Mon Oct 20. Today: radiation and temperature (cont) sun-earth geometry energy balance >> conceptual model of climate change Tues:

Similar documents
Mon April 17 Announcements: bring calculator to class from now on (in-class activities, tests) HW#2 due Thursday

Lecture 5: Greenhouse Effect

Lecture 4: Global Energy Balance

Lecture 3: Global Energy Cycle

Lecture 4: Global Energy Balance. Global Energy Balance. Solar Flux and Flux Density. Blackbody Radiation Layer Model.

Lecture 5: Greenhouse Effect

Lecture # 04 January 27, 2010, Wednesday Energy & Radiation

Lecture 9: Climate Sensitivity and Feedback Mechanisms

Lecture 2 Global and Zonal-mean Energy Balance

Earth: the Goldilocks Planet

Lecture 4: Radiation Transfer

Lecture 6. Solar vs. terrestrial radiation and the bare rock climate model.

Temperature Scales

Spectrum of Radiation. Importance of Radiation Transfer. Radiation Intensity and Wavelength. Lecture 3: Atmospheric Radiative Transfer and Climate

ESS15 Lecture 7. The Greenhouse effect.

Lecture 3: Atmospheric Radiative Transfer and Climate

1. Weather and climate.

Electromagnetic Radiation. Radiation and the Planetary Energy Balance. Electromagnetic Spectrum of the Sun

Announcements: HW 1 in; HW 2 out (due: Thurs Oct 23) This week: Chap 2 and the science of systems

Atmospheric "greenhouse effect" - How the presence of an atmosphere makes Earth's surface warmer

Atmospheric "greenhouse effect" - How the presence of an atmosphere makes Earth's surface warmer

Earth s Energy Balance and the Atmosphere

Lecture 2: Global Energy Cycle

Understanding the Greenhouse Effect

PTYS 214 Spring Announcements. Midterm 3 next Thursday!

Radiation in climate models.

TOPIC # 7 The RADIATION LAWS

Wednesday, September 8, 2010 Infrared Trapping the Greenhouse Effect

Lecture 2: Global Energy Cycle

Solar Flux and Flux Density. Lecture 2: Global Energy Cycle. Solar Energy Incident On the Earth. Solar Flux Density Reaching Earth

Agronomy 406 World Climates January 11, 2018

Energy and the Earth AOSC 200 Tim Canty

- matter-energy interactions. - global radiation balance. Further Reading: Chapter 04 of the text book. Outline. - shortwave radiation balance

ATM S 111: Global Warming Solar Radiation. Jennifer Fletcher Day 2: June

Outline. Stock Flow and temperature. Earth as a black body. Equation models for earth s temperature. Balancing earth s energy flows.

Very Dynamic! Energy in the Earth s Atmosphere. How Does it Get Here? All Objects Radiate Energy!

Temperature AOSC 200 Tim Canty

2. What does a mercury barometer measure? Describe this device and explain how it physically works.

Friday 8 September, :00-4:00 Class#05

Radiative Balance and the Faint Young Sun Paradox

The Greenhouse Effect. Lan Ma

Lecture 4: Heat, and Radiation

ATS150 Global Climate Change Spring 2019 Candidate Questions for Exam #1

Climate Dynamics (PCC 587): Clouds and Feedbacks

Blackbody Radiation. A substance that absorbs all incident wavelengths completely is called a blackbody.

The Structure and Motion of the Atmosphere OCEA 101

Climate vs Weather J. J. Hack/A. Gettelman: June 2005

TOPIC # 6 The RADIATION LAWS

OBJECTIVES FOR TODAY S CLASS:

GARP 0102 Earth Radiation Balance (Part 1)

Today s AZ Daily Star has 2 interesting articles: one on our solar future & the other on an issue re: our state-mandated energy-efficiency plan

AST 105 Intro Astronomy The Solar System

The inputs and outputs of energy within the earth-atmosphere system that determines the net energy available for surface processes is the Energy

Let s make a simple climate model for Earth.

