AT760 Global Carbon Cycle. Assignment #3 Due Friday, May 4, 2007 Atmospheric Transport and Inverse Modeling of CO 2

Size: px
Start display at page:

Download "AT760 Global Carbon Cycle. Assignment #3 Due Friday, May 4, 2007 Atmospheric Transport and Inverse Modeling of CO 2"

Transcription

1 AT760 Global Carbon Cycle Assignment 3 Due Friday, May 4, 2007 Atmospheric Transport and Inverse Modeling of CO 2 In this exercise you will develop a very simplified model of the mixing of the global atmosphere. Sources and sinks of CO 2 at the surface of the model will be specified, and a global distribution of timemean CO 2 will be obtained. Then you will sample the CO 2 from your model, and try to estimate the original map of sources and sinks using the Bayesian synthesis inversion method discussed in class. Problem 1: The forward transport model Calculate [CO 2 ] concentrations from fluxes Consider an atmosphere consisting of six wellmixed boxes. The boxes divide the Earth by zones: Northern, Tropical, and Southern; and by altitude: lower and upper troposphere. Divide the zones at 30 N and 30 S latitude. In the vertical, the lower boxes will represent the air from the surface to 800 mb (about 2 km), and the upper box will span from there to 200 mb (which we ll think of as the tropopause). We ll ignore the stratosphere. Transport: Pretend the atmospheric transport is just by mixing, rather than organized advection, convection, and turbulence. Each zone mixes vertically, and adjacent zones mix horizontally in the upper troposphere. We ll ignore horizontal mixing in the lower troposphere. Predict the rate of change of concentration in each box due to surface fluxes (sources and sinks) and mixing with each adjacent box. Because the masses of the upper and lower boxes differ, you ll also have to take this into account. So, for each box M!C!t N = F + " M (C C) i i i=1 $ i 1

2 AT760 Assignment 3 Due May 4, 2007 where M is the mass of the current box, C is the concentration of CO 2, F is the surface flux of CO 2 into the box, C i is the mixng ratio of CO 2 in the i th neighboring box, and τ i is the time scale for mixing between box i and the current box. There are N neighboring boxes with which to mix. The timescale for vertical mixing in the tropics is 10 days, because of the vigorous convective clouds there, but 20 days outside the tropics. Horizontal mixing is slower: use 50 days for mixing between the tropics and the higher latitudes of both hemispheres, but only in the upper boxes. We ll assume that horizontal mixing between the lower boxes is negligible. Units: You can work this problem in a variety of ways, but here s my suggestion. Predict the mass mixing ratio of carbon (not CO 2 ) in each box, so that C is kg C per kg air. That way M is just the mass of each box in kg. (Don t worry about the extra mass of C, which is negligible compared to M.) Surface fluxes S are then to be expressed in kg s 1, and mixing times are in s. I ll give you fluxes in Gt C yr 1, and mixing times in days, but you can just convert them. 1 GtC is kg or g. CO 2 concentrations are usually written in ppm by volume, which is the same as mole fraction or µmol mol 1. This can be a bit confusing, because you ve predicted kg C kg air 1. The molecular weight of carbon (not CO 2 ) is 12 g mol 1, and the molecular weight of dry air is 29 g mol 1. The mass of air in each box is M = A Δp/g where A = the area of the surface of the box (m 2 ), Δp is the pressure depth (in Pascals, 1 mb = 100 Pa), and g = 9.81 m s 2. As it turns out, exactly half the area of the Earth s surface lies between 30 N and 30 S latitude. The radius of the Earth is 6371 km. Let the surface pressure be mb. Sources and Sinks: Prescribe the following surface fluxes for your model = 2 Gt C yr 1 (uptake by the Southern Ocean) = +1 Gt C yr 1 (deforestation plus Equatorial upwelling minus Cfertilization) = +5 Gt C yr 1 (fossil fuel combustion minus a big land sink) Numerics: I suggest using an explicit timedifferencing scheme because it s the easiest to code. This is a diffusion problem, and explicit schemes are unstable for diffusion, but it should be OK if your model time step is much shorter than the fastest mixing time in the problem. I suggest a time step of 1 day. Procedure: Start the model from an initial condition with 375 ppm of CO 2 everywhere, and run it for 3 years. Make a plot of the concentration in each box over time, using different linestyles or colors for each box. 2

3 AT760 Assignment 3 Due May 4, 2007 Problem 2: The inverse model Estimate fluxes from [CO 2 ] concentrations Now suppose you don t know the surface fluxes,, and, but have a set of observations of [CO 2 ] and want to estimate the fluxes using the transport model you developed in problem 1. Consider an observing system in which we make measurements of the mean CO 2 concentration in each of the lower boxes in the a given year. Each measured concentration results from the influence of the three fluxes after mixing by atmospheric transport. There is also some background or offset concentration that all three observations share. So the concentration at the observing stations (C NL, C TL, C SL ) can be represented in terms of the three unknown fluxes (,, ) as a linear system of three equations in three unknowns (four if you count C 0 ): C NL =!C NL! +!C NL! +!C NL! C TL =!C TL! +!C TL! +!C TL!. C SL =!C SL! +!C SL! +!C SL! For the very simple problem here, it can be shown the time variation is irrelevant after equilibrium gradients have been established, and you can therefore just substitute the final value of your simulated concentrations for annual means. This linear system can be rewritten in matrix form as where d = G m! d = " C NL C TL C SL $!!!,!!G = % ( ) ' ' ' ' ' ' ' ' ' +!!,!!!m = ", $. % 3

