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Published bySuparman Irawan Modified over 6 years ago
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Lecture 8 Detectors Spectrophotometer design Background correction
Width of the spectral peak Ch Harris
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Spectrometer Monochromator Detector (filter, wavelength selector)
Light Source Detector Sample Spectrometer Data Processing
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A phototube K/Cs/Sb GaAs - + Ag/O/Cs 90 V Wavelength, nm
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Photomultiplier Anode Several electrons for each incident electron
for each photon Quarz envelope Light, h Photoemissive cathode Anode
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Photoelectromultiplier
dynode dynode photon electron
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Single beam Double beam
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Double beam with the beams separated in time
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Single beam design with
210-element area detector
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Flat background Ipeak Ipeak – I0 I0 I Intensities at two different
wavelengthes Peak I0 Baseline wavelength
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Flat background Ipeak I0 I Peak First derivative eliminates
constant Peak First derivative eliminates flat background I0 Baseline Wavelength (l)
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Linear Background Ipeak Ipeak – (I1+I2) / 2 I1 I2 I Background
Wavelength (l)
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Linear Background Ibackground = Kl+b I Background
First: Background Second: Second derivative eliminates linear background Wavelength (l)
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Original Second 4th First
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Well defined peaks and valleys
High noise Some peaks visible Almost featureless: little information Low noise
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Only photons of one specified wavelength are
absorbed Excited state Ground state
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Width Velocity of a particle >1000 m/s Doppler
Speed of light 300,000,000 m/s collisions Approximately as Doppler Both effects increase with the temperature and decrease with the size of the molecule/atom Width is around nm in visible area Multiple energy levels
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Energy levels of excited state Energy sublevels Energy levels of ground state
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Molecular spectra - wide bands
A primitive rule: Molecular spectra - wide bands Atomic spectra - narrow lines
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