lecture 3 absorption physics and absorbing materials

39
Lecture 4 Absorption Part 1 – theoretical basis of absorption, absorption by individual particles, bulk absorption Collin Roesler 20 July 2021

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Page 1: Lecture 3 Absorption physics and absorbing materials

Lecture 4

Absorption Part 1 – theoretical basis of absorption, absorption by individual particles, bulk absorption

Collin Roesler

20 July 2021

Page 2: Lecture 3 Absorption physics and absorbing materials

Lecture Overview

• Overview of the electromagnetic spectrum

• Absorption on molecular scales

• Major absorbers in the ocean

• Lecture 5: Measuring absorption in the ocean

• Lab 2: Absorption by solutions

• Lab 3: Absorption by particles

Page 3: Lecture 3 Absorption physics and absorbing materials

Electromagnetic Radiation

• Charged particles (dipoles) create electric fields E (oscillation between +,-)

+_

Page 4: Lecture 3 Absorption physics and absorbing materials

Electromagnetic Radiation

• Charged particles, dipoles, create electric fields E (oscillation between +,-)

• When a charged particle moves, it creates a magnetic field, B

• The electromagnetic field oscillates as the energy propagates ExB (right hand rule)

Page 5: Lecture 3 Absorption physics and absorbing materials

Electromagnetic Radiation

• Charged particles, dipoles, create electric fields E (oscillation between +,-)

• When a charged particle moves, it creates a magnetic field, B

• The electromagnetic field oscillates as the energy propagates ExB (right hand rule)

• the range of oscillation frequencies is described by the Electro-Magnetic (EM) spectrum

http://www.antonine-education.co.uk/physics_gcse

Page 6: Lecture 3 Absorption physics and absorbing materials

What is absorption?

• Since electromagnetic radiation is energy propagation, when molecules absorb radiation, they absorb energy

• The energy associated with each part of the spectrum is given by E = hc/l• h Planck’s constant

• c speed of light in a vacuum

• l wavelength

• What happens to the molecule depends upon the amount of energy, and therefore the wavelength

Page 7: Lecture 3 Absorption physics and absorbing materials

MICROWAVEExtreme UV Infrared MicrowaveUltravioletX-raysGamma rays

Visible

Interactions between energy and matter

molecularrotation

molecularvibration

Electrontransition

Nuclearconfiguration

Photo-ionization

Page 8: Lecture 3 Absorption physics and absorbing materials

Quantized electronic states• Amount of energy required to move an electron to a higher orbital (electronic state

transition) is quantized

• A molecule absorbs radiation only of this specific quantized energy

• The quantized energy determines the absorption peak wavelength

• This example shows a molecule with two higher energy levels (E2 and E3) and thus two absorption peaks

Electrontransition

Page 9: Lecture 3 Absorption physics and absorbing materials

Quantized vibrational states

• Each orbital is associated with a series of higher excited states, associated with vibrational energy, which are also quantized

• These determine the wavelengths of the absorption side peaks that have higher or lower energy, but have a lower probability for absorption

molecularvibration

Page 10: Lecture 3 Absorption physics and absorbing materials

Quantized rotational states

• Each vibrational state is associated with a series of higher rotational states, which are also quantized

• These determine the wavelengths of the absorption that smooth the absorption peaks

molecularrotation

Page 11: Lecture 3 Absorption physics and absorbing materials

Quantized states• Each level is really a distribution as a function of internuclear

separation

• With probabilities (likelihoods of occurrence)

• Higher probability of transition → higher absorption coefficient

Page 12: Lecture 3 Absorption physics and absorbing materials

Chlorophyll a has two electronic states associated with the energy equivalent of blue

(443 nm) and red (676 nm) wavelengths

http://plantphys.info/plant_physiology/light.shtml http://www.mie.utoronto.ca/labs

Tetra (4) pyrrole rings

Phytol chain (tail)

Page 13: Lecture 3 Absorption physics and absorbing materials

Chlorophyll a

http://scifun.chem.wisc.edu/chemweek/chlrphyl/chlrphyl.gif

http://www.photochembgsu.com/assets/images/graph2.gif

Soret band Q-band

Page 14: Lecture 3 Absorption physics and absorbing materials

Milenković et al. 2012

Rückmann et al 1999

Page 15: Lecture 3 Absorption physics and absorbing materials

What are the major absorbers in the ocean?