4 AT760 Assignment 3 Due May 4, 2007 Solution: To estimate the fluxes, solve the matrix equation d = G m for the vector m, subject to prior constraints on the fluxes, and considering uncertainties in both the fluxes and the concentration data. The inversion should be done using the weighted leastsquares method discussed by Tarantola (1987) and Gurney et al (2002), as presented in class. Observations: Let there be a single observation in each surface grid box, representing conditions at the end of your run. The madeup observations d = [7.345, 4.750, 2.803] represent changes from the initial condition of 375 ppmv at the beginning of the simulation in each surface box at the end of 3 years. d is a vector with 3 elements. Jacobian matrix G: The partial derivatives in each term are simply the annual mean response of [CO 2 ] at each site to a flux of unit strength in each region. These can easily be found by just running your transport model from problem 1 to equilibrium three times, with a flux of 1 GtC yr 1 in each of the three zones and zero in the other two. Take the final concentration in each box and subtract the initial 375 to obtain each element of G. G is a 3x3 matrix. Error covariance in the observations are formally given by the matrix C d, whose main diagonal contains σ 2 of each observation of CO 2. Traditionally this would be thought of as measurement error, but for the CO 2 problem it contains primarily representation error (degree to which individual observations differ from the zonal annual mean in the model) and transport error. Use σ=0.2 ppm (σ 2 =0.04 ppm 2 ) for each of these, and assume they are uncorrelated. That means the offdiagonal elements will all be exactly zero, and that the inverse C d 1 is found by replacing the elements on the main diagonal of C d with their reciprocals. C d 1 is a 3x3 matrix. For prior constraints, assume that the fluxes in each box are the ones given in Problem 1: m prior = [+5, +1, 2] Gt C yr 1. Let uncertainty in these prior estimates have a standard deviation of 1.0 Gt C yr 1 and no correlation in the errors. This corresponds to C m matrix that has 1.0 down the diagonal and 0.0 elsewhere. As for the error covariance of the observations, the inverse of C m is therefore the same as C m itself. C m 1 is a 3x3 matrix. Remember (or look up) the rules for multiplying and adding matrices, and for finding their inverse. You will find that the biggest matrix you have to work with in this problem is a 3x3, so it would be easy to do this whole problem with pencil and paper (no coding). You might have to remind yourself how to do Gaussian elimination to get the final answers. You may you a computer for this if you prefer, but in either case, please show your work. Don t just hand in a final answer. 4

5 AT760 Assignment 3 Due May 4, 2007 The solution is found from m est = m prior + [G T C 1 d G + C 1 m ] 1 G T C 1 d [d G m prior ] with uncertainty in the final estimate given by C m = [G T C 1 d G + C 1 m ] 1 Here m prior is your prior estimate of the fluxes C m 1 is the reciprocal of the covariance matrix of prior flux estimates C d 1 is the reciprocal of the error covariance matrix of the data C m is the a posteriori covariance matrix. Uncertainty (1 σ) in your final estimates (in Gt C yr 1 ) is given by the square root of each element of the main diagonal of C m. Make a table of your results as follows: NH Tropics SH Prior Estimate Uncertainty 5

Carbon Cycle: Definition of the problem. Inez Fung

Carbon Cycle: Definition of the problem. Inez Fung Carbon Cycle: Definition of the problem Inez Fung Mean Meridional Circulation + Convection June July August pressure Dec Jan Feb Intertropical Convergence Zone (ITCZ): v=0: barrier to interhemispheric

More information

: 1.9 ppm y -1

: 1.9 ppm y -1 Atmospheric CO 2 Concentration Year 2006 Atmospheric CO 2 concentration: 381 ppm 35% above pre-industrial Atmoapheric [CO2] (ppmv) 4001850 1870 1890 1910 1930 1950 1970 1990 2010 380 360 340 320 300 280

More information

Carbon Cycle: An Inverse Problem. Inez Fung

Carbon Cycle: An Inverse Problem. Inez Fung Carbon Cycle: An Inverse Problem Inez Fung Outstanding Questions Only half of the CO 2 produced by human activities is remaining in the atmosphere Where are the sinks that are absorbing over 40% of the

More information

2. Outline of the MRI-EPS

2. Outline of the MRI-EPS 2. Outline of the MRI-EPS The MRI-EPS includes BGM cycle system running on the MRI supercomputer system, which is developed by using the operational one-month forecasting system by the Climate Prediction

More information

K32: The Structure of the Earth s Atmosphere

K32: The Structure of the Earth s Atmosphere K32: The Structure of the Earth s Atmosphere Chemical composition Vertical Layers Temperature structure Coriolis Force and horizontal structure Hadley Cells and Heat sources Current Molecular Composition

More information

Unit 2 Meteorology Test **Please do not write on this test** 5. El Nino & La Nina 6. Photosynthesis 7. Coriolis Effect 8.

