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An Introduction
to
Spectrometric Methods
1
Bivek Timalsina
bivektim@gmail.com
Quantum Mechanical Properties of
Electromagnetic Radiation (EMR)
 The amount of energy involved in transitions from its ground state to
exited state (following absorption of energy) and from excited to ground
state (by emission of radiation) is given by the following equation;
ΔE = E1 – E2 = hV
where, ΔE = change in energy state of the electron or the energy of
electromagnetic radiation absorbed or emitted by an atom or molecule.
E1 = energy of electron in original state,
E2 = energy of electron in the final state,
h = the Plank’s constant
V= frequency of the electromagnetic radiation in hertz (C/ λ),
where, C= speed of electromagnetic radiation (3x108 m/s)
λ = wavelength of electromagnetic radiation
(= 6.63 x 10-34 JS)The greater the energy, the higher the frequency and
wavenumber and the shorter the wavelength
2
Energy level and transition in atom and
molecule
E0
E1
E2
E3
E4
Atomic energy level Molecular energy level
3
Emission of Radiation
4
Absorption of Radiation
5
The Beer-Lambert Law
I0
Sample
I
Detector
Source
Cuvette
6
 Transmittance, T, is simply defined as “the fraction of light that reaches a
detector after passing through a sample”
T = I/I0 …………… (i)
Where, I0 = intensity of Incident radiation
I= intensity of transmitted radiation
 Percentage Transmission (%T) = % T = I/I0 x 100
0 < %T < 100
The Beer-Lambert Law
 Absorbance (A):
A = -log T = log (1/T) = log (I o / I)
Absorbance is also called as Optical Density (O.D.)
range from 0 (= 100% T) to infinity (=0%T).
 The Beer-Lambert law states
Absorbance is directly proportional to:
1. concentration, c, of absorbing species in the sample (A c)
2. path length of light, L, through the sample (A L)
A = € C L ……………… (iii)
Where, € = Molar absorbance coefficient of the absorber
C = Concentration of absorbing solution, and
b = Path length through the solution (or thickness) 7
The Beer-Lambert Law
 Absorbance (A):
A = € C L ……………… (iii)
 Concentration of the analyte is given in unit mol/L (M)
 The path length, L, in cm
 , is called the molar absorptivity or molar absorption
coefficient
“Absorbance of 1 M solution measured in a cell of 1 cm
pathlength”
 , is characteristic for each substance at a particular
wavelength, .
11111 
 cmMcmmolL
cm
L
molcl
A

8
Concentration
Absorbance,A
0
0.5
1
Concentration
Transmittance,T
A=cL
certain 
constant L
One analyte
T=10-A =10- bc
Beer’s law is a relation between absorbance
and concentration which is a straight line
passes by origin at constant pathlength, b,
and at certain wavelength, .
Transmittance decreases
exponentially as concentration
increases
Beer’s law is obeyed for
monochromatic light
Slope = L
The Beer-Lambert Law
9
Beer’s Law and Multicomponent samples
 For sample containing several absorbing components (say X and
Y) given that there are no interactions between the components, the
total absorbance is,
Atotal = Ax+ By = €x Cx L + €y Cy L
10
The Beer-Lambert Law
Blank
Detector
Source
I0
Use of Blank
I0
Sample
I
Detector
Source
Cuvette
11
The Beer-Lambert Law
A = € C L
Use of Curve
12
This relationship is a linear for the most part. However, under certain
circumstances the Beer relationship gives a non-linear relationship.
These deviations from the Beer Lambert law can be classified into three
categories:
Real Deviations - These are fundamental deviations due to the limitations
of the law itself.
Chemical Deviations- These are deviations observed due to specific
chemical species of the sample which is being analyzed.
Instrument Deviations - These are deviations which occur due to how the
absorbance measurements are made.
Derivation of Beer Lambert Law
13
Readout
Absorbance
0.00
Source
Detector
The Beer-Lambert Law
A = € C L
14
Path Length Dependence, L
Path Length Dependence, L
Readout
Absorbance
0.22
Source
Detector
b
Sample
The Beer-Lambert Law
A = € C L
15
Path Length Dependence, L
Readout
Absorbance
0.44
Source
Detector Samples
Of course, we are not introducing two cells in the
light pathway, but let us assume that we doubled
the path length of light through the absorbing
medium
The Beer-Lambert Law
A = € C L
16
Readout
Absorbance
0.66
Source
Detector Samples
The Beer-Lambert Law
A = € C L
17
Path Length Dependence, L
Concentration Dependence, c
Readout
Absorbance
0.00
Source
Detector
The Beer-Lambert Law
A = € C L
18
Concentration Dependence, c
Readout
Absorbance
0.42
Source
Detector
b
Sample
The Beer-Lambert Law
A = € C L
19
Concentration Dependence, c
Readout
Absorbance
0.63
Source
Detector
b
Sample
The Beer-Lambert Law
A = € C L
20
Wavelength Dependence, 
Readout
Absorbance
0.30
Source
Detector
b
The blue solution do absorb the red radiation
The Beer-Lambert Law
A = € C L
21
Wavelength Dependence, 
Readout
Absorbance
0.00
Source
Detector
b
The red solution can not absorb the red
radiation but it can absorb radiation that
is complimentary to red.
The Beer-Lambert Law
A = € C L
22
23