Page 16: Lecture 3 Absorption physics and absorbing materials

Example of absorption spectra for three environments

• What do they have in common?• All have strong red

absorption

• How do they differ?• Variable blue

absorption

0

0.2

0.4

0.6

0.8

400 500 600 700

a(l

) (

m-1

)

Wavelength (nm)

estuarine

coastal

open ocean

Page 17: Lecture 3 Absorption physics and absorbing materials

Absorption is a conservative property

• Total absorption = sum of individual absorbing constituents

𝑎𝑡𝑜𝑡𝑎𝑙 = 𝑎𝑤𝑎𝑡𝑒𝑟 +𝑎𝑑𝑖𝑠𝑠𝑜𝑙𝑣𝑒𝑑 +𝑎𝑝𝑎𝑟𝑡𝑖𝑐𝑙𝑒𝑠

• Absorption is proportional to the concentration (Beer’s Law)

𝑎𝑐ℎ𝑙 𝑚−1 = [𝑐ℎ𝑙](

𝑚𝑔

𝑚3) × 𝑎𝑐ℎ𝑙

∗ (𝑚2

𝑚𝑔)

Page 18: Lecture 3 Absorption physics and absorbing materials

It is impractical to measure absorption spectrum for each absorber

Group components by their common absorption properties (an our inability to separate them operationally)

𝑎𝑇 = 𝑎𝑤 + 𝑎𝐶𝐷𝑂𝑀 + 𝑎𝑛𝑎𝑝 + 𝑎𝑝ℎ𝑦𝑡 +⋯

Page 19: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Water

By Kebes at English Wikipedia, CC BY-SA 3.0, https://commons.wikimedia.org/w/index.php?curid=23793083

Page 20: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Water

Nice (but dated) compendium athttp://omlc.org/spectra/water/abs/index.html

R. M. Pope and E. S. Fry 1997Integrating cavity absorption meter

Page 21: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Water

variations are methodological

Page 22: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Water

natural variations

Pegau and Zaneveld 1993 Limnol Oceanogr.

Temperature

5oC

30oC

Sullivan et al. 2006 Appl Opt

Page 23: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Water

natural variations

Pegau etal. 1997 Appl.Opt.

Salinity

Sullivan et al. 2006 Appl Opt

Page 24: Lecture 3 Absorption physics and absorbing materials

Absorbing Components: Dissolved inorganic matter

• Basic for UV detection of nitrate, ISUS

• Johnson, K. S. and L. J. Coletti. 2002

http://www.mbari.org/chemsensor/ISUShome.htm

Page 25: Lecture 3 Absorption physics and absorbing materials

Absorbing Components: Colored dissolved organic matter (CDOM)

Kirk 1983

Dierssen et al. 2006

http://clarklittlephotography.com

a CD

OM

(l)

(m-1

)

Wavelength (nm)

Page 26: Lecture 3 Absorption physics and absorbing materials

Absorbing Components: Colored dissolved organic matter (CDOM)

Kirk 1983

aCDOM(l) = aCDOM(lref) exp(-SCDOM (l-lref))

Carder et al. 1989 L&O

Page 27: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Colored dissolved organic matter (CDOM)

aCDOM(l) = aCDOM(lo) exp(-SCDOM (l-lo))

Carder et al. 1989 L&O

S0.01-humic

0.02-fulvic

S=0.014

S=0.011

Simeon et al. 2003 JGR

Equatorial Pacific –filtrate pore size and spectral slope

Page 28: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Colored dissolved organic matter (CDOM)

Roesler et al. 1989(global synthesis)

Babin et al. 2003(European coastal waters)

Page 29: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Particles

Scan (ap)

Scan (aNAP)Methanolextraction

difference (aphyt)

Kishino et al. 1985

Page 30: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Phytoplankton

Individual cells, microphotometry

1989 L&O

Page 31: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Phytoplankton

Roesler et al. 1989 L&O

Species

Page 32: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Phytoplankton

Global Relationships

Babin et al. 2003

Bricaud et al. 1995

a*phyt

(m2/mg chl)

aphyt(l)aphyt(440)

Page 33: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:other protists

Morel and Ahn 1990 JMR

heterotrophic bacteriaciliates and flagellates

cytochrome 412

Page 34: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Non-Algal Particles

aNAP(l) = aNAP (lo) exp(-SNAP (l-lo))

Roesler et al. 1989(global synthesis)

Babin et al. 2003(European coastal waters)

Page 35: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:Non-algal particles → what are they?

JMR

Photobleaching natural light levels

Iturriaga and Siegel 1989 L&O

Page 36: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:inorganic particles

Babin and Stramski 2003

Patterson et al. 1977 JGR

Page 37: Lecture 3 Absorption physics and absorbing materials

Absorbing Components:inorganic particles

Estapa et al. 2012

2nd Derivative used to quantify concentration of iron oxide mineralsMeasured spectra

Page 38: Lecture 3 Absorption physics and absorbing materials

To model the impacts of absorbing constituents → add them up

Morel and Prieur 1977

Which component dominates?- blue waters- green waters

phytoplankton (V-type)inorganic particles (U-type)

0.000

0.020

0.040

0.060

0.080

400 500 600 700

a(l

) (

m-1

)

Wavelength (nm)

aphyt

acdom

anap

water

Page 39: Lecture 3 Absorption physics and absorbing materials

More on absorption

• Today • Lecture 5: Measuring absorption (Collin)

• Lab 2 CDOM absorption methods

• Wednesday• Lab 3 Particulate absorption methods