Unit 2 Meteorology Test **Please do not write on this test** 5. El Nino & La Nina 6. Photosynthesis 7. Coriolis Effect 8. Matching (2 points each) 1. weather 2. climate 3. Greenhouse Effect 4. Convection Unit 2 Meteorology Test **Please do not write on this test** 5. El Nino & La Nina 6. Photosynthesis 7. Coriolis Effect

More information

A B C D PROBLEMS Dilution of power plant plumes. z z z z

A B C D PROBLEMS Dilution of power plant plumes. z z z z 69 PROBLEMS 4. Dilution of power plant plumes Match each power plant plume (-4) to the corresponding atmospheric lapse rate (A-D, solid lines; the dashed line is the adiabatic lapse rate Γ). Briefly comment

More information

Regional Climatology. Lab Number One Atmospheric Processes

Regional Climatology. Lab Number One Atmospheric Processes Name: Time of Class: Due Date: Regional Climatology Lab Number One Atmospheric Processes Part I: Group Discussion and Answer Directions: Arrange a group of three to five individuals. Discuss each of the

More information

Boundary layer equilibrium [2005] over tropical oceans

Boundary layer equilibrium [2005] over tropical oceans Boundary layer equilibrium [2005] over tropical oceans Alan K. Betts [akbetts@aol.com] Based on: Betts, A.K., 1997: Trade Cumulus: Observations and Modeling. Chapter 4 (pp 99-126) in The Physics and Parameterization

More information

Volume in n Dimensions

Volume in n Dimensions Volume in n Dimensions MA 305 Kurt Bryan Introduction You ve seen that if we have two vectors v and w in two dimensions then the area spanned by these vectors can be computed as v w = v 1 w 2 v 2 w 1 (where

More information

5.6 Solving Equations Using Both the Addition and Multiplication Properties of Equality

5.6 Solving Equations Using Both the Addition and Multiplication Properties of Equality 5.6 Solving Equations Using Both the Addition and Multiplication Properties of Equality Now that we have studied the Addition Property of Equality and the Multiplication Property of Equality, we can solve

More information

Course , General Circulation of the Earth's Atmosphere Prof. Peter Stone Section 4: Water Vapor Budget

Course , General Circulation of the Earth's Atmosphere Prof. Peter Stone Section 4: Water Vapor Budget Course 12.812, General Circulation of the Earth's Atmosphere Prof. Peter Stone Section 4: Water Vapor Budget Water Vapor Distribution First let us look at the distribution of specific humidity, q. The

More information

Atmospheric CO2 Observations

Atmospheric CO2 Observations ATS 760 Global Carbon Cycle Atmospheric CO2 Observations (in-situ) BRW MLO Point Barrow, Alaska Scott Denning CSU ATS Mauna Loa, Hawaii 1 ATS 760 Global Carbon Cycle SPO SMO American Samoa South Pole Interannual

More information

3. Carbon Dioxide (CO 2 )

3. Carbon Dioxide (CO 2 ) 3. Carbon Dioxide (CO 2 ) Basic information on CO 2 with regard to environmental issues Carbon dioxide (CO 2 ) is a significant greenhouse gas that has strong absorption bands in the infrared region and

More information

ATMO/OPTI 656b Spring 08. Physical Properties of the Atmosphere

ATMO/OPTI 656b Spring 08. Physical Properties of the Atmosphere Physical Properties of the Atmosphere Thin as a piece of paper The atmosphere is a very thin layer above the solid Earth and its oceans. This is true of the atmospheres of all of the terrestrial planets.

More information

2. Meridional atmospheric structure; heat and water transport. Recall that the most primitive equilibrium climate model can be written

2. Meridional atmospheric structure; heat and water transport. Recall that the most primitive equilibrium climate model can be written 2. Meridional atmospheric structure; heat and water transport The equator-to-pole temperature difference DT was stronger during the last glacial maximum, with polar temperatures down by at least twice

More information

1. Composition and Structure

1. Composition and Structure Atmospheric sciences focuses on understanding the atmosphere of the earth and other planets. The motivations for studying atmospheric sciences are largely: weather forecasting, climate studies, atmospheric

More information

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

G109 Alternate Midterm Exam October, 2004 Instructor: Dr C.M. Brown 1 Time allowed 50 mins. Answer ALL questions Total possible points;50 Number of pages:8 Part A: Multiple Choice (1 point each) [total 24] Answer all Questions by marking the corresponding number on the

More information

Vertical Structure of Atmosphere

Vertical Structure of Atmosphere ATMOS 3110 Introduction to Atmospheric Sciences Distribution of atmospheric mass and gaseous constituents Because of the earth s gravitational field, the atmosphere exerts a downward forces on the earth

More information

2/22/ Atmospheric Characteristics

2/22/ Atmospheric Characteristics 17.1 Atmospheric Characteristics Atmosphere: the gaseous layer that surrounds the Earth I. In the past, gases came from volcanic eruptions A. Water vapor was a major component of outgassing B. Other gases

More information

Atmospheric Sciences 321. Science of Climate. Lecture 13: Surface Energy Balance Chapter 4

Atmospheric Sciences 321. Science of Climate. Lecture 13: Surface Energy Balance Chapter 4 Atmospheric Sciences 321 Science of Climate Lecture 13: Surface Energy Balance Chapter 4 Community Business Check the assignments HW #4 due Wednesday Quiz #2 Wednesday Mid Term is Wednesday May 6 Practice

