Energy Inputs and Outputs

Size: px
Start display at page:

Download "Energy Inputs and Outputs"

Transcription

1 Energy Inputs and Outputs Sun Earth ultravilet visible infrared Bth Sun and Earth behave as blackbdies (absrb 100% incident radiatin; emit radiatin at all wavelengths in all directins) Earth receives energy frm sun in the frm f shrtwave radiatin with peak in the visible (λ = μm) Earth emits energy t space in the frm f lngwave radiatin in the infrared (λ = 5-20 μm) functin f Earth s temperature SOLAR RADIATION SPECTRUM: blackbdy at 5800 K Ttal Slar Radiatin Received By Earth Slar cnstant fr Earth: 1368 W m -2 (Nte: 1 W = 1 J s -1 ) Slar radiatin received tp f atmsphere unit area f sphere = (1368) x (π r e2 )/( π r e2 ) = 32 W m -2 1

2 A N-Atmsphere Earth Assume 30% f incming slar energy is reflected by surface (albed f surface = 0.3) Energy absrbed by surface = 70% f 32 W m -2 = 239. W m -2 Balanced by energy emitted by surface Stefan-Bltzmann law: Energy emitted = σ T ;(σ=5.67 x 10-8 W m -2 K - ) 239. W m -2 = σ T T = 255 K (-18 C) much less than average temperature f 288 K (15 C) What is missing? Absrptin f terrestrial radiatin by the atmsphere TERRESTRIAL RADIATION SPECTRUM FROM SPACE: cmpsite f blackbdy radiatin spectra fr different T Scene ver Niger valley, N Africa (nn) NORMAL VIBRATIONAL MODES OF CO 2 Greenhuse gases = gases with vib-rt absrptin features at 5-50 μm Majr greenhuse gases: H 2 O, CO 2, CH, O 3, N 2 O, CFCs, Nt greenhuse gases: N 2, O 2, Ar, Mlecules that can acquire a charge assymetry be stretching r flexing are greenhuse gases. 2

3 An Idealized Earth+Atmsphere W m W m W m -2 (1-f)σ T σ T absrbed = f σ T f=atmspheric absrptin efficiency Slar radiatin at surface = 70% f 32 W m -2 = 239. W m -2 Infrared flux frm surface = σ T Absrptin f infrared flux by atmsphere = f σ T Kirchhff s law: efficiency f absrptin = efficiency f emissin IR flux frm atmspheric layer = f σ T 1 (up and dwn) IR flux t space = f σ T 1 + (1-f)σ T Radiatin Balance Equatins W m W m -2 (1-f)σ T fσ T 1 absrbed = f σ T 239. W m -2 σ T Balance at tp f atmsphere f σ T 1 + (1-f) σ T = 239. Balance fr atmspheric layer f σ T 1 + f σ T 1 = f σ T Slve fr T and T 1 The Greenhuse Effect W m W m -2 (1-f)σ T fσ T 1 absrbed = f σ T 239. W m -2 σ T Fr f=0.77, T =288 K and T 1 =22 K (33 K warmer than the n-atmsphere case) As f increases, T and T 1 increase Greenhuse gases gases that affect f (absrptin efficiency f atms.) Earth has a natural greenhuse effect; human activities enhance effect 3

4 TERRESTRIAL RADIATION SPECTRUM FROM SPACE: cmpsite f blackbdy radiatin spectra fr different T Scene ver Niger valley, N Africa trpsphere surface tp f stratsphere Hw des the additin f a greenhuse gas warm the earth? 1. Initial state Example f a GG absrbing at 11 μm 2. Add t atmsphere a GG absrbing at 11 μm; emissin at 11 μm decreases (we dn t see the surface anymre at that λ, but the atmsphere) 3. At new steady state, ttal emissin integrated ver all λ s must be cnserved Emissin at ther λ s must increase The Earth must heat! 3. Cncept f Radiative Frcing Glbal mean radiative frcing f the climate system relative t 1750 AD Purpse: t quantify a radiative perturbatin assciated with an increase in a greenhuse gas IPCC, 2007

5 Aersl direct and indirect effects Figure 2.10 IPCC, 2007 Radiative Frcing and Temperature Change Increasing the abundance f a greenhuse gas by Δm crrespnds t an increase in Δf f the absrptin efficiency, and an initial decrease in IR radiatin emitted t space (by ΔF) Respnse f system t energy imbalance: T and T 1 increase may cause ther greenhuse gases t change T and T 1 may increase r decrease depending n internal climate feedbacks Δf ΔT etc Ultimately, the system gets back in balance Radiative frcing is nly a measure f initial change in utging terrestrial radiatin Climate mdels (GCMs) indicate ΔT surface = λ ΔF where λ (climate sensitivity parameter) ranges frm 0.3 t 1. K m 2 W -1 depending n the GCM Psitive Feedback Cause enhance Effect Effect enhances cause increase effect bm!!! Ex: Water vapr feedback Ex: warmer melting land ice lwer albed further warming 5

