower absorbed light (usually uv-vis) by jumping to a lower energy vibrational state.energy vibrational state.
The excess energy is used to make the conversion. No The excess energy is used to make the conversion. No light is given off.light is given off.
Internal Conversion:Internal Conversion: The molecule transitions to a lower energy electronic The molecule transitions to a lower energy electronic
state without giving off light. state without giving off light. Excess energy is used to covert the molecule from one Excess energy is used to covert the molecule from one
electronic state to another.electronic state to another. Poorly understoodPoorly understood
External conversion:External conversion: The molecule gives off energy to an external source, The molecule gives off energy to an external source,
such as by collision with another similar molecule or such as by collision with another similar molecule or solvent molecule. This is called solvent molecule. This is called ““quenchingquenching””
Intersystem Crossing:Intersystem Crossing: The molecule goes from a singlet to triplet excited The molecule goes from a singlet to triplet excited
state and uses up energy changing the spin of an state and uses up energy changing the spin of an electron.electron.