lecture 29 ch18&19
TRANSCRIPT
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CHM 320 Lecture 30 Chapt. 18, 20
Chapter 18 Fundamentals of
Spectrophotometry (contd)AND
Chapter 20 - Spectrophotometers
Homework for Chapter 20 Due Friday, April 19
Problems 20-1, 20-3, 20-4, 20-6, 20-26 Note: We will talk about some applications of spectrophotometryin class, but will not have any homework assigned from Chapt. 19.
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CHM 320 Lecture 30 Chapt. 18, 20
Absorption of Light
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T = P/P owhere T => transmittance
P => power of transmittedradiationPo => power of incident
radiation%T = (P/P o)*100
where %T => percent transmittance
Absorption Methods,Transmittance
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Absorbance => A = - log 10T = - log 10 (P/P o)
Absorbance and transmittance
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CHM 320 Lecture 30 Chapt. 18, 20
Absorption Methods,Beers Law
A = bc
b => path length (cm)c => concentration (M)
=> molar absorptivity(M -1cm -1)
A
Concentration (M)
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CHM 320 Lecture 30 Chapt. 18, 20
Light sources
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Examples of Sources
Deuterium lamp - good source for UV continuumradiation - widely used in UV spectrophotometers
Tungsten filament lamp - Good source of continuumradiation in the 330- 2000 nm range; common invisible, near-IR colorimeters, spectrophotometers.
Stable light output with regulated power supply.Similar to regular light-bulb but run at 3000 K. Heated metal and ceramic filaments used for the
mid-IR, which is ~ 500-4000 cm -1 (A warm objectis an efficient IR source). Common source for IRspectroscopy is called a Nernst Glower, globar, or anichrome wire.
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Purpose of monochromator:
Separation of multi- light into individual s
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MonochromatorsComponents:
entrance slit, collimating element (lens or mirror),prism or grating as dispersing element, focusingelement (lens or mirror), exit slit
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monochromator
http://www.chem.hope.edu/~polik/labtour/monochromator-inside.html
An important use of diffraction isin produci ng monochromaticlight from white light sources
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How do gratings work?
The incident beam isdiffracted in a mannergiven by Equation (1)
The term m isreferred to as theorder of thediffraction
Dispersion increases
with order butintensity diminishes
http://www.optics.org/spectrogon/holograt/specprop.html
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CHM 320 Lecture 30 Chapt. 18, 20
Sample ContainersUltra-Violet
quartz
Visible quartz
glassInfrared
NaCl AgCl KBr
Criteria for Sample Containers Transparent to excitation light
Compatible with samples Rugged
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CHM 320 Lecture 30 Chapt. 18, 20
Types of DetectorsUV-Visible
Photon Detectors Vacuum Phototubes Photomultiplier Tubes
Photodiodes Linear Photodiode arrays
Charge-Transfer (Charge Coupled Device, CCD)Infrared
Heat Detectors
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Photoelectric effect based detectors:
phototubes
Phototubes are usedfor high light intensityapplications
Photons producephotoelectrons; thephotocurrent isproportional tointensity
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Photomultiplier tubesare used for low lightintensity and photoncounting applications
Photons strike primaryelectrode, emits e-;these electrons strike
successive secondarysurfaces, finallyproducing a largepulse of electrons
http://laxmi.nuc.ucla.edu:8248/M248_99/autorad/Scint/pmt.html
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Semiconductor-base Detectors (Photodiodes and CCDs)
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Detectors for IR
Heat detectors
thermocouple Ferroelectric
Semiconductor-based detectors (like HgCdTe)
Low bandgap semiconductors
Must be cooled for good quantum efficiency,low noise