6 Negative Feedback Negative feedback Cause suppress Effect Effect suppresses cause decrease effect self-regulatin Example: warmer mre cluds higher albed cling effect (negative feedback) Feedbacks water vapr feedback: psitive. CO 2 Greenhuse effect Temperature Greenhuse effect Water vapr ice-albed feedback: psitive r negative?. clud feedbacks: psitive r negative? ptentially large (cluds can reflect slar radiatin r absrb IR radiatin depending n their height, thickness and micrphysical prperties) Largest uncertainty in current estimates f climate change. land surface feedback: psitive r negative? (surface albed affect, CO 2 fertilizatin, sil misture) GLOBAL WARMING POTENTIAL (GWP): fundatin fr climate plicy The GWP measures the integrated radiative frcing ver a time hrizn Δt frm the injectin f 1 kg f a species X at time t, relative t CO 2 : GWP = Gas t t t +Δt t +Δt ΔF ΔF 1 kg X 1 kg CO2 dt dt Lifetime (years) GWP fr time hrizn 20 years 100 years 500 years CO 2 ~ CH N 2 O CFC-12 (CF 2 Cl 2 ) HFC-13a (CH 2 FCF 3 ) SF

Environmental Modelling (ENGO 583/ENEN 635)

Environmental Modelling (ENGO 583/ENEN 635) Suggested citatin: Hassan, Q.K. 2018. Lecture nte n: Mdelling the effect f greenhuse gases n temperature, In Envirnmental Mdelling, Calgary, AB, Canada. Envirnmental Mdelling (ENGO 583/ENEN 635) Lecture

More information

Chapter 11: Atmosphere

Chapter 11: Atmosphere Chapter 11: Atmsphere Sectin 1: Atmspheric Basics Objectives 1. Describe the cmpsitin f the atmsphere. 2. Cmpare and cntrast the varius layers f the atmsphere. 3. Identify three methds f transferring energy

More information

Phy 212: General Physics II 1 Chapter 18 Worksheet 3/20/2008

Phy 212: General Physics II 1 Chapter 18 Worksheet 3/20/2008 Phy 1: General Physics II 1 hapter 18 rksheet 3/0/008 Thermal Expansin: 1. A wedding ring cmpsed f pure gld (inner diameter = 1.5 x 10 - m) is placed n a persn s finger (diameter = 1.5 x 10 - m). Bth the

More information

11. DUAL NATURE OF RADIATION AND MATTER

11. DUAL NATURE OF RADIATION AND MATTER 11. DUAL NATURE OF RADIATION AND MATTER Very shrt answer and shrt answer questins 1. Define wrk functin f a metal? The minimum energy required fr an electrn t escape frm the metal surface is called the

More information

Electromagnetic Radiation

Electromagnetic Radiation CLASSICALLY -- ELECTROMAGNETIC RADIATION Maxwell (1865) Electrmagnetic Radiatin http://apd.nasa.gv/apd/astrpix.html Classically, an electrmagnetic wave can be viewed as a self-sustaining wave f electric

More information

Dispersion Ref Feynman Vol-I, Ch-31

Dispersion Ref Feynman Vol-I, Ch-31 Dispersin Ref Feynman Vl-I, Ch-31 n () = 1 + q N q /m 2 2 2 0 i ( b/m) We have learned that the index f refractin is nt just a simple number, but a quantity that varies with the frequency f the light.

More information

Chem 115 POGIL Worksheet - Week 8 Thermochemistry (Continued), Electromagnetic Radiation, and Line Spectra

Chem 115 POGIL Worksheet - Week 8 Thermochemistry (Continued), Electromagnetic Radiation, and Line Spectra Chem 115 POGIL Wrksheet - Week 8 Thermchemistry (Cntinued), Electrmagnetic Radiatin, and Line Spectra Why? As we saw last week, enthalpy and internal energy are state functins, which means that the sum

More information

Climate Application: Aerosol Direct Radiative Forcing. Alex Kuwano SIOG 135/236 Spring 2018

Climate Application: Aerosol Direct Radiative Forcing. Alex Kuwano SIOG 135/236 Spring 2018 Climate Applicatin: Aersl Direct Radiative Frcing Alex Kuwan SIOG 135/236 Spring 2018 Backgrund Infrmatin SW shrtwave LW - lngwave Figure 2. Figure 1. Backgrund Infrmatin AOD Aersl ptical depth τ = z kabs

More information

Let s make a simple climate model for Earth.

Let s make a simple climate model for Earth. Let s make a simple climate model for Earth. What is the energy balance of the Earth? How is it controlled? ó How is it affected by humans? Energy balance (radiant energy) Greenhouse Effect (absorption

More information

Climate Change: some basic physical concepts and simple models. David Andrews

Climate Change: some basic physical concepts and simple models. David Andrews Climate Change: some basic physical concepts and simple models David Andrews 1 Some of you have used my textbook An Introduction to Atmospheric Physics (IAP) I am now preparing a 2 nd edition. The main

More information

Outline. 13./ 16. March Introduction. Photochemistry. Ozone chemistry Chapman model Catalytic cycles

Outline. 13./ 16. March Introduction. Photochemistry. Ozone chemistry Chapman model Catalytic cycles Institute f Applied Physics University f Bern 13./ 16. March 2012 Outline The rle f Ozne hle: what causes what? Culd it be that ClO destrys O 3? Atmsphere as a chemical vessel The can be thught f as a

More information

UNIT 13: WEATHER AND CLIMATE

UNIT 13: WEATHER AND CLIMATE ABSTRACT This unit cvers the tpics f meterlgy and basic weather predictin, factrs impacting weather, and factrs impacting climate. UNIT 13: WEATHER AND CLIMATE STUDENT NOTES PACKET STUDENT NAME: Unit 13:

More information

Radiative Balance and the Faint Young Sun Paradox

Radiative Balance and the Faint Young Sun Paradox Radiative Balance and the Faint Young Sun Paradox Solar Irradiance Inverse Square Law Faint Young Sun Early Atmosphere Earth, Water, and Life 1. Water - essential medium for life. 2. Water - essential

More information

Chapter 23 Electromagnetic Waves Lecture 14

Chapter 23 Electromagnetic Waves Lecture 14 Chapter 23 Electrmagnetic Waves Lecture 14 23.1 The Discvery f Electrmagnetic Waves 23.2 Prperties f Electrmagnetic Waves 23.3 Electrmagnetic Waves Carry Energy and Mmentum 23.4 Types f Electrmagnetic

More information

To get you thinking...

