Hand in Question sheets with answer booklets Calculators allowed Mobile telephones or other devices not allowed

Similar documents
Lecture 9: Climate Sensitivity and Feedback Mechanisms

Lecture 3: Global Energy Cycle

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

Lecture 3: Atmospheric Radiative Transfer and Climate

Earth: the Goldilocks Planet

Lecture 2: Global Energy Cycle

1. Weather and climate.

G109 Midterm Exam (Version A) October 10, 2006 Instructor: Dr C.M. Brown 1. Time allowed 50 mins. Total possible points: 40 number of pages: 5

Radiation in the atmosphere

Understanding the Greenhouse Effect

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

The Atmosphere. Topic 3: Global Cycles and Physical Systems. Topic 3: Global Cycles and Physical Systems. Topic 3: Global Cycles and Physical Systems

Lecture 2 Global and Zonal-mean Energy Balance

PTYS 214 Spring Announcements. Midterm 3 next Thursday!

Lecture 10: Climate Sensitivity and Feedback

MAPH & & & & & & 02 LECTURE

Glaciology HEAT BUDGET AND RADIATION

Radiation and the atmosphere

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

8.5 GREENHOUSE EFFECT 8.6 GLOBAL WARMING HW/Study Packet

8. Clouds and Climate

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

Radiation in climate models.

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

Data and formulas at the end. Exam would be Weds. May 8, 2008

The Structure and Motion of the Atmosphere OCEA 101

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

G109 Alternate Midterm Exam October, 2004 Instructor: Dr C.M. Brown

Agronomy 406 World Climates January 11, 2018

Habitable Planets. Much of it stolen from. Yutaka ABE University of Tokyo

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

Assessment Schedule 2017 Earth and Space Science: Demonstrate understanding of processes in the atmosphere system (91414)

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

Planetary Atmospheres

Fundamentals of Atmospheric Radiation and its Parameterization

1. Radiative Transfer. 2. Spectrum of Radiation. 3. Definitions

Radiative Balance and the Faint Young Sun Paradox

Radiative equilibrium Some thermodynamics review Radiative-convective equilibrium. Goal: Develop a 1D description of the [tropical] atmosphere

Earth: A Dynamic Planet A. Solar and terrestrial radiation

Data and formulas at the end. Real exam is Wednesday May 8, 2002

Planetary Atmospheres

Earth s Energy Balance and the Atmosphere

ATMS 321: Sci. of Climate Final Examination Study Guide Page 1 of 4

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

Planetary Temperatures

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

Climate Dynamics (PCC 587): Feedbacks & Clouds

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

1. The frequency of an electromagnetic wave is proportional to its wavelength. a. directly *b. inversely

GEO1010 tirsdag

Equation for Global Warming

THE EXOSPHERIC HEAT BUDGET

PTYS 214 Fall Announcements

Chapter 02 Energy and Matter in the Atmosphere

1. The most important aspects of the quantum theory.

Chapter 11 Lecture Outline. Heating the Atmosphere

General Comments about the Atmospheres of Terrestrial Planets

The University of British Columbia Geography 200 Sample Exam Questions. Here are some reminders about GEOB 200 Fianl exam:

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

Energy: Warming the earth and Atmosphere. air temperature. Overview of the Earth s Atmosphere 9/10/2012. Composition. Chapter 3.

Let s make a simple climate model for Earth.

Outline. Planetary Atmospheres. General Comments about the Atmospheres of Terrestrial Planets. General Comments, continued

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

AT350 EXAM #1 September 23, 2003

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

Earth s Energy Budget: How Is the Temperature of Earth Controlled?

2. Illustration of Atmospheric Greenhouse Effect with Simple Models

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

EAS270, The Atmosphere 2 nd Mid-term Exam 2 Nov. 2016

Name(s) Period Date. Earth s Energy Budget: How Is the Temperature of Earth Controlled?

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

Energy Balance and Temperature

Lecture 4: Radiation Transfer

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

AT 350 EXAM #1 February 21, 2008

AST 105 Intro Astronomy The Solar System

Climate 1: The Climate System

Prentice Hall EARTH SCIENCE. Tarbuck Lutgens

Chapter 2. Heating Earth's Surface & Atmosphere

T eff = [F s (1 - A)/(4σ)] ¼ = K.

P607 Climate and Energy (Dr. H. Coe)

Temperature Scales

Project 3 Convection and Atmospheric Thermodynamics

Lecture 4: Global Energy Balance

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

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

Radiation Conduction Convection

ATMOS 5140 Lecture 1 Chapter 1

Exercises. Exercises 145

The current climate epoch: The Holocene

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

Remote Sensing C. Rank: Points: Science Olympiad North Regional Tournament at the University of Florida. Name(s): Team Name: School Name:

ATMS 321 Problem Set 1 30 March 2012 due Friday 6 April. 1. Using the radii of Earth and Sun, calculate the ratio of Sun s volume to Earth s volume.