Chapter 2. Heating Earth's Surface & Atmosphere

P607 Climate and Energy (Dr. H. Coe)

Radiation Conduction Convection

COURSE CLIMATE SCIENCE A SHORT COURSE AT THE ROYAL INSTITUTION

Emission Temperature of Planets. Emission Temperature of Earth

8. Clouds and Climate

Earth: A Dynamic Planet A. Solar and terrestrial radiation

Course Outline CLIMATE SCIENCE A SHORT COURSE AT THE ROYAL INSTITUTION. 1. Current climate. 2. Changing climate. 3. Future climate change

Earth Systems Science Chapter 3

Climate Dynamics Simple Climate Models

Thursday, November 1st.

Planetary Atmospheres

ATMOS 5140 Lecture 1 Chapter 1

Radiative Equilibrium Models. Solar radiation reflected by the earth back to space. Solar radiation absorbed by the earth

- global radiative energy balance

Energy, Temperature, & Heat. Energy, Temperature, & Heat. Temperature Scales 1/17/11

Solar Radiation and Environmental Biophysics Geo 827, MSU Jiquan Chen Oct. 6, 2015

WRAP UP OF TOPIC #5... ELECTROMANGETIC RADAITAION & THE ELECTROMAGNETIC SPECTRUM

Lecture 10: Climate Sensitivity and Feedback

Which picture shows the larger flux of blue circles?

Equation for Global Warming

Atmospheric Radiation

Global Energy Balance: Greenhouse Effect

Lecture 1b: Global Energy Balance. Instructor: Prof. Johnny Luo

CLIMATE AND CLIMATE CHANGE MIDTERM EXAM ATM S 211 FEB 9TH 2012 V1

THE GREENHOUSE EFFECT

Composition, Structure and Energy. ATS 351 Lecture 2 September 14, 2009

Planetary Atmospheres

Climate Dynamics (PCC 587): Feedbacks & Clouds

Learning goals. Good absorbers are good emitters Albedo, and energy absorbed, changes equilibrium temperature

Energy and Radiation. GEOG/ENST 2331 Lecture 3 Ahrens: Chapter 2

Lecture 2: Light And Air

PTYS 214 Spring Announcements. Midterm 3 next Thursday! Midterms 4 and 5 more spread out

IB Physics Lesson Year Two: Standards from IB Subject Guide beginning 2016

ATMOS 5140 Lecture 7 Chapter 6

Chapter 10 Planetary Atmospheres: Earth and the Other Terrestrial Worlds. What is an atmosphere? About 10 km thick

Polar regions Temperate Regions Tropics High ( cirro ) 3-8 km 5-13 km 6-18 km Middle ( alto ) 2-4 km 2-7 km 2-8 km Low ( strato ) 0-2 km 0-2 km 0-2 km

Chapter 2: The global ledger of radiation and heat

SIT IN YOUR GROUP AREA TODAY!

9/5/16. Section 3-4: Radiation, Energy, Climate. Common Forms of Energy Transfer in Climate. Electromagnetic radiation.

Take away concepts. What is Energy? Solar Radiation Emission and Absorption. Energy: The ability to do work

WRAP UP OF TOPIC #6. Fire up your CLICKERS for some questions to solidify the concepts from the last few classes:

PTYS 214 Fall Announcements

2. Energy Balance. 1. All substances radiate unless their temperature is at absolute zero (0 K). Gases radiate at specific frequencies, while solids

HEATING THE ATMOSPHERE

Radiation and the atmosphere

Transcription:

Mon Oct 20 Announcements: bring calculator to class from now on > in-class activities > midterm and final Today: radiation and temperature (cont) sun-earth geometry energy balance >> conceptual model of climate change Tues: Wed: Thurs: T e (as opposed to T s ) and the greenhouse effect energy budget, balance at different levels atmospheric composition and structure greenhouse gas chemistry (why do these molecules absorb IR?) multiple roles of clouds in energy balance local energy balance

upcoming talks Monday 20 October: 3:30 310 ATG Prof Jim Tillman, UW Climate Mars: Viking Lander and next generation TUESDAY 21 October 12:30 ATG 310c, Weather discussion, Rick Steed FRIDAY 24 October: 3:30 14 OTB (Oceanography Teaching Bldg) Dr. Ralph Keeling Scripps Institute of Oceanography "Fate of anthropogenic CO2 and changing biogeochemistry of the oceans"

Radiation/Wavelength note 1. Electromagnetic radiation: - propagates through space - has a characteristic wavelength, for now just two types: SW: shortwave (mostly visible) LW: longwave SW and LW... not same meaning as radio!