More information

A simple method for seamless verification applied to precipitation hindcasts from two global models

A simple method for seamless verification applied to precipitation hindcasts from two global models A simple method for seamless verification applied to precipitation hindcasts from two global models Matthew Wheeler 1, Hongyan Zhu 1, Adam Sobel 2, Debra Hudson 1 and Frederic Vitart 3 1 Bureau of Meteorology,

More information

Diagnosis of Relative Humidity Changes in a Warmer Climate Using Tracers of Last Saturation

Diagnosis of Relative Humidity Changes in a Warmer Climate Using Tracers of Last Saturation Diagnosis of Relative Humidity Changes in a Warmer Climate Using Tracers of Last Saturation 8 March, 2011 Jonathon Wright Department of Applied Mathematics & Theoretical Physics University of Cambridge

More information

8 Mechanisms for tropical rainfall responses to equatorial

8 Mechanisms for tropical rainfall responses to equatorial 8 Mechanisms for tropical rainfall responses to equatorial heating More reading: 1. Hamouda, M. and Kucharski, F. (2019) Ekman pumping Mechanism driving Precipitation anomalies in Response to Equatorial

More information

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

Electromagnetic Radiation. Radiation and the Planetary Energy Balance. Electromagnetic Spectrum of the Sun Radiation and the Planetary Energy Balance Electromagnetic Radiation Solar radiation warms the planet Conversion of solar energy at the surface Absorption and emission by the atmosphere The greenhouse

More information

HEIGHT-LATITUDE STRUCTURE OF PLANETARY WAVES IN THE STRATOSPHERE AND TROPOSPHERE. V. Guryanov, A. Fahrutdinova, S. Yurtaeva

HEIGHT-LATITUDE STRUCTURE OF PLANETARY WAVES IN THE STRATOSPHERE AND TROPOSPHERE. V. Guryanov, A. Fahrutdinova, S. Yurtaeva HEIGHT-LATITUDE STRUCTURE OF PLANETARY WAVES IN THE STRATOSPHERE AND TROPOSPHERE INTRODUCTION V. Guryanov, A. Fahrutdinova, S. Yurtaeva Kazan State University, Kazan, Russia When constructing empirical

More information

Computational Fluid Dynamics Prof. Sreenivas Jayanti Department of Computer Science and Engineering Indian Institute of Technology, Madras

Computational Fluid Dynamics Prof. Sreenivas Jayanti Department of Computer Science and Engineering Indian Institute of Technology, Madras Computational Fluid Dynamics Prof. Sreenivas Jayanti Department of Computer Science and Engineering Indian Institute of Technology, Madras Lecture 46 Tri-diagonal Matrix Algorithm: Derivation In the last

More information

p = ρrt p = ρr d = T( q v ) dp dz = ρg

p = ρrt p = ρr d = T( q v ) dp dz = ρg Chapter 1: Properties of the Atmosphere What are the major chemical components of the atmosphere? Atmospheric Layers and their major characteristics: Troposphere, Stratosphere Mesosphere, Thermosphere

More information

CHAPTER 4. THE HADLEY CIRCULATION 59 smaller than that in midlatitudes. This is illustrated in Fig. 4.2 which shows the departures from zonal symmetry

CHAPTER 4. THE HADLEY CIRCULATION 59 smaller than that in midlatitudes. This is illustrated in Fig. 4.2 which shows the departures from zonal symmetry Chapter 4 THE HADLEY CIRCULATION The early work on the mean meridional circulation of the tropics was motivated by observations of the trade winds. Halley (1686) and Hadley (1735) concluded that the trade

More information

Lecture 11: Meridonal structure of the atmosphere

Lecture 11: Meridonal structure of the atmosphere Lecture 11: Meridonal structure of the atmosphere September 28, 2003 1 Meridional structure of the atmosphere In previous lectures we have focussed on the vertical structure of the atmosphere. Today, we

More information

TIME SERIES COMPARISONS OF MIPAS LEVEL 2 NEAR REAL TIME PRODUCTS WITH CLIMATOLOGY

TIME SERIES COMPARISONS OF MIPAS LEVEL 2 NEAR REAL TIME PRODUCTS WITH CLIMATOLOGY TIME SERIES COMPARISONS OF MIPAS LEVEL 2 NEAR REAL TIME PRODUCTS WITH CLIMATOLOGY Vivienne Payne, Anu Dudhia, and Chiara Piccolo Atmospheric, Oceanic and Planetary Physics, Department of Physics, University

More information

On Stationary state, also called steady state. Lifetimes and spatial scales of variability

On Stationary state, also called steady state. Lifetimes and spatial scales of variability On sources and sinks ATOC 3500/CHEM 3151 Week 5-6 Additional Notes February 16/18, 2016 On lifetimes, variability, and models On Stationary state, also called steady state Lifetimes and spatial scales

More information

Physical Oceanography, MSCI 3001 Oceanographic Processes, MSCI Dr. Katrin Meissner Week 5.

