Print version Updated: 17 April 2013 Lecture #33 Toxics: Photolysis (Chapra, L42) David Reckhow CEE 577 #33 1
Overall decay rate k 1 is a combination of Hydrolysis (k h ) Photolysis (k p ) Biodegradation (k b ) Any other loss process not otherwise included in the model Any of these processes may be affected by sorption Photolysis is most commonly attributed to dissolve forms only 𝑙 1 = 𝑙 ℎ + 𝑔 𝑞1 𝑙 𝑞 + 𝑙 𝑐 David Reckhow CEE 577 #33 2
Photolysis Chemical breakdown initiated by light energy two types direct photolysis sensitized (or indirect) photolysis Several steps some solar light reaches water surface some of this light penetrates to the solute some of this is absorbed by the solute some of absorbed light is capable of causing a reaction David Reckhow CEE 577 #33 3
Solar Radiation David Reckhow CEE 577 #33 4
Attenuation of light through water Attenuation coefficient (cm -1 ) Beer-Lambert’s Law − α λ λ = λ ( ) z I ( z , ) I ( 0 , ) e D Light Intensity (einstein/cm 2 /s) at depth z, and wavelength, λ and the attenuation coefficient is from: λ 1 I ( 0 , ) α λ = ( ) ln λ D H I ( H , ) David Reckhow CEE 577 #33 5
Measured light intensity with depth Lake San Vincente Tyler & Smith, 1970 David Reckhow CEE 577 #33 6
Average light absorption over depth H ( ) λ I ( 0 , ) − α λ = − ( ) H I 1 e D H einsteins/cm 3 /s David Reckhow CEE 577 #33 7
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Spectral overlap (a) benzene; (b) naphthacene or tetracene David Reckhow CEE 577 #33 9
Absorption of Light Molar extinction coefficient (L/mole/cm) Attenuation due to background and contaminant [ ] − α λ + ε λ λ = λ ( ) ( ) c I ( , ) I ( 0 , ) e Integrating over the depth and isolating on the contaminant we get: − α λ − ε λ λ ( ) H ( ) I ( 0 , )( 1 e ) D λ = ( ) I c α λ a H ( ) David Reckhow CEE 577 #33 10
Quantum Yield Once absorption occurs, energy is dissipated by: emission of heat emission of light: luminescence contact with another molecule: photosensitization decomposition: direct photolysis Fraction following last pathway is quantum yield number of moles transform ed Φ r λ = ( ) λ total moles of photons of wavelengt h absorbed And combining with absorption equation: − α λ ε λ λ − ( ) H ( ) I ( 0 , )( 1 e ) D λ = Φ λ λ = Φ λ ( ) ( ) ( ) ( ) k k α λ p a H ( ) David Reckhow CEE 577 #33 11
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To next lecture David Reckhow CEE 577 #33 13
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