To get you thinking... T get yu thinking... 1.) What is an element? Give at least 4 examples f elements. 2.) What is the atmic number f hydrgen? What des a neutral hydrgen atm cnsist f? Describe its "mtin". 3.) Hw des an atm

More information

MANIPAL INSTITUTE OF TECHNOLOGY

MANIPAL INSTITUTE OF TECHNOLOGY MANIPAL INSTITUTE OF TECHNOLOGY MANIPAL UNIVERSITY, MANIPAL SECOND SEMESTER B.Tech. END-SEMESTER EXAMINATION - MAY 013 SUBJECT: ENGINEERING PHYSICS (PHY101/10) Time: 3 Hrs. Max. Marks: 50 Nte: Answer any

More information

Journal of Molecular EvOlution by Springer-Verlag. 1979

Journal of Molecular EvOlution by Springer-Verlag. 1979 0022-28447900140057~ 01.60 J. Ml. Evl. 14, 57--64 (1979) Jurnal f Mlecular EvOlutin by Springer-Verlag. 1979 Slar Radiatin Incident n the Martian Surface W.R. Kuhn and S.K. Atreya Department f Atmspheric

More information

Short notes for Heat transfer

Short notes for Heat transfer Furier s Law f Heat Cnductin Shrt ntes fr Heat transfer Q = Heat transfer in given directin. A = Crss-sectinal area perpendicular t heat flw directin. dt = Temperature difference between tw ends f a blck

More information

PTYS 214 Spring Announcements. Midterm 3 next Thursday!

PTYS 214 Spring Announcements. Midterm 3 next Thursday! PTYS 214 Spring 2018 Announcements Midterm 3 next Thursday! 1 Previously Habitable Zone Energy Balance Emission Temperature Greenhouse Effect Vibration/rotation bands 2 Recap: Greenhouse gases In order

More information

d sinθ = mλ Interference and diffraction double slit or diffraction grating d sinθ = mλ d sinθ is the path difference x (small angle approximation)

d sinθ = mλ Interference and diffraction double slit or diffraction grating d sinθ = mλ d sinθ is the path difference x (small angle approximation) Wave Optics Wave prperties f light The clrs in a rainbw are ROY G. BIV (Red, range, yellw, green, blue, indig, vilet). White light is a cmbinatin f all clrs Black is the absence f light Wavelength determines

More information

Lecture 2 Global and Zonal-mean Energy Balance

Lecture 2 Global and Zonal-mean Energy Balance Lecture 2 Global and Zonal-mean Energy Balance A zero-dimensional view of the planet s energy balance RADIATIVE BALANCE Roughly 70% of the radiation received from the Sun at the top of Earth s atmosphere

More information

Chapter 17: Thermodynamics: Spontaneous and Nonspontaneous Reactions and Processes

Chapter 17: Thermodynamics: Spontaneous and Nonspontaneous Reactions and Processes Chapter 17: hermdynamics: Spntaneus and Nnspntaneus Reactins and Prcesses Learning Objectives 17.1: Spntaneus Prcesses Cmparing and Cntrasting the hree Laws f hermdynamics (1 st Law: Chap. 5; 2 nd & 3

More information

AP CHEMISTRY CHAPTER 6 NOTES THERMOCHEMISTRY

AP CHEMISTRY CHAPTER 6 NOTES THERMOCHEMISTRY AP CHEMISTRY CHAPTER 6 NOTES THERMOCHEMISTRY Energy- the capacity t d wrk r t prduce heat 1 st Law f Thermdynamics: Law f Cnservatin f Energy- energy can be cnverted frm ne frm t anther but it can be neither

More information

General Chemistry II, Unit I: Study Guide (part I)

General Chemistry II, Unit I: Study Guide (part I) 1 General Chemistry II, Unit I: Study Guide (part I) CDS Chapter 14: Physical Prperties f Gases Observatin 1: Pressure- Vlume Measurements n Gases The spring f air is measured as pressure, defined as the

More information

Monday 9 September, :30-11:30 Class#03

Monday 9 September, :30-11:30 Class#03 Monday 9 September, 2013 10:30-11:30 Class#03 Topics for the hour Solar zenith angle & relationship to albedo Blackbody spectra Stefan-Boltzman Relationship Layer model of atmosphere OLR, Outgoing longwave

More information

CHEM 103: Chemistry in Context

CHEM 103: Chemistry in Context CHEM 103: Chemistry in Context Unit 4.2 Atmospheric Chemistry: the chemistry of global climate change Reading: Chapter 3 Unit 4.2: Chemistry Behind Global Climate Change Solar energy balance Earth s surface

More information

Earth: the Goldilocks Planet

Earth: the Goldilocks Planet Earth: the Goldilocks Planet Not too hot (460 C) Fig. 3-1 Not too cold (-55 C) Wave properties: Wavelength, velocity, and? Fig. 3-2 Reviewing units: Wavelength = distance (meters or nanometers, etc.) Velocity

