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Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

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Page 1: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Lecture 3IOPs: Absorption physics and

absorbing materials

Collin Roesler3 July 2007

Page 2: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Lecture Overview

• Overview of the electromagnetic spectrum

• What is absorption?• Who are the absorbers?• Impacts on ocean color

Page 3: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Electromagnetic Spectrum• Charged particles create

electric fields (oscillation between +,-)

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

• The electromagnetic field oscillates as the energy propagates

• the range of oscillation frequencies is described by the EM spectrum

http://wps.prenhall.com/wps/media/objects/610/625137/Chaisson

Page 4: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Black body radiation

http://aeon.physics.weber.edu/jca/PHSX1030/Images/blackbody.jpg

• Any object with a temperature >0 K emits electromagnetic radiation

• The spectrum of that emission depends upon the temperature (Planck’s Law)

• As T , emitted energy (Stefan-Boltzman’s Law), and the frequency of emitted energy (shorter wavelengths)

• As T , the of maximal emission (Wein’s Law)

• Energy contained in a packet of EM radiation (e.g. visible photon) with wavelength

Page 5: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

So the sun, at ~5800 K, emits primarily visible radiation (light),

most of which penetrates the atmosphere

Page 6: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Light Penetration

Page 7: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

What is absorption?

• since electromagnetic radiation is energy propagation, when materials absorb radiation, they absorb energy

• what happens to the molecule depends upon the wavelength (frequency)

Page 8: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Interactions between energy and matter

MICROWAVE

Page 9: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

The amount of energy required to move an electron to another orbital shell is

quantized

400 450 500 550 600 650 700

interatomic distance

Page 10: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

quantized energy states

400 450 500 550 600 650 700

interatomic distance

Page 11: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

quantized vibrational states

interatomic distance

400 450 500 550 600 650 700

Page 12: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

The chlorophyll a molecule has two higher energy orbital shells associated with the

energy equivalent of a blue (443 nm) and a red (676 nm) photon

http://www.mie.utoronto.ca/labs

Page 13: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Example of absorption spectra for three environments

0

0.2

0.4

0.6

0.8

400 500 600 700

Wavelength (nm)

abso

rpti

on (

m-1)

open ocean

coastal

estuarine

all have strong red absorption

but variable blue absorption

Page 14: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing matter

aT = aw + adissolved compounds + aparticles

Ideally…

Page 15: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing matter

waterchromophoric dissolved matterphytoplankton (in vivo pigments)chromophoric organic particulate matter (not pigments)chromophoric inorganic particulate matter (minerals)

aT = aw + aCDM + a + aCOPM + aCIPM

Practically…

Page 16: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:Water

variations are methodological

Page 17: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:Water

natural variations

Pegau and Zaneveld 1993 Limnol Oceanogr.

Temperature

5oC

30oC

Page 18: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:Water

natural variations

Pegau etal. 1997 Appl.Opt.

Salinity

Page 19: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:Chromophoric Dissolved Matter

aCDM() = aCDM(o) exp(-S (-o))

Kirk 1983Carder et al. 1989 L&O

Page 20: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:Chromophoric Dissolved Matter

aCDM() = aCDM(o) exp(-S (-o))

Carder et al. 1989 L&O

S0.01

0.02

S=0.014

S=0.011

Simeon et al. 2003 JGR

Equatorial Pacific

Page 21: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:Phytoplankton

1989 L&O

Individual cells

Roesler et al. 1989 L&O

Species

Page 22: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:Phytoplankton

Pigment Packaging impact on absorption

Morel and Bricaud 1981 DSR

Page 23: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:other protists

Morel and Ahn 1990 JMR

heterotrophic bacteriaciliates and flagellates

cytochrome 412

Page 24: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:organic detrital particles

Iturriaga and Siegel 1989 L&OJMR

Page 25: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

Absorbing Components:inorganic particles

Babin and Stramski 2003Patterson et al. 1977 JGR

Page 26: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

To model the impacts of absorbing constituents…add them up

0

0.2

0.4

0.6

0.8

400 500 600 700

Wavelength (nm)

abso

rpti

on (

m-1)

Page 27: Lecture 3 IOPs: Absorption physics and absorbing materials Collin Roesler 3 July 2007

More on absorption

• CDOM absorption methods– Lecture today– Lab today

• Phytoplankton absorption– Lecture Thursday

• Particulate absorption methods– Lecture Thursday– Lab Thursday