Fig. 3-3 Sun Earth 0.3 2.0 Sun Fig. 3-8 Radiation vs Wavelength 5 30 Earth

Stefan-Boltzmann Law Hotter objects emit more total energy: Stephan-Boltzmann Law: E = σ T 4 σ = 5.67e-8 [a constant] 0.3 2.0 T is temp in Kelvin, the absolute temperature scale T(K) = T(C) + 273 5 30 Applies to an ideal material known as a "blackbody". (The emissions from most physical objects are close to this ideal.)

Kelvin (absolute) Temperature Scale T(K) = T(C) + 273 Reference Point water boils water freezes???? Celcius Scale (C) 100 0-273 Kelvin Scale (K) 373 273 0 What is the meaning of "absolute zero" temperature? Consider... Hotter objects emit more total energy Can there be a negative temperature on the Kelvin scale? What is the meaning of "temperature", anyway?

Kelvin/Boltzmann applications Stephan-Boltzmann Law: E = σ T 4 where σ = 5.67e-8, E is in W/m 2, and T is in Kelvin (K) Kelvin vs Celcius scale: T(K) = T(C) + 273 The average surface temperature of the Earth is 15C. Express this in degrees Kelvin. An object warms from 0C to 10C. What is the fractional increase in temperature? What is the fractional increase in emitted, radiative energy? If the Sun were to warm up by 10%, by how much would the solar constant increase? (i) fractional increase, (ii) absolute increase T SUN ~ 6000 K, T EARTH ~ 255 K What is the ratio of energy flux, E (W/m 2 ) from the Sun to that from the Earth?

Sun-Earth Geometry: flux on an angled surface overhead sun, tropics sun low in the sky, high latitudes

The earth intercepts the same amount of solar energy as flat disc of area πr 2 Sun-Earth Geometry: factor of 4 Define the solar constant, S 0 : the flux of solar energy passing through space at the Earth's orbital distance. S 0 = 1370 W/m 2 The earth emits LW radiation over the surface area of a sphere, 4πr 2 E IN = E OUT S 0 (1-A) πr 2 = σ T e 4 4πr 2

Energy balance E IN = E OUT S 0 (1-A) πr 2 = σ T e 4 4πr 2 Now divide both sides by the surface area of the Earth, 4πr 2. This will give the energy fluxes averaged over the Earth's surface. S 0 4 (1-A) = σ T e 4 In-class activity: S 0 = 1370 W/m 2 the average albedo of the Earth is 0.30 >> calculate E IN << E IN = 240 W/m 2 The average flux of solar energy absorbed by the Earth system. (averaged over entire surface, including day/night)

Tues Oct 21 Announcements: bring calculator to class from now on > in-class activities > midterm and final Today: conceptual model of climate change: forcing > feedback > response "effective radiating temperature", T e greenhouse effect (property of a planet's atmosphere) energy budget: needs to balance at every level [everything you need for HW#2 by end of today]

Energy Balance and Climate Change Energy balance equation (E is energy flux, W/m 2 ) E IN = energy absorbed by Earth E OUT energy emitted by Earth Energy Balance Theory of Climate Change if E OUT < E IN [imbalance] then T surface will go up until balance is restored

Energy Balance Theory of Climate Change T s = λ F F: forcing, change in energy balance (W/m 2 ) T s : response, change in surface temperature (K) λ: feedbacks, climate sensitivity {K/(W/m 2 )} What are the characteristics of each of these terms? F: imposed changes on the climate system; increasing GHGs, changed surface albedo, increasing aerosols T s : λ: climate response in terms of GAAST; can be measured and predicted for the past (test of understanding) involves full complexity of the climate system; requires climate models; involves feedbacks, mainly (i) water vapor, (ii) ice-albedo, (iii) clouds

Energy Balance Theory of Climate Change T s = λ F F: forcing, change in energy balance (W/m 2 ) T s : response, change in surface temperature (K) λ: feedbacks, climate sensitivity {K/(W/m 2 )} There are two important terms left out of the above equation. What are they? Response time of the climate system Natural variability of the climate system (We will incorporate these later.)