More information

BOUNDED UNCERTAINTY AND CLIMATE CHANGE ECONOMICS. Christopher Costello, Andrew Solow, Michael Neubert, and Stephen Polasky

BOUNDED UNCERTAINTY AND CLIMATE CHANGE ECONOMICS. Christopher Costello, Andrew Solow, Michael Neubert, and Stephen Polasky BOUNDED UNCERTAINTY AND CLIMATE CHANGE ECONOMICS Christpher Cstell, Andrew Slw, Michael Neubert, and Stephen Plasky Intrductin The central questin in the ecnmic analysis f climate change plicy cncerns

More information

Physics 262/266. George Mason University. Prof. Paul So

Physics 262/266. George Mason University. Prof. Paul So Physics 262/266 Gerge Masn University Prf. Paul S PHYS 262/266 Annuncements WELCOME TO A NEW SEMESTER! Curse Website - http://cmplex.gmu.edu/www-phys/phys262 - http://cmplex.gmu.edu/www-phys/phys266 Recitatins

More information

An interactive cirrus cloud radiative parameterization

An interactive cirrus cloud radiative parameterization JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 104, NO. D8, PAGES 9501-9515, APRIL 27, 1999 An interactive cirrus clud radiative parameterizatin fr glbal climate mdels Everette Jseph and Wei-Chyung Wang Atmspheric

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 4: Mdel checing fr ODE mdels In Petre Department f IT, Åb Aademi http://www.users.ab.fi/ipetre/cmpmd/ Cntent Stichimetric matrix Calculating the mass cnservatin relatins

More information

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

9/5/16. Section 3-4: Radiation, Energy, Climate. Common Forms of Energy Transfer in Climate. Electromagnetic radiation. Section 3-4: Radiation, Energy, Climate Learning outcomes types of energy important to the climate system Earth energy balance (top of atm., surface) greenhouse effect natural and anthropogenic forcings

More information

Torben Königk Rossby Centre/ SMHI

Torben Königk Rossby Centre/ SMHI Fundamentals of Climate Modelling Torben Königk Rossby Centre/ SMHI Outline Introduction Why do we need models? Basic processes Radiation Atmospheric/Oceanic circulation Model basics Resolution Parameterizations

More information

Entropy, Free Energy, and Equilibrium

Entropy, Free Energy, and Equilibrium Nv. 26 Chapter 19 Chemical Thermdynamics Entrpy, Free Energy, and Equilibrium Nv. 26 Spntaneus Physical and Chemical Prcesses Thermdynamics: cncerned with the questin: can a reactin ccur? A waterfall runs

More information

Chapter 9: Quantization of Light

Chapter 9: Quantization of Light Chapter 9: Quantizatin Light 9.1 Planck s Quantum Thery 9.1.1 Distinguish between Planck s quantum thery and classical thery energy The undatin the Planck s quantum thery is a thery black bdy radiatin.

More information

Thermodynamics and Equilibrium

Thermodynamics and Equilibrium Thermdynamics and Equilibrium Thermdynamics Thermdynamics is the study f the relatinship between heat and ther frms f energy in a chemical r physical prcess. We intrduced the thermdynamic prperty f enthalpy,

More information

Chapter 17 Free Energy and Thermodynamics

Chapter 17 Free Energy and Thermodynamics Chemistry: A Mlecular Apprach, 1 st Ed. Nivald Tr Chapter 17 Free Energy and Thermdynamics Ry Kennedy Massachusetts Bay Cmmunity Cllege Wellesley Hills, MA 2008, Prentice Hall First Law f Thermdynamics

More information

Recitation 06. n total = P total V/RT = (0.425 atm * 10.5 L) / ( L atm mol -1 K -1 * 338 K) = mol

Recitation 06. n total = P total V/RT = (0.425 atm * 10.5 L) / ( L atm mol -1 K -1 * 338 K) = mol Recitatin 06 Mixture f Ideal Gases 1. Chapter 5: Exercise: 69 The partial pressure f CH 4 (g) is 0.175 atm and that f O 2 (g) is 0.250 atm in a mixture f the tw gases. a. What is the mle fractin f each

More information

**DO NOT ONLY RELY ON THIS STUDY GUIDE!!!**

**DO NOT ONLY RELY ON THIS STUDY GUIDE!!!** Tpics lists: UV-Vis Absrbance Spectrscpy Lab & ChemActivity 3-6 (nly thrugh 4) I. UV-Vis Absrbance Spectrscpy Lab Beer s law Relates cncentratin f a chemical species in a slutin and the absrbance f that

More information

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review

CHEM Thermodynamics. Change in Gibbs Free Energy, G. Review. Gibbs Free Energy, G. Review Review Accrding t the nd law f Thermdynamics, a prcess is spntaneus if S universe = S system + S surrundings > 0 Even thugh S system

More information

Essential Questions. Unit One: The Atmosphere Layers of the atmosphere Standards

Essential Questions. Unit One: The Atmosphere Layers of the atmosphere Standards Essential Questins Unit One: The Atmsphere Layers f the atmsphere Standards Curse Title: Meterlgy Curse Descriptin: Weather and Climate is the scientific study f atmspheric prcesses and patterns, and their

More information

ECE 546 Lecture 02 Review of Electromagnetics

ECE 546 Lecture 02 Review of Electromagnetics C 546 Lecture 0 Review f lectrmagnetics Spring 018 Jse. Schutt-Aine lectrical & Cmputer ngineering University f Illinis jesa@illinis.edu C 546 Jse Schutt Aine 1 Printed Circuit Bard C 546 Jse Schutt Aine