Inaugural University of Michigan Science Olympiad Tournament

Clouds, Haze, and Climate Change

Ross Salawitch. Class Web Site: 4) Geostrophy (balance of pressure force & Coriolis Force storms)

Today. Spectra. Thermal Radiation. Wien s Law. Stefan-Boltzmann Law. Kirchoff s Laws. Emission and Absorption. Spectra & Composition

1 Thermodynamics: some Preliminaries

Tananyag fejlesztés idegen nyelven

Transcription:

York University Department of Earth and Space Science and Engineering ESSE 3030 Department of Physics and Astronomy PHYS 3080 Atmospheric Radiation and Thermodynamics Final Examination 2:00 PM 11 December 2016 Duration: 3 hours Hand in Question sheets with answer booklets Calculators allowed Mobile telephones or other devices not allowed 100 marks in total: Q1 40 marks Q2 15 marks Q3 15 marks Q4 10 marks Q5 10 marks Q6 10 marks Useful information is given on page 5. 1

1. Explain: (4 marks each, 40 in total) a) Blue sky, red sunset. b) On a clear still night, the surface temperature drops more rapidly when the air above is dry than when it is moist. c) Surface temperature and the effective radiating temperature for a planet are not equal. d) Two climate feedback processes. e) High altitude clouds tend to have a warming effect on climate while low clouds tend to have a cooling effect. f) Ice crystals grow most rapidly by vapour deposition when there are also liquid water droplets present. g) Chapman profile for absorption of solar radiation. h) The Earth s climate would be very different if the atmosphere did not contain particulate matter (aerosol). i) Atomic Oxygen is the most abundant constituent in the atmosphere above a height of 150 km. j) The dryness of the stratosphere is explained by the circulation pattern in which air enters by rising through the tropical tropopause. 2. a) Show that if the Earth were covered entirely with ice having an albedo of 0.75, it would be possible to remain in that state indefinitely if the composition of the atmosphere did not change. (5 marks) b) If the sun were somewhat bluer in colour, so that it s wavelength of maximum emission was 0.4 μm instead of 0.475 μm, calculate the effective radiating temperature of the Earth under these conditions. (5 marks) c) Compute the temperature at the top of the troposphere (the skin temperature ) assuming that transfer of infrared radiation is the only important process. (5 marks) 2

3. Consider a simple climate model in which the Earth s atmosphere is represented as a single layer that is transparent to solar radiation, but has an absorptivity, a, in the infrared. The Earth s overall albedo is 0.3. a) Draw a diagram to illustrate the contributions to the radiation budget above the atmosphere and directly above the surface. (5 marks) b) Determine the IR absorptivity for the atmosphere that will result in a ground temperature that is equal to the current average of 288 K for the Earth. (5 marks) c) A doubling of carbon dioxide will cause the infrared absorptivity of the atmosphere to increase by 2.6 %. Calculate the resulting change in surface temperature. (5 marks) 4.) a) What fraction of incident radiation is absorbed in passing through the layer in the atmosphere extending from optical depth 0.2 to 4.0. (5 marks) b) Of the intensity that is emitted to space by an isothermal atmosphere, what fraction is emitted from the layer extending from an optical depth of 0.2 to 4.0. (5 marks) 5.) a) The spectra of intensity of infrared radiation measured from orbit above Antarctica and the Sahara Desert are shown in Figures 1a and 1b. Explain why there is a relative maximum for wavelengths in the range 13 17 μm above Antarctica, but there is a relative minimum for the same wavelengths above the Sahara Desert. (5 marks) b) Figure 1c shows the spectrum of infrared radiation measured above the Pacific Ocean when the atmosphere was cloud free and also above a thick thunderstorm anvil outflow cloud. Estimate the height of the anvil cloud top assuming that the lapse rate was 6 o C per km throughout the troposphere. (5 marks) 6.) Consider a location in the tropics where the average flux of solar radiation at the top of the atmosphere is 400 W/m 2. A cloud scatters 50 % of the incident solar radiation back to space, and it has an infrared absorptivity of 1.0. a) Calculate the temperature of the cloud top for which the combined effects of the cloud on solar and infrared radiation would cancel. (5 marks) b) What is the lowest cloud top height for a net positive heating effect on climate? Assume the ground temperature is 30 o C and the lapse rate is 6 o C per km throughout the troposphere. (5 marks) 3

Figure 1. Spectra of infrared radiation intensity measured from an orbiting satellite above (a) the Sahara Desert (no clouds), (b) Antarctica (no clouds), and (c) the tropical western Pacific Ocean. (c) includes a spectrum measured above clear air as well as a specrum measured above a thick thunderstorm anvil outflow cloud (as labeled). Plank function curves at various temperatures are shown (dashed lines) for comparison. 4

Information Earth-Sun mean distance: 149.598 x 10 9 m (one A.U.) Radius of Sun: 6.96 x 10 8 m Radius of Earth: 6371 x 10 3 m Effective temperature of Sun: 5770 K Cross sectional area of a sphere: πr 2 Surface area of a sphere: 4πR 2 Solid Angle: W = Area on sphere/r 2 ; dw = sinq dq df Flux of solar radiation at the Earth: Fs = 1370 W/m 2 Albedo of the Earth: A = 0.3 Plank Function: B(λ,T) = 2hc 2 /λ 5 (e hc/kλt 1) Plank s constant: h = 6.626 10-34 J s Boltzmann s constant: k = 1.381 10-23 J/K Speed of light: c = 3 x 10 8 m/s Stephan-Boltzmann Law: F = σt 4 Stephan s constant: σ = 5.67 10-8 W m -2 K -4 For isotropic radiation: F = p I Wien s displacement Law: λp = 2898/T μm Beer s Law: I = Io exp(-χ); dχ = kρdz/cosθ Schwarzchild s equation:!" #$!% = I + J Ideal Gas Law: P = ρrt; R = 287 J Kg -1 K -1 Barometric Law: P(z) = Po exp(-z/h); H = RT/g; Po = 100 10 3 Pa ; g = 9.81 m/s 2 Latent Heat of Sublimation for water ice at temperature 270 K: 2464 J/g 5