Post on 25-Feb-2016
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Lecture 8
DetectorsSpectrophotometer designBackground correctionWidth of the spectral peak
Ch. 20 Harris
Light Source
Sample
Monochromator(filter,
wavelength selector)
Detector
SpectrometerData Processing
- +90 V
A phototube
Wavelength, nm
GaAsK/Cs/Sb
Ag/O/Cs
Photoemissive cathode
Light, h
Quarzenvelope
Anode
Several electronsfor each photon
Several electrons for each incident electron
Photomultiplier
photon electron
Photoelectromultiplier
dynode
dynode
Single beam
Double beam
Double beam with the beams separated in time
Single beam design with 210-element area detector
Baseline
Peak
I
wavelength
I0
Ipeak
Ipeak – I0
Intensities at two different wavelengthes
Flat background
Baseline
Peak
I
Wavelength ()
I0
IpeakFlat background
0)( II
III
signal
backgroundsignaltotal
constant
signalII
First derivative eliminates flat background
Wavelength ()
I
Background
Linear Background
I1
I2
Ipeak
Ipeak – (I1+I2) / 22
21 IIII peaksignal
Wavelength ()
I
Background
Linear Background
Ibackground = K+b 10)( III
III
signal
backgroundsignaltotal
1III signal
2
2
2
2
signalII
First:
Second:
Second derivative eliminates linear background
4 2 0 2 40
0.1
0.2
0.3
.4
0
f x( )
44 x
4 2 0 2 4
0.2
0
0.2
.3
0.3
f x( )
44 x
4 2 0 2 4
0.4
0.2
0
0.2.2
0.5
f x( )
44 x
4 2 0 2 4
0.5
0
0.5
1
1.3
.8
f x( )
44 x
Original
First
Second
4th
Almost featureless:little information
Some peaks visible
Well defined peaks and valleys
Low noise
High noise
Only photons of one specified wavelength areabsorbed
hchE
Ground state
Excited state
Width
Doppler cv
Speed of light 300,000,000 m/s
Velocity of a particle >1000 m/s
collisions Approximately as Doppler
Both effects increase with the temperature and
decrease with the size of the molecule/atom
Multiple energy levels
Width is around 0.01-0.001 nm in visible area
Energy levels of ground state
Energy levels of excited state
Energy sublevels
A primitive rule:
Molecular spectra - wide bands
Atomic spectra - narrow lines