More information

Work, Energy, and Power

Work, Energy, and Power rk, Energy, and Pwer Physics 1 There are many different TYPES f Energy. Energy is expressed in JOULES (J 419J 4.19 1 calrie Energy can be expressed mre specifically by using the term ORK( rk The Scalar

More information

Global Energy Balance: Greenhouse Effect

Global Energy Balance: Greenhouse Effect Global Energy Balance: Greenhouse Effect Atmospheric Composition & Structure Physical Causes of Greenhouse Effects Chapter 3: 44 48. Atmospheric Composition Why does water vapor vary so much? Saturation

More information

1. Weather and climate.

1. Weather and climate. Lecture 31. Introduction to climate and climate change. Part 1. Objectives: 1. Weather and climate. 2. Earth s radiation budget. 3. Clouds and radiation field. Readings: Turco: p. 320-349; Brimblecombe:

More information

GASES. PV = nrt N 2 CH 4 CO 2 O 2 HCN N 2 O NO 2. Pressure & Boyle s Law Temperature & Charles s Law Avogadro s Law IDEAL GAS LAW

GASES. PV = nrt N 2 CH 4 CO 2 O 2 HCN N 2 O NO 2. Pressure & Boyle s Law Temperature & Charles s Law Avogadro s Law IDEAL GAS LAW GASES Pressure & Byle s Law Temperature & Charles s Law Avgadr s Law IDEAL GAS LAW PV = nrt N 2 CH 4 CO 2 O 2 HCN N 2 O NO 2 Earth s atmsphere: 78% N 2 21% O 2 sme Ar, CO 2 Sme Cmmn Gasses Frmula Name

More information

Types of Energy COMMON MISCONCEPTIONS CHEMICAL REACTIONS INVOLVE ENERGY

Types of Energy COMMON MISCONCEPTIONS CHEMICAL REACTIONS INVOLVE ENERGY CHEMICAL REACTIONS INVOLVE ENERGY The study energy and its transrmatins is knwn as thermdynamics. The discussin thermdynamics invlve the cncepts energy, wrk, and heat. Types Energy Ptential energy is stred

More information

The Solar Interior - The Standard Model. Topics to be covered: o Solar interior. Radiative Zone. Convective Zone

The Solar Interior - The Standard Model. Topics to be covered: o Solar interior. Radiative Zone. Convective Zone Lecture 1 - The Slar Interir Tpics t be cvered: Slar interir Cre Radiative zne Cnvectin zne Lecture 1 - The Slar Interir The Slar Interir - The Standard Mdel Cre Energy generated by nuclear fusin (the

More information

Lecture 9: Climate Sensitivity and Feedback Mechanisms

Lecture 9: Climate Sensitivity and Feedback Mechanisms Lecture 9: Climate Sensitivity and Feedback Mechanisms Basic radiative feedbacks (Plank, Water Vapor, Lapse-Rate Feedbacks) Ice albedo & Vegetation-Climate feedback Cloud feedback Biogeochemical feedbacks

More information

Lecture 5: Greenhouse Effect

Lecture 5: Greenhouse Effect /30/2018 Lecture 5: Greenhouse Effect Global Energy Balance S/ * (1-A) terrestrial radiation cooling Solar radiation warming T S Global Temperature atmosphere Wien s Law Shortwave and Longwave Radiation

More information

Differentiation Applications 1: Related Rates

Differentiation Applications 1: Related Rates Differentiatin Applicatins 1: Related Rates 151 Differentiatin Applicatins 1: Related Rates Mdel 1: Sliding Ladder 10 ladder y 10 ladder 10 ladder A 10 ft ladder is leaning against a wall when the bttm

More information

Lecture 5: Greenhouse Effect

Lecture 5: Greenhouse Effect Lecture 5: Greenhouse Effect S/4 * (1-A) T A 4 T S 4 T A 4 Wien s Law Shortwave and Longwave Radiation Selected Absorption Greenhouse Effect Global Energy Balance terrestrial radiation cooling Solar radiation

More information

A) 0.77 N B) 0.24 N C) 0.63 N D) 0.31 N E) 0.86 N. v = ω k = 80 = 32 m/s. Ans: (32) 2 = 0.77 N

A) 0.77 N B) 0.24 N C) 0.63 N D) 0.31 N E) 0.86 N. v = ω k = 80 = 32 m/s. Ans: (32) 2 = 0.77 N Q1. A transverse sinusidal wave travelling n a string is given by: y (x,t) = 0.20 sin (2.5 x 80 t) (SI units). The length f the string is 2.0 m and its mass is 1.5 g. What is the magnitude f the tensin

More information

[ ] [ ] [ ] [ ] [ ] [ J] dt x x hard to solve in general solve it numerically. If there is no convection. is in the absence of reaction n

[ ] [ ] [ ] [ ] [ ] [ J] dt x x hard to solve in general solve it numerically. If there is no convection. is in the absence of reaction n .3 The material balance equatin Net change f [J] due t diffusin, cnvectin, and reactin [ ] [ ] [ ] d J J J n = D v k [ J ] fr n - th reactin dt x x hard t slve in general slve it numerically If there is

More information

GOAL... ability to predict

GOAL... ability to predict THERMODYNAMICS Chapter 18, 11.5 Study f changes in energy and transfers f energy (system < = > surrundings) that accmpany chemical and physical prcesses. GOAL............................. ability t predict

More information

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site.

