Please read Chapter 4 in Archer Textbook

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Presentation transcript:

Please read Chapter 4 in Archer Textbook Greenhouse Gases ATS 150 Spring 2015 Lecture 5 Please read Chapter 4 in Archer Textbook

Gases Gases are made of moving molecules separated by empty space Kinetic energy of molecular motion is proportional to temperature Gases don’t behave as blackbodies or even graybodies! About 99% of Earth’s atmosphere is N2 & O2

Long Waves = small photons Short Waves = BIG PHOTONS Waves and Photons Electromagnetic radiation behaves as both waves and particles! Experiments show both kinds of behavior: Oscillating fields with troughs and crests (waves) Individual packets of energy (particles) Long Waves = small photons Short Waves = BIG PHOTONS

Energy is “Quantized” When radiation interacts with atoms and molecules, only certain “jumps” in energy are possible Electrons orbit at specific energy levels above an atomic nucleus Absorption of a photon of just the right energy can make them “jump up” to the next level Emission of a photon occurs when an electron “falls” down to a level below

Atomic Emission Big jumps take lots of energy, small jumps take less Big drops emit energetic photons (short wavelengths) Small drops emit less energetic photons (longer wavelengths) Most electron transitions in gases absorb/emit visible or UV light

Molecules and Photons Molecules are groups of atoms that share electrons (chemical bonds) Molecular transitions involve changes in vibration, rotation, bending, and stretching of chemical bonds Photons can interact with molecules to change states Transitions involve specific amounts of energy, so only certain wavelengths are active Molecular transitions typically absorb & emit in thermal infrared

PhET Simulation

Dancing Molecules and Heat Rays! AT606 Fall 2006 4/25/2017 Dancing Molecules and Heat Rays! Nearly all of the air is made of oxygen (O2) and nitrogen (N2) in which two atoms of the same element share electrons Infrared (heat) energy radiated up from the surface can be absorbed by these molecules, but not very well N O Diatomic molecules can vibrate back and forth like balls on a spring, but the ends are identical No electric dipole! CSU ATS Scott Denning

Dancing Molecules and Heat Rays! AT606 Fall 2006 4/25/2017 Dancing Molecules and Heat Rays! Carbon dioxide (CO2) and water vapor (H2O) are different! They have many more ways to vibrate and rotate, so they are very good at absorbing and emitting infrared (heat) radiation O C O O H H Molecules that have many ways to wiggle are called “Greenhouse” molecules CSU ATS Scott Denning

CO2 Vibrations O C O O C O O O C O C O 7.2 mm 15 mm 4.3 mm Resting or ground state CO2 Vibrations O C O No dipole … weak! 7.2 mm O C O 15 mm O O C Temporary electric dipole … strong! 4.3 mm O C O

H2O Vibrations Water molecules are “bent!” 2.7 mm 6.3 mm Water molecules are “bent!” This gives them a positively charged end (with the hydrogen) and a negatively charged end (with the oxygen) This “permanent dipole moment” allows H2O to absorb & emit photons without moving bonds

Line Broadening Exact energy difference between states absorbs & emits very specific wavelengths Photons collide with moving molecules – Doppler effect stretches or compresses Combinations (e.g., vibration + rotation) produce more lines Collisions among molecules can add or subtract energy too

AT606 Fall 2006 Molecular Absorbers 4/25/2017 Remember 99% of the molecules in the atmosphere are O2 and N2, almost no absorption or emission in thermal infrared Molecules that can form electric dipoles or have many ways to vibrate absorb in many wavelengths A single methane (CH4 ) molecule absorbs almost 100 times more thermal radiation than CO2 But there’s 500 x more CO2 CSU ATS Scott Denning

Atmospheric Absorption Visible radiation passes almost freely through Earth's atmosphere Earth's emitted thermal energy either fits through a narrow “window” or is absorbed by greenhouse gases and reradiated Complete absorption from 5-8 mm (H2O) and > 14 mm (CO2) Little absorption between about 8 m and 11 mm (“window”)

Optical “Thickness” 14.3 mm CO2 band 11 mm “window” In CO2 absorption bands, atmosphere is totally opaque to IR photons They get absorbed and re-emitted higher up It’s cold up there! Think about the Layer Model IR photons IR photons

View from Space Hot surface emits directly to space in window region Cold upper layers emit to space in optically thick regions Total emission much less than from sfc CO2 O3 H2O

Effect of Adding CO2 Optically thick regions are as cold as they can get But the thick regions get wider with added CO2 Rate of total emission (area under black curve) decreases less and less 1 ppm 10 ppm 1000 ppm 100 ppm wavelength (mm)

Total rate of cooling to space (area under spectral curve) Band Saturation As more CO2 gets added, it has less and less effect, but never goes to zero Total rate of cooling to space (area under spectral curve)

Logarithmic Effect due to band saturation “Radiative forcing” of CO2 is expressed as the number of Watts per square meter per doubling, not per unit change in concentration Temperature changes are degrees per doubling too (not degrees per ppm)

Absorption by CO2 Causes Warming No CO2 Absorption by CO2 Causes Warming Iout = 249 W m-2 1000 ppm CO2 As CO2 is added, big parts of the spectrum are emitted higher up where it’s colder This reduces the rate of total heat loss below solar gain The surface warms to compensate, emitting more from window regions, to re-establish equilibrium w/sun Iout = 223 W m-2 1000 ppm CO2 Iout = 249 W m-2 8.5 K Warmer!

Earth-Atmosphere Energy Balance Earth's surface absorbs the 51 units of shortwave and 96 more of longwave energy units from atmospheric gases and clouds. These 147 units gained by earth are due to shortwave and longwave greenhouse gas absorption and emittance. Earth's surface loses these 147 units through convection, evaporation, and radiation.