Physical Oceanography, MSCI 3001 Oceanographic Processes, MSCI Dr. Katrin Meissner Week 5. Physical Oceanography, MSCI 3001 Oceanographic Processes, MSCI 5004 Dr. Katrin Meissner k.meissner@unsw.e.au Week 5 Ocean Dynamics Transport of Volume, Heat & Salt Flux: Amount of heat, salt or volume

More information

Rotating stratified turbulence in the Earth s atmosphere

Rotating stratified turbulence in the Earth s atmosphere Rotating stratified turbulence in the Earth s atmosphere Peter Haynes, Centre for Atmospheric Science, DAMTP, University of Cambridge. Outline 1. Introduction 2. Momentum transport in the atmosphere 3.

More information

What Goes Around Comes Around: Humankind, the Environmental Crisis, and the Future of Life on Earth

What Goes Around Comes Around: Humankind, the Environmental Crisis, and the Future of Life on Earth What Goes Around Comes Around: Humankind, the Environmental Crisis, and the Future of Life on Earth Again Earth As A Closed System Reminder: Earth Sciences 088F Final Exam Saturday, December 9, 2006 7:00

More information

Getting Started with Communications Engineering

Getting Started with Communications Engineering 1 Linear algebra is the algebra of linear equations: the term linear being used in the same sense as in linear functions, such as: which is the equation of a straight line. y ax c (0.1) Of course, if we

More information

ATMO/OPTI 656b Spring 09. Physical properties of the atmosphere

ATMO/OPTI 656b Spring 09. Physical properties of the atmosphere The vertical structure of the atmosphere. Physical properties of the atmosphere To first order, the gas pressure at the bottom of an atmospheric column balances the downward force of gravity on the column.

More information

Seasonal & Diurnal Temp Variations. Earth-Sun Distance. Eccentricity 2/2/2010. ATS351 Lecture 3

Seasonal & Diurnal Temp Variations. Earth-Sun Distance. Eccentricity 2/2/2010. ATS351 Lecture 3 Seasonal & Diurnal Temp Variations ATS351 Lecture 3 Earth-Sun Distance Change in distance has only a minimal effect on seasonal temperature. Note that during the N. hemisphere winter, we are CLOSER to

More information

ATMOSPHERIC ENERGY and GLOBAL TEMPERATURES. Physical Geography (Geog. 300) Prof. Hugh Howard American River College

ATMOSPHERIC ENERGY and GLOBAL TEMPERATURES. Physical Geography (Geog. 300) Prof. Hugh Howard American River College ATMOSPHERIC ENERGY and GLOBAL TEMPERATURES Physical Geography (Geog. 300) Prof. Hugh Howard American River College RADIATION FROM the SUN SOLAR RADIATION Primarily shortwave (UV-SIR) Insolation Incoming

More information

Chapter 4 Water Vapor

Chapter 4 Water Vapor Chapter 4 Water Vapor Chapter overview: Phases of water Vapor pressure at saturation Moisture variables o Mixing ratio, specific humidity, relative humidity, dew point temperature o Absolute vs. relative

More information

Winds and Global Circulation

Winds and Global Circulation Winds and Global Circulation Atmospheric Pressure Winds Global Wind and Pressure Patterns Oceans and Ocean Currents El Nino How is Energy Transported to its escape zones? Both atmospheric and ocean transport

More information

F = ma. ATS 150 Global Climate Change Winds and Weather. Scott Denning CSU CMMAP 1. Please read Chapter 6 from Archer Textbook

F = ma. ATS 150 Global Climate Change Winds and Weather. Scott Denning CSU CMMAP 1. Please read Chapter 6 from Archer Textbook Winds and Weather Please read Chapter 6 from Archer Textbook Circulation of the atmosphere and oceans are driven by energy imbalances Energy Imbalances What Makes the Wind Blow? Three real forces (gravity,

More information

The Equations of Motion in a Rotating Coordinate System. Chapter 3

The Equations of Motion in a Rotating Coordinate System. Chapter 3 The Equations of Motion in a Rotating Coordinate System Chapter 3 Since the earth is rotating about its axis and since it is convenient to adopt a frame of reference fixed in the earth, we need to study

More information

ERTH 465 Fall Lab 5. Absolute Geostrophic Vorticity. 200 points.

ERTH 465 Fall Lab 5. Absolute Geostrophic Vorticity. 200 points. Name Date ERTH 465 Fall 2015 Lab 5 Absolute Geostrophic Vorticity 200 points. 1. All labs are to be kept in a three hole binder. Turn in the binder when you have finished the Lab. 2. Show all work in mathematical

More information

DIRECTED NUMBERS ADDING AND SUBTRACTING DIRECTED NUMBERS

DIRECTED NUMBERS ADDING AND SUBTRACTING DIRECTED NUMBERS DIRECTED NUMBERS POSITIVE NUMBERS These are numbers such as: 3 which can be written as +3 46 which can be written as +46 14.67 which can be written as +14.67 a which can be written as +a RULE Any number

More information

Chapter 3- Energy Balance and Temperature

Chapter 3- Energy Balance and Temperature Chapter 3- Energy Balance and Temperature Understanding Weather and Climate Aguado and Burt Influences on Insolation Absorption Reflection/Scattering Transmission 1 Absorption An absorber gains energy

More information

Gaussian Quiz. Preamble to The Humble Gaussian Distribution. David MacKay 1

Gaussian Quiz. Preamble to The Humble Gaussian Distribution. David MacKay 1 Preamble to The Humble Gaussian Distribution. David MacKay Gaussian Quiz H y y y 3. Assuming that the variables y, y, y 3 in this belief network have a joint Gaussian distribution, which of the following