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site. Find this material useful? Yu can help ur team t keep this site up and bring yu even mre cntent cnsider dnating via the link n ur site. Still having truble understanding the material? Check ut ur Tutring

More information

Radiation Conduction Convection

Radiation Conduction Convection Lecture Ch. 3a Types of transfers Radiative transfer and quantum mechanics Kirchoff s law (for gases) Blackbody radiation (simplification for planet/star) Planck s radiation law (fundamental behavior)

More information

Chem 75 February 16, 2017 Exam 2 Solutions

Chem 75 February 16, 2017 Exam 2 Solutions 1. (6 + 6 pints) Tw quick questins: (a) The Handbk f Chemistry and Physics tells us, crrectly, that CCl 4 bils nrmally at 76.7 C, but its mlar enthalpy f vaprizatin is listed in ne place as 34.6 kj ml

More information

Name: Period: Date: ATOMIC STRUCTURE NOTES ADVANCED CHEMISTRY

Name: Period: Date: ATOMIC STRUCTURE NOTES ADVANCED CHEMISTRY Name: Perid: Date: ATOMIC STRUCTURE NOTES ADVANCED CHEMISTRY Directins: This packet will serve as yur ntes fr this chapter. Fllw alng with the PwerPint presentatin and fill in the missing infrmatin. Imprtant

More information

Equation for Global Warming

Equation for Global Warming Equation for Global Warming Derivation and Application Contents 1. Amazing carbon dioxide How can a small change in carbon dioxide (CO 2 ) content make a critical difference to the actual global surface

More information

Matter Content from State Frameworks and Other State Documents

Matter Content from State Frameworks and Other State Documents Atms and Mlecules Mlecules are made f smaller entities (atms) which are bnded tgether. Therefre mlecules are divisible. Miscnceptin: Element and atm are synnyms. Prper cnceptin: Elements are atms with

More information

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics Chapters 9 and 35 Thermchemistry and Chemical Thermdynamics 1 Cpyright (c) 011 by Michael A. Janusa, PhD. All rights reserved. Thermchemistry Thermchemistry is the study f the energy effects that accmpany

More information

Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals of Diffusion

Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals of Diffusion Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals f Diffusin Diffusin: Transprt in a slid, liquid, r gas driven by a cncentratin gradient (r, in the case f mass transprt, a chemical ptential

More information

Unique nature of Earth s atmosphere: O 2 present photosynthesis

Unique nature of Earth s atmosphere: O 2 present photosynthesis Atmospheric composition Major components N 2 78% O 2 21% Ar ~1% Medium components CO 2 370 ppmv (rising about 1.5 ppmv/year) CH 4 1700 ppbv H 2 O variable Trace components H 2 600 ppbv N 2 O 310 ppbv CO

More information

Determination of radiative forcing of Saharan dust using combined TOMS and ERBE data

Determination of radiative forcing of Saharan dust using combined TOMS and ERBE data JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 105, NO. D16, PAGES 20,649-20,661, AUGUST 27, 2000 Determinatin f radiative frcing f Saharan dust using cmbined TOMS and ERBE data N. Christina Hsu Raythen ITSS, Lanham,

More information

( ) kt. Solution. From kinetic theory (visualized in Figure 1Q9-1), 1 2 rms = 2. = 1368 m/s

( ) kt. Solution. From kinetic theory (visualized in Figure 1Q9-1), 1 2 rms = 2. = 1368 m/s .9 Kinetic Mlecular Thery Calculate the effective (rms) speeds f the He and Ne atms in the He-Ne gas laser tube at rm temperature (300 K). Slutin T find the rt mean square velcity (v rms ) f He atms at

More information

NUMBERS, MATHEMATICS AND EQUATIONS

NUMBERS, MATHEMATICS AND EQUATIONS AUSTRALIAN CURRICULUM PHYSICS GETTING STARTED WITH PHYSICS NUMBERS, MATHEMATICS AND EQUATIONS An integral part t the understanding f ur physical wrld is the use f mathematical mdels which can be used t

More information

Retrieval of surface radiative fluxes on the Dlarginal zone of sea ice from. operational satellite data

Retrieval of surface radiative fluxes on the Dlarginal zone of sea ice from. operational satellite data Annals f Glacilgy 7 993 Internatinal Glacilgical Sciety Retrieval f surface radiative fluxes n the Dlarginal zne f sea ice frm. peratinal satellite data CLAUDE KERGOMARD, BERNARD BONNEL AND YVES FOUQUART

More information

Study Guide Physics Pre-Comp 2013

Study Guide Physics Pre-Comp 2013 I. Scientific Measurement Metric Units S.I. English Length Meter (m) Feet (ft.) Mass Kilgram (kg) Pund (lb.) Weight Newtn (N) Ounce (z.) r pund (lb.) Time Secnds (s) Secnds (s) Vlume Liter (L) Galln (gal)

More information

Lecture 12: Chemical reaction equilibria

Lecture 12: Chemical reaction equilibria 3.012 Fundamentals f Materials Science Fall 2005 Lecture 12: 10.19.05 Chemical reactin equilibria Tday: LAST TIME...2 EQUATING CHEMICAL POTENTIALS DURING REACTIONS...3 The extent f reactin...3 The simplest

More information

SAP report on GWPs in Group I of Annex A, C and F. SAP co-chairs: David W. Fahey, Paul A. Newman, John Pyle, Bonfils Safari SAP members