Effective Radiating Temperature -1 S 0 4 E IN = E OUT (1-A) = σ T e 4 where S 0 is the solar constant A is the planetary albedo σ is the Stephan-Boltzmann constant and T e is the "effective radiating temperature" Given values for S 0, A, and σ, we can solve for T e : T e 4 = S 0 4σ (1-A) T [ ] 0.25 e = (1-A) S 0 4σ

Effective Radiative Temperature -2 T [ ] 0.25 e = (1-A) S 0 4σ σ = 5.67e-8 [universal constant] For Earth: S 0 = 1370 W/m 2 A = 0.30 Calculate T e??? T e = 255 K (or -18 C) "The Earth radiates as if it were a blackbody at 255 K." but... the Earth's surface temperature (T s ) is 288 K (or +15 C).???

Greenhouse Effect If the Earth had no atmosphere (and still had an albedo of 0.30), its surface temperature would be 255 K. The atmosphere acts like a blanket, trapping heat near the surface and keeping it much warmer than it would otherwise be. The magnitude of this "greenhouse effect" ( T g ) is: T g = T s -T e = 288 K - 255 K T g = 33 K T g is a property of the atmosphere. (Should really be called "the atmosphere effect".)

Text Box on page 43 What are the assumptions of this model? Atmosphere is a separate "layer" with temperature T e. Atmosphere does not absorb any SW radiation. Atmosphere completely absorbs the LW radiation emitted by the surface.

Text Box on page 43 Good: Atmosphere acts like a blanket. Simple numerical model of the greenhouse effect. BAD: Calculation is not very accurate ( T g = 48 K) Includes a misleading, incorrect equation: 1/4 T s = 2 T e

Venus (runaway greenhouse) Sister planets In fact, you cannot "predict" T s from knowledge of T e. T e is a function of S 0 and A T s = T e + T g where, T g is a property of the atmosphere of a planet Earth ("just right") Mars (virtually no greenhouse) Note: formula from the Text Box on page 43 gives wildly inaccurate estimates of greenhouse effect for Venus and Mars.

Energy Budget: TOA and surface Top-of-Atmosphere budget: IN = OUT Surface budget: IN = OUT

Energy Budget: atmosphere Atmosphere budget: IN = OUT

Vertical structure of the atmosphere Pressure: the weight of air overhead (e.g. psi or lbs/in 2 ) Note log scale on pressure graph. a. At what height are you above 99% of the atmospheric mass? b. What fraction of atmospheric mass is in the Troposphere? a. 30 km b. 90% c. 6 km Lapse rate: The rate at which temperature changes with height in the atmosphere. A measure of vertical stability. c. What height corresponds to T e?

Satellite View of Energy Budget visible satellite infrared satellite

Wed Oct 22 Announcements: HW#2 due Thursday at beginning of class Monday's record rain Today: vertical structure, "lapse rate" atmospheric composition greenhouse gas absorption - how does it work? dual role of clouds Speaking of atoms...

Vertical structure of the atmosphere Pressure: the weight of air overhead (e.g. psi or lbs/in 2 ) a. At sea level, P = 15 psi. Why don't we feel it? b. At what depth underwater is pressure doubled? c. 6 km Lapse rate: The rate at which temperature changes with height in the atmosphere. A measure of vertical stability. c. What height corresponds to T e?