More information

THE OCEAN CARBON CYCLE

THE OCEAN CARBON CYCLE THE OCEAN CARBON CYCLE 21st February 2018 1 Box-model of the global ocean phosphorus, alkalinity, carbon 2 Pre-industrial model 3 Evolution during the industrial period 4 13 C isotopic evolution BOX-MODEL

More information

A look at synoptic CO2 in the midlatitudes and tropics using continuous CO2 observations and Transcom continuous results

A look at synoptic CO2 in the midlatitudes and tropics using continuous CO2 observations and Transcom continuous results A look at synoptic CO2 in the midlatitudes and tropics using continuous CO2 observations and Transcom continuous results Nicholas Parazoo Transcom 2008 June 2-5 Scales of Variation Diurnal Synoptic Seasonal

More information

Solutions Manual to Exercises for Weather & Climate, 8th ed. Appendix A Dimensions and Units 60 Appendix B Earth Measures 62 Appendix C GeoClock 63

Solutions Manual to Exercises for Weather & Climate, 8th ed. Appendix A Dimensions and Units 60 Appendix B Earth Measures 62 Appendix C GeoClock 63 Solutions Manual to Exercises for Weather & Climate, 8th ed. 1 Vertical Structure of the Atmosphere 1 2 Earth Sun Geometry 4 3 The Surface Energy Budget 8 4 The Global Energy Budget 10 5 Atmospheric Moisture

More information

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

The Atmosphere. Topic 3: Global Cycles and Physical Systems. Topic 3: Global Cycles and Physical Systems. Topic 3: Global Cycles and Physical Systems The Atmosphere 1 How big is the atmosphere? Why is it cold in Geneva? Why do mountaineers need oxygen on Everest? 2 A relatively thin layer of gas over the Earths surface Earth s radius ~ 6400km Atmospheric

More information

[Disclaimer: This is not a complete list of everything you need to know, just some of the topics that gave people difficulty.]

[Disclaimer: This is not a complete list of everything you need to know, just some of the topics that gave people difficulty.] Math 43 Review Notes [Disclaimer: This is not a complete list of everything you need to know, just some of the topics that gave people difficulty Dot Product If v (v, v, v 3 and w (w, w, w 3, then the

More information

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

Data and formulas at the end. Exam would be Weds. May 8, 2008 ATMS 321: Science of Climate Practice Mid Term Exam - Spring 2008 page 1 Atmospheric Sciences 321 Science of Climate Practice Mid-Term Examination: Would be Closed Book Data and formulas at the end. Exam

More information

Activity: The Atmosphere in the Vertical

Activity: The Atmosphere in the Vertical Activity: The Atmosphere in the Vertical Educational Outcomes: The atmosphere has thickness as well as horizontal extent. For a more complete understanding of weather, knowledge of atmospheric conditions

More information

TOPIC #12 NATURAL CLIMATIC FORCING

TOPIC #12 NATURAL CLIMATIC FORCING TOPIC #12 NATURAL CLIMATIC FORCING (Start on p 67 in Class Notes) p 67 ENERGY BALANCE (review) Global climate variability and change are caused by changes in the ENERGY BALANCE that are FORCED review FORCING

More information

Chapter 2 Earth s atmosphere (Lectures 4 and 5)

Chapter 2 Earth s atmosphere (Lectures 4 and 5) Chapter 2 Earth s atmosphere (Lectures 4 and 5) Keywords: Earth s atmosphere; International standard atmosphere; geopotential altitude; stability of atmosphere. Topics 2.1 Introduction 2.2 Earth s atmosphere

More information

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

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 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 Part A: Short Answer & Problems (12), Fill in the Blanks (6).

More information

Website Lecture 3 The Physical Environment Part 1

Website   Lecture 3 The Physical Environment Part 1 Website http://websites.rcc.edu/halama Lecture 3 The Physical Environment Part 1 1 Lectures 3 & 4 1. Biogeochemical Cycling 2. Solar Radiation 3. The Atmosphere 4. The Global Ocean 5. Weather and Climate

More information

Changes in Density Within An Air are Density Velocity Column Fixed due and/or With Respect to to Advection Divergence the Earth

Changes in Density Within An Air are Density Velocity Column Fixed due and/or With Respect to to Advection Divergence the Earth The Continuity Equation: Dines Compensation and the Pressure Tendency Equation 1. General The Continuity Equation is a restatement of the principle of Conservation of Mass applied to the atmosphere. The

More information

AN ALGEBRA PRIMER WITH A VIEW TOWARD CURVES OVER FINITE FIELDS

AN ALGEBRA PRIMER WITH A VIEW TOWARD CURVES OVER FINITE FIELDS AN ALGEBRA PRIMER WITH A VIEW TOWARD CURVES OVER FINITE FIELDS The integers are the set 1. Groups, Rings, and Fields: Basic Examples Z := {..., 3, 2, 1, 0, 1, 2, 3,...}, and we can add, subtract, and multiply

More information

Determining Fluxes of CO 2 using Mass Constraints

Determining Fluxes of CO 2 using Mass Constraints Determining Fluxes of CO 2 using Mass Constraints Paul O. Wennberg Gretchen Keppel-Aleks, Debra Wunch, Tapio Schneider Fluxes from variations in boundary layer CO2 Annual mean surface CO2 [ppm] Mixing

More information

Interhemispheric climate connections: What can the atmosphere do?