SAP report on GWPs in Group I of Annex A, C and F. SAP co-chairs: David W. Fahey, Paul A. Newman, John Pyle, Bonfils Safari SAP members SAP report on GWPs in Group I of Annex A, C and F SAP co-chairs: David W. Fahey, Paul A. Newman, John Pyle, Bonfils Safari SAP members Background Kigali Amendment comment, 204....the Scientific Assessment

More information

ASTR 1040: Stars & Galaxies

ASTR 1040: Stars & Galaxies ASTR 1040: Stars & Galaxies Onward t Galaxies, starting with ur wn! M51 Whirlpl Prf. Juri Tmre TA: Ryan Orvedahl Lecture 21 Tues 1 Apr 2014 6 Our Milky Way Galaxy in verview, aspects f any spiral galaxy

More information

Impact of an improved longwave radiation model, RRTM, on the energy budget and thermodynamic properties of the NCAR

Impact of an improved longwave radiation model, RRTM, on the energy budget and thermodynamic properties of the NCAR JOURNAL OF GEOPHYSCAL RESEARCH, VOL. 105, NO. Dll, PAGES 14,873-14,890, JUNE 16, 2000 mpact f an imprved lngwave radiatin mdel, RRTM, n the energy budget and thermdynamic prperties f the NCAR cmmunity

More information

Lecture 3a: Surface Energy Balance

Lecture 3a: Surface Energy Balance Lecture 3a: Surface Energy Balance Instructor: Prof. Johnny Luo http://www.sci.ccny.cuny.edu/~luo Total: 50 pts Absorption of IR radiation O 3 band ~ 9.6 µm Vibration-rotation interaction of CO 2 ~

More information

Name: Period: Date: BONDING NOTES ADVANCED CHEMISTRY

Name: Period: Date: BONDING NOTES ADVANCED CHEMISTRY Name: Perid: Date: BONDING NOTES ADVANCED CHEMISTRY Directins: This packet will serve as yur ntes fr this chapter. Fllw alng with the PwerPint presentatin and fill in the missing infrmatin. Imprtant terms

More information

GAW Patnership with BIPM (International Metrology)

GAW Patnership with BIPM (International Metrology) GAW Patnership with BIPM (Internatinal Metrlgy) J. Vialln, BIPM GAW Sympsium 10-13 April 2017, WMO, Geneva The BIPM / Internatinal Metrlgy The BIPM is an intergvernmental rganizatin established by the

More information

CHEM 116 Concentrations and Colligative Properties

CHEM 116 Concentrations and Colligative Properties UMass stn, Chem 116 CHEM 116 Cncentratins and Clligative Prperties FSG is Mndays 11:00 am Lecture 10 Prf. Sevian and Tuesdays 3:30 pm bth in S-1-89 Tday s agenda Ways f expressing cncentratin Clligative

More information

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 Atmospheric "greenhouse effect" - How the presence of an atmosphere makes Earth's surface warmer Some relevant parameters and facts (see previous slide sets) (So/) 32 W m -2 is the average incoming solar

More information

ATOMIC ORBITAL MODEL OF THE ATOM Be able to draw rough sketches of s, p and d orbitals with different principal quantum numbers

ATOMIC ORBITAL MODEL OF THE ATOM Be able to draw rough sketches of s, p and d orbitals with different principal quantum numbers Chapter 7 Atmic Structure and Peridicity ATOMIC ORBITAL MODEL OF THE ATOM Be able t draw rugh sketches f s, p and d rbitals with different principal quantum numbers ELECTRONIC CONFIGURATIONS Knw the difference

More information

CHEM 1001 Problem Set #3: Entropy and Free Energy

CHEM 1001 Problem Set #3: Entropy and Free Energy CHEM 1001 Prblem Set #3: Entry and Free Energy 19.7 (a) Negative; A liquid (mderate entry) cmbines with a slid t frm anther slid. (b)psitive; One mle f high entry gas frms where n gas was resent befre.

More information

Chapter 2: The global ledger of radiation and heat

Chapter 2: The global ledger of radiation and heat Chapter 2: The global ledger of radiation and heat PROPERTIES OF RADIATION Everything radiates at all wavelengths! This includes the Sun, Earth, a candy bar, even us Fortunately, most objects don t radiate

More information

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

Climate vs Weather J. J. Hack/A. Gettelman: June 2005 Climate vs Weather J. J. Hack/A. Gettelman: June 2005 What is Climate? J. J. Hack/A. Gettelman: June 2005 Characterizing Climate Climate change and its manifestation in terms of weather (climate extremes)

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Problem Solving 10: The Greenhouse Effect. Section Table and Group

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Problem Solving 10: The Greenhouse Effect. Section Table and Group MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Problem Solving 10: The Greenhouse Effect Section Table and Group Names Hand in one copy per group at the end of the Friday Problem Solving

More information

Introduction to Electromagnetic Radiation and Radiative Transfer

Introduction to Electromagnetic Radiation and Radiative Transfer Introduction to Electromagnetic Radiation and Radiative Transfer Temperature Dice Results Visible light, infrared (IR), ultraviolet (UV), X-rays, γ-rays, microwaves, and radio are all forms of electromagnetic

More information

11/1/18. Our Milky Way Galaxy THIS INSPIRES A SONG! Onward to Galaxies, starting with our own! Stars and gas are all moving!