Lapse rate and convection Lapse rate: The rate at which temperature changes with height in the atmosphere. A measure of vertical stability. Stable: Warm fluid on top of cold fluid. Unstable: Warm fluid below cold fluid. Box Fig. 3-3

A dialectic on atmospheric vertical structure KKC Fig 3-9 Weather (clouds, rain) happens in the Troposphere because the Troposphere is unstable. Why is the troposphere unstable? Because temperature decreases with height. Yes, but why does temperature decrease with height? Because it is heated from below. Yes, but how does it come about that it is heated from below? Because the atmosphere is mostly transparent to solar (or, SW) radiation.

SW spectral absorption by the atmosphere most (non-reflected) SW radiation passes through the atmosphere

spectral absorption by the atmosphere LW most LW radiation emitted by the surface is absorbed by the atmosphere Fig 3-13 terrestrial (LW) radiation

Atmospheric constituents main gases (O 2, N 2, Ar are 99.9% of dry volume of atmosphere) variable gas (water vapor) trace gases (CO 2, O 2, CFC's, SO 2, etc, etc, etc) particles (dust, seasalt, sulfate, soot, organics)

Greenhouse gases ppmv, parts per million by volume: molecules of trace substance per million molecules of air

GHG absorption

hi-lo cloud: Bad Figure! σ 250 4 = 221 W/m 2 σ 280 4 = 349 W/m 2 σ 288 4 = 390 W/m 2 250 K 280 K 288 K

upcoming talks FRIDAY 24 October: 3:30 14 OTB (Oceanography Teaching Bldg) Dr. Ralph Keeling Scripps Institute of Oceanography "Fate of anthropogenic CO2 and changing biogeochemistry of the oceans"

Thur Oct 23 Announcements: HW #2 due today Readings for next week are on the web Modeling chapter from new edition of book Lorius et al. article on ice-ages and climate sensitivity midterm next Friday paper #1 due next Friday Today: multiple role of clouds in energy balance local energy balance, diurnal effects Tomorrow (Friday): guidance on papers review/questions supplementary topics

Heat-trapping by clouds calculate the heat-trapping (W/m2) by the cloud Cloud: E OUT = σ T 4 = 5.67e-8*270 4 = 301 W/m 2 301 W/m 2 T top =270 K Cloud 89 W/m 2 "trapped" Surface: within Troposphere E OUT = σ T 4 = 5.67e-8*288 4 = 390 W/m 2 390 W/m 2 Heat-trapping = 390-301 = 89 W/m 2 T surface = 288 K What assumptions underlie this calculation? All LW radiation is absorbed by cloud. Cloud emits according to cloud-top temperature.

Greenhouse role of clouds LW The previous slide demonstrates that clouds are a major participant in the Earth's greenhouse effect. warming SW But... We know from previous lectures that clouds are a major player in controlling Earth's albedo. cooling net Question... What is the net effect of a cloud on the energy balance????

Local Energy Balance calculate E IN, E OUT, and net energy effect for each cloud type High thin cloud T=250 K A=0.20 E IN = S 0 /4(1-A) = 1370/4*0.4 = 137 W/m 2 E IN = S 0 /4(1-A) = 1370/4*0.8 = 274 W/m 2 E OUT = σ T 4 = 5.67e-8*280 4 = 349 W/m 2 E OUT = σ T 4 = 5.67e-8*250 4 = 221 W/m 2 E NET = E IN -E OUT = 137-349 = -212 W/m 2 E NET = E IN -E OUT = 274-221 T=280 K A=0.60 = +53 W/m 2 Low, thick cloud

Multiple roles of clouds in the energy budget SW: Clouds are the major player in the Earth's albedo LW: Clouds are a major player in heat-trapping (greenhouse effect) high clouds: modest albedo (small SW effect) lots of "heat-trapping" complete IR absorption cold, so have low IR emission low clouds: high albedo (big SW effect) modest "heat-trapping" complete IR absorption almost as warm as the surface, so emit almost as much IR upwards

High vs Low Clouds graphic

Home Weather record Where on these plots do you see the SW effect of clouds? Where do you see the LW effect of clouds? Sunlight Outdoor Temperature Time