Interhemispheric climate connections: What can the atmosphere do? Interhemispheric climate connections: What can the atmosphere do? Raymond T. Pierrehumbert The University of Chicago 1 Uncertain feedbacks plague estimates of climate sensitivity 2 Water Vapor Models agree

More information

Carbon Flux Data Assimilation

Carbon Flux Data Assimilation Carbon Flux Data Assimilation Saroja Polavarapu Environment Canada Thanks: D. Jones (U Toronto), D. Chan (EC), A. Jacobson (NOAA) DAOS Working group Meeting, 15-16 Aug. 2014 The Global Carbon Cycle http://www.scidacreview.org/0703/html/biopilot.html

More information

Please bring the task to your first physics lesson and hand it to the teacher.

Please bring the task to your first physics lesson and hand it to the teacher. Pre-enrolment task for 2014 entry Physics Why do I need to complete a pre-enrolment task? This bridging pack serves a number of purposes. It gives you practice in some of the important skills you will

More information

Temperature (T) degrees Celsius ( o C) arbitrary scale from 0 o C at melting point of ice to 100 o C at boiling point of water Also (Kelvin, K) = o C

Temperature (T) degrees Celsius ( o C) arbitrary scale from 0 o C at melting point of ice to 100 o C at boiling point of water Also (Kelvin, K) = o C 1 2 3 4 Temperature (T) degrees Celsius ( o C) arbitrary scale from 0 o C at melting point of ice to 100 o C at boiling point of water Also (Kelvin, K) = o C plus 273.15 0 K is absolute zero, the minimum

More information

Ocean Constraints on the Atmospheric Inverse Problem: The contribution of Forward and Inverse Models

Ocean Constraints on the Atmospheric Inverse Problem: The contribution of Forward and Inverse Models Ocean Constraints on the Atmospheric Inverse Problem: The contribution of Forward and Inverse Models Nicolas Gruber Institute of Geophysics and Planetary Physics & Department of Atmospheric Sciences, University

More information

The linear additivity of the forcings' responses in the energy and water cycles. Nathalie Schaller, Jan Cermak, Reto Knutti and Martin Wild

The linear additivity of the forcings' responses in the energy and water cycles. Nathalie Schaller, Jan Cermak, Reto Knutti and Martin Wild The linear additivity of the forcings' responses in the energy and water cycles Nathalie Schaller, Jan Cermak, Reto Knutti and Martin Wild WCRP OSP, Denver, 27th October 2011 1 Motivation How will precipitation

More information

CHAPTER 1. MEASURES OF ATMOSPHERIC COMPOSITION

CHAPTER 1. MEASURES OF ATMOSPHERIC COMPOSITION 1 CHAPTER 1. MEASURES OF ATMOSPHERIC COMPOSITION The objective of atmospheric chemistry is to understand the factors that control the concentrations of chemical species in the atmosphere. In this book

More information

Understanding Global Environmental Trends and Projections. Ants Leetmaa Geophysical Fluid Dynamics Laboratory Princeton, NJ 08542

Understanding Global Environmental Trends and Projections. Ants Leetmaa Geophysical Fluid Dynamics Laboratory Princeton, NJ 08542 Understanding Global Environmental Trends and Projections Ants Leetmaa Geophysical Fluid Dynamics Laboratory Princeton, NJ 08542 Climate Scenarios Used for Attribution Studies of Climate Variability and

More information

Lecture 1. Equations of motion - Newton s second law in three dimensions. Pressure gradient + force force

Lecture 1. Equations of motion - Newton s second law in three dimensions. Pressure gradient + force force Lecture 3 Lecture 1 Basic dynamics Equations of motion - Newton s second law in three dimensions Acceleration = Pressure Coriolis + gravity + friction gradient + force force This set of equations is the

More information

Today s Lecture (Lecture 5): General circulation of the atmosphere

Today s Lecture (Lecture 5): General circulation of the atmosphere Climate Dynamics (Summer Semester 2017) J. Mülmenstädt Today s Lecture (Lecture 5): General circulation of the atmosphere Reference Hartmann, Global Physical Climatology (1994), Ch. 2, 3, 6 Peixoto and

More information

General Atmospheric Circulation

General Atmospheric Circulation General Atmospheric Circulation Take away Concepts and Ideas Global circulation: The mean meridional (N-S) circulation Trade winds and westerlies The Jet Stream Earth s climate zones Monsoonal climate

More information

PROBLEMS Sources of CO Sources of tropospheric ozone

PROBLEMS Sources of CO Sources of tropospheric ozone 220 PROBLEMS 11. 1 Sources of CO The two principal sources of CO to the atmosphere are oxidation of CH 4 and combustion. Mean rate constants for oxidation of CH 4 and CO by OH in the troposphere are k