11/1/18. Our Milky Way Galaxy THIS INSPIRES A SONG! Onward to Galaxies, starting with our own! Stars and gas are all moving! ASTR 1040: Stars & Galaxies Prf. Juri Tmre TAs: Ryan Hrtn, Lren Matilsky Lecture 20 Thur 1 Nv 2018 zeus.clrad.edu/astr1040-tmre M51 Whirlpl Onward t Galaxies, starting with ur wn! Our Milky Way Galaxy

More information

THE EXOSPHERIC HEAT BUDGET

THE EXOSPHERIC HEAT BUDGET E&ES 359, 2008, p.1 THE EXOSPHERIC HEAT BUDGET What determines the temperature on earth? In this course we are interested in quantitative aspects of the fundamental processes that drive the earth machine.

More information

Edexcel GCSE Physics

Edexcel GCSE Physics Edexcel GCSE Physics Tpic 10: Electricity and circuits Ntes (Cntent in bld is fr Higher Tier nly) www.pmt.educatin The Structure f the Atm Psitively charged nucleus surrunded by negatively charged electrns

More information

Stefan-Boltzmann law for the Earth as a black body (or perfect radiator) gives:

Stefan-Boltzmann law for the Earth as a black body (or perfect radiator) gives: 2. Derivation of IPCC expression ΔF = 5.35 ln (C/C 0 ) 2.1 Derivation One The assumptions we will make allow us to represent the real atmosphere. This remarkably reasonable representation of the real atmosphere

More information

Honors Physics Final Review Summary

Honors Physics Final Review Summary Hnrs Physics Final Review Summary Wrk Dne By A Cnstant Frce: Wrk describes a frce s tendency t change the speed f an bject. Wrk is dne nly when an bject mves in respnse t a frce, and a cmpnent f the frce

More information

Work and Heat Definitions

Work and Heat Definitions Wrk and eat Deinitins FL- Surrundings: Everything utside system + q -q + System: he part S the rld e are bserving. Wrk, : transer energy as a result unbalanced rces - eat, q: transer energy resulting rm

More information

NAME TEMPERATURE AND HUMIDITY. I. Introduction

NAME TEMPERATURE AND HUMIDITY. I. Introduction NAME TEMPERATURE AND HUMIDITY I. Intrductin Temperature is the single mst imprtant factr in determining atmspheric cnditins because it greatly influences: 1. The amunt f water vapr in the air 2. The pssibility

More information

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 Atmospheric "greenhouse effect" - How the presence of an atmosphere makes Earth's surface warmer Some relevant parameters and facts (see previous slide sets) (So/) 32 W m -2 is the average incoming solar

More information

Atmospheric Radiation

Atmospheric Radiation Atmospheric Radiation NASA photo gallery Introduction The major source of earth is the sun. The sun transfer energy through the earth by radiated electromagnetic wave. In vacuum, electromagnetic waves

More information

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review)

Part One: Heat Changes and Thermochemistry. This aspect of Thermodynamics was dealt with in Chapter 6. (Review) CHAPTER 18: THERMODYNAMICS AND EQUILIBRIUM Part One: Heat Changes and Thermchemistry This aspect f Thermdynamics was dealt with in Chapter 6. (Review) A. Statement f First Law. (Sectin 18.1) 1. U ttal

More information

ALE 21. Gibbs Free Energy. At what temperature does the spontaneity of a reaction change?

ALE 21. Gibbs Free Energy. At what temperature does the spontaneity of a reaction change? Name Chem 163 Sectin: Team Number: ALE 21. Gibbs Free Energy (Reference: 20.3 Silberberg 5 th editin) At what temperature des the spntaneity f a reactin change? The Mdel: The Definitin f Free Energy S

More information

Energy Balance and Temperature. Ch. 3: Energy Balance. Ch. 3: Temperature. Controls of Temperature

Energy Balance and Temperature. Ch. 3: Energy Balance. Ch. 3: Temperature. Controls of Temperature Energy Balance and Temperature 1 Ch. 3: Energy Balance Propagation of Radiation Transmission, Absorption, Reflection, Scattering Incoming Sunlight Outgoing Terrestrial Radiation and Energy Balance Net

More information

Energy Balance and Temperature

Energy Balance and Temperature Energy Balance and Temperature 1 Ch. 3: Energy Balance Propagation of Radiation Transmission, Absorption, Reflection, Scattering Incoming Sunlight Outgoing Terrestrial Radiation and Energy Balance Net

More information

The Atmosphere. Giovanna Jerse

The Atmosphere. Giovanna Jerse The Atmsphere Givanna Jerse Thickness f the Atmsphere Apprximately 80% f the atmsphere ccurs in the lwest 20km abve the Earth. Radius f the Earth is ver 6,000 km Atmsphere is a thin shell cvering the Earth.

More information

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

Learning goals. Good absorbers are good emitters Albedo, and energy absorbed, changes equilibrium temperature Greenhouse effect Learning goals Good absorbers are good emitters Albedo, and energy absorbed, changes equilibrium temperature Wavelength (color) and temperature related: Wein s displacement law Sun/Hot:

More information

M.Sc. in Meteorology. Physical Meteorology Prof Peter Lynch. Mathematical Computation Laboratory Dept. of Maths. Physics, UCD, Belfield.

M.Sc. in Meteorology. Physical Meteorology Prof Peter Lynch. Mathematical Computation Laboratory Dept. of Maths. Physics, UCD, Belfield. M.Sc. in Meteorology Physical Meteorology Prof Peter Lynch Mathematical Computation Laboratory Dept. of Maths. Physics, UCD, Belfield. Part 3 Radiative Transfer in the Atmopshere 2 Outline of Material

More information