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Atomic emissions and absorption
Instrumentation I Atomic emissions and absorption 2/12/11
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Atomic emission E = hv = h*c/l
When excited, an atom will absorb external energy and raise its electrons above the ground state. This is a transient and unstable state. The electrons will return to the ground state, but need to return the energy they absorbed to reach the higher state in discrete quanta of energy.
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Every element has a distinct pattern of allowable quanta based on
the electron configuration of that element. h = Plank’s constant = x J*sec The energy is typically given off as light Hydrogen is the easiest to visualize
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According to Plank’s equation, each transition can be related
to a wavelength
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Each element will have a distinctive pattern of emission
Hydrogen nm Iron
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Note that all wavelength in a spectra do not have the same intensity
This can be caused by re-absorbtion or interference) Hg spectrum
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Prismatic dispersion
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Diffraction. Close point sources
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Reflective diffraction
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Atomic emission spectroscopy
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Getting the best excitation = ICP
Induction Coupled Plasma
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ICP reduces sample induced interferences- 7000-8000 degree plasma
Primarily used in metals analysis Sensitive to 1 part/billion range
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Atomic absorption spectroscopy
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Example AAS
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Comparision
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FTIR Absorption of broadband infrared and subsequent analysis
of interference
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Typical FTIR spectrum
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polypropylene Comparison analysis
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