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Introduction to spectroscopic methods

  • 2. Quantum Mechanical Properties of Electromagnetic Radiation (EMR)  The amount of energy involved in transitions from its ground state to exited state (following absorption of energy) and from excited to ground state (by emission of radiation) is given by the following equation; ΔE = E1 – E2 = hV where, ΔE = change in energy state of the electron or the energy of electromagnetic radiation absorbed or emitted by an atom or molecule. E1 = energy of electron in original state, E2 = energy of electron in the final state, h = the Plank’s constant V= frequency of the electromagnetic radiation in hertz (C/ λ), where, C= speed of electromagnetic radiation (3x108 m/s) λ = wavelength of electromagnetic radiation (= 6.63 x 10-34 JS)The greater the energy, the higher the frequency and wavenumber and the shorter the wavelength 2
  • 3. Energy level and transition in atom and molecule E0 E1 E2 E3 E4 Atomic energy level Molecular energy level 3
  • 6. The Beer-Lambert Law I0 Sample I Detector Source Cuvette 6  Transmittance, T, is simply defined as “the fraction of light that reaches a detector after passing through a sample” T = I/I0 …………… (i) Where, I0 = intensity of Incident radiation I= intensity of transmitted radiation  Percentage Transmission (%T) = % T = I/I0 x 100 0 < %T < 100
  • 7. The Beer-Lambert Law  Absorbance (A): A = -log T = log (1/T) = log (I o / I) Absorbance is also called as Optical Density (O.D.) range from 0 (= 100% T) to infinity (=0%T).  The Beer-Lambert law states Absorbance is directly proportional to: 1. concentration, c, of absorbing species in the sample (A c) 2. path length of light, L, through the sample (A L) A = € C L ……………… (iii) Where, € = Molar absorbance coefficient of the absorber C = Concentration of absorbing solution, and b = Path length through the solution (or thickness) 7
  • 8. The Beer-Lambert Law  Absorbance (A): A = € C L ……………… (iii)  Concentration of the analyte is given in unit mol/L (M)  The path length, L, in cm  , is called the molar absorptivity or molar absorption coefficient “Absorbance of 1 M solution measured in a cell of 1 cm pathlength”  , is characteristic for each substance at a particular wavelength, . 11111   cmMcmmolL cm L molcl A  8
  • 9. Concentration Absorbance,A 0 0.5 1 Concentration Transmittance,T A=cL certain  constant L One analyte T=10-A =10- bc Beer’s law is a relation between absorbance and concentration which is a straight line passes by origin at constant pathlength, b, and at certain wavelength, . Transmittance decreases exponentially as concentration increases Beer’s law is obeyed for monochromatic light Slope = L The Beer-Lambert Law 9
  • 10. Beer’s Law and Multicomponent samples  For sample containing several absorbing components (say X and Y) given that there are no interactions between the components, the total absorbance is, Atotal = Ax+ By = €x Cx L + €y Cy L 10
  • 11. The Beer-Lambert Law Blank Detector Source I0 Use of Blank I0 Sample I Detector Source Cuvette 11
  • 12. The Beer-Lambert Law A = € C L Use of Curve 12
  • 13. This relationship is a linear for the most part. However, under certain circumstances the Beer relationship gives a non-linear relationship. These deviations from the Beer Lambert law can be classified into three categories: Real Deviations - These are fundamental deviations due to the limitations of the law itself. Chemical Deviations- These are deviations observed due to specific chemical species of the sample which is being analyzed. Instrument Deviations - These are deviations which occur due to how the absorbance measurements are made. Derivation of Beer Lambert Law 13
  • 14. Readout Absorbance 0.00 Source Detector The Beer-Lambert Law A = € C L 14 Path Length Dependence, L
  • 15. Path Length Dependence, L Readout Absorbance 0.22 Source Detector b Sample The Beer-Lambert Law A = € C L 15
  • 16. Path Length Dependence, L Readout Absorbance 0.44 Source Detector Samples Of course, we are not introducing two cells in the light pathway, but let us assume that we doubled the path length of light through the absorbing medium The Beer-Lambert Law A = € C L 16
  • 17. Readout Absorbance 0.66 Source Detector Samples The Beer-Lambert Law A = € C L 17 Path Length Dependence, L
  • 21. Wavelength Dependence,  Readout Absorbance 0.30 Source Detector b The blue solution do absorb the red radiation The Beer-Lambert Law A = € C L 21
  • 22. Wavelength Dependence,  Readout Absorbance 0.00 Source Detector b The red solution can not absorb the red radiation but it can absorb radiation that is complimentary to red. The Beer-Lambert Law A = € C L 22
  • 23. 23

Notas del editor

  1. Log 10 X = Y ------ X = 10Y Log 1000 = 3 ------ 1000 = 103