DE = hn em E 2

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Spectroscopic Analysis
Part 3 – Spectroscopy Experiments
Chulalongkorn University, Bangkok, Thailand January 2012
Dr Ron Beckett
Water Studies Centre
School of Chemistry
Monash University, Melbourne, Australia
Email: Ron.Beckett@monash.edu
Water
Studies
Centre
1
Energy is Quantized
The energy of atoms and molecules is quantized.
They can only exist in allowed energy states or levels
Electronic energy levels
in a H atom
1s 2s 2p 3s 3p
The lowest energy state
has the single electron in
the 1s orbital
1s1
2
Absorption and Emission of EMR
When EMR is absorbed or emitted by matter is
does so in whole photons only (NOT fractions)
Absorption involves
promotion from a
lower energy state to
a higher one
Emission results in
a jump from a higher
energy level to a
lower energy level
E2
DE = hn
E1
E2
DE = hn
E1
3
E2
DE = hn
Intensity
E1
n
Frequency
Intensity
E2
DE = hn
n
E1
Frequency
4
1. Absorption Spectroscopy Experiments
Slit
Monochromator
Detector
Light
Source
Sample
Slit
Recorder
5
Techniques of Wavelength Selection
1. Filters
• Absorption filters
– Coloured glass or
gelatin
– Normally broad
spectral bandwidth
• Cutoff or bandwidth
filters
– Can be combined to
provide narrower
bandwidth
6
Techniques of Wavelength Selection
2. Prism Monochromators
2
Entrance
slit
Collimating
lens
1
Prism
Bunsen prism monochromator
Focussing
lens
Focal
plane
Slit
7
Techniques of Wavelength Selection
3. Diffraction Grating Monochromators
– Glass or plastic plate covered with fine lines
– Reflect light of different wavelengths at different angles.
Condition for constructive interference (transmission)
must be achieved where the path difference between
adjacent beams must be an integral number of
wavelengths
n = d(sin i + sin r)
where n is the diffraction order
.
n=1
i
n=2
r
8
3. Diffraction Grating Monochromators
Concave mirrors
Reflection Grating
Entrance slit
1
Exit slit
2
9
3. Diffraction Grating Monochromators
10
EMR Detectors for Spectroscopy
1. Photographic Plates
11
EMR Detectors for Spectroscopy
2. Phototubes and Photomultipliers
Use the photoelectric effect to convert photons into
a measureable electric current
12
EMR Detectors for Spectroscopy
3. Silicon Photodiodes
Consist of a p-n silicon junction which increases
in conductivity when exposed to UV-visible
radiation. The change in conductivity is used
to measure the light intensity.
Photo Diode Array Detectors
A series of such photodiodes can be constructed
and used to simultaneously detect the radiation
of different wavelengths separated by a
13
monochromator
Origin of an Absorption Peak
Energy Transition
E2
DE = hn
E1
Absorption Spectrum
Intensity
n
Frequency
14
Absorption Spectrum
15
Absorption Spectrum
16
2. Emission Spectroscopy Experiments
Sample
Monochromator
Detector
Excitation
Energy
Heat
Electrical
EMR
Slit
Recorder
17
Origin of an Emission Peak
Energy Transition
E2
DE = hn
Excitation
E1
Emission Spectrum
Intensity
n
Frequency
18
3. Fluorescence Spectroscopy Experiments
Monochromator
Sample
nem
Detector
nex
Slit
Slit
Monochromator
Slit
Recorder
Light
Source
19
Origin of a Fluorescence Peak
E2
Energy Transition
E3
DE = hnex
Radiationless energy loss
DE = hnem
E1
Emission Spectrum
Intensity
nem
Frequency
20
21
Forensic Application of Fluorescence
Visualization of fingerprints
Fingerprint visualized
by redwop fluorescent
fingerprint powder
Cyanoacrylate
fumed +
Rhodamine 6G
Cyanoacrylate
fumed
22
4. Chemiluminescence
Excitation to a higher molecular electronic state by
a chemical reaction followed by emission of EMR
E2
Excitation by a
chemical reaction
D E = hn
E1
23
Chemiluminescence Observed in Nature
e.g. firefly, fungi, jellyfish, bacteria, crustacea and fish
all may exhibit bioluminescence.
24
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