More information

Lecture 10 March 15, 2010, Monday. Atmospheric Pressure & Wind: Part 1

Lecture 10 March 15, 2010, Monday. Atmospheric Pressure & Wind: Part 1 Lecture 10 March 15, 2010, Monday Atmospheric Pressure & Wind: Part 1 Speed, Velocity, Acceleration, Force, Pressure Atmospheric Pressure & Its Measurement Ideal Gas Law (Equation of State) Pressure Gradient

More information

Climate & Earth System Science. Introduction to Meteorology & Climate CHAPTER 1 LECTURE 1. Question: Introduction to the Atmosphere

Climate & Earth System Science. Introduction to Meteorology & Climate CHAPTER 1 LECTURE 1. Question: Introduction to the Atmosphere Climate & Earth System Science Introduction to Meteorology & Climate MAPH 10050 Peter Lynch Peter Lynch Meteorology & Climate Centre School of Mathematical Sciences University College Dublin Meteorology

More information

Lungs of the Planet with Dr. Michael Heithaus

Lungs of the Planet with Dr. Michael Heithaus Lungs of the Planet with Dr. Michael Heithaus Problem Why do people call rain forests the lungs of the planet? Usually it is because people think that the rain forests produce most of the oxygen we breathe.

More information

Lungs of the Planet. 1. Based on the equations above, describe how the processes of photosynthesis and cellular respiration relate to each other.

Lungs of the Planet. 1. Based on the equations above, describe how the processes of photosynthesis and cellular respiration relate to each other. Lungs of the Planet Name: Date: Why do people call rain forests the lungs of the planet? Usually it is because people think that the rain forests produce most of the oxygen we breathe. But do they? To

More information

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

Habitable Planets. Much of it stolen from. Yutaka ABE University of Tokyo Habitable Planets Much of it stolen from Yutaka ABE University of Tokyo 1. Habitability and Water Why water? Importance of Liquid Gas: highly mobile, but low material density. Solid: high density but very

More information

Dynamics of the Zonal-Mean, Time-Mean Tropical Circulation

Dynamics of the Zonal-Mean, Time-Mean Tropical Circulation Dynamics of the Zonal-Mean, Time-Mean Tropical Circulation First consider a hypothetical planet like Earth, but with no continents and no seasons and for which the only friction acting on the atmosphere

More information

WaVaCS summerschool Autumn 2009 Cargese, Corsica

WaVaCS summerschool Autumn 2009 Cargese, Corsica Introduction Part I WaVaCS summerschool Autumn 2009 Cargese, Corsica Holger Tost Max Planck Institute for Chemistry, Mainz, Germany Introduction Overview What is a parameterisation and why using it? Fundamentals

More information

Estimating Regional Sources and Sinks of CO 2 Using GOSAT XCO 2

Estimating Regional Sources and Sinks of CO 2 Using GOSAT XCO 2 Estimating Regional Sources and Sinks of CO 2 Using GOSAT XCO 2 Feng Deng Dylan Jones Daven Henze Nicolas Bousserez Kevin Bowman Joshua Fisher Ray Nassar IWGGMS-9 YokohamaJapan May 2013 1 XCO 2 Observations

More information

The Transfer of Heat

The Transfer of Heat The Transfer of Heat Outcomes: S2-4-03 Explain effects of heat transfer within the atmosphere and hydrosphere on the development and movement of wind and ocean currents. Coriolis Effect In our ecology

More information

Clouds and Rain Unit (3 pts)

Clouds and Rain Unit (3 pts) Name: Section: Clouds and Rain Unit (Topic 8A-2) page 1 Clouds and Rain Unit (3 pts) As air rises, it cools due to the reduction in atmospheric pressure Air mainly consists of oxygen molecules and nitrogen

More information

Atmospheric Thermodynamics

Atmospheric Thermodynamics Atmospheric Thermodynamics Atmospheric Composition What is the composition of the Earth s atmosphere? Gaseous Constituents of the Earth s atmosphere (dry air) Constituent Molecular Weight Fractional Concentration

More information

MAR 110 LECTURE #9 Earth s Heat Budget / Atmosphere Dynamics

MAR 110 LECTURE #9 Earth s Heat Budget / Atmosphere Dynamics MAR 110: Lecture 9 Outline Heat Budget / Atmosphere Dynamics 1 MAR 110 LECTURE #9 Earth s Heat Budget / Atmosphere Dynamics External Energy Source-the Sun The portion of the sun s energy that is intercepted

More information

Linear Algebra, Summer 2011, pt. 2

Linear Algebra, Summer 2011, pt. 2 Linear Algebra, Summer 2, pt. 2 June 8, 2 Contents Inverses. 2 Vector Spaces. 3 2. Examples of vector spaces..................... 3 2.2 The column space......................... 6 2.3 The null space...........................

More information

USING PROGRAM HURRICANE. Download all the files, including the (empty) output subdirectory into a new folder on your machine.

USING PROGRAM HURRICANE. Download all the files, including the (empty) output subdirectory into a new folder on your machine. USING PROGRAM HURRICANE Download all the files, including the (empty) output subdirectory into a new folder on your machine. QuickStart: First compile hurr.f. Modify the first column of the input file

More information

ATM S 111, Global Warming Climate Models

ATM S 111, Global Warming Climate Models ATM S 111, Global Warming Climate Models Jennifer Fletcher Day 27: July 29, 2010 Using Climate Models to Build Understanding Often climate models are thought of as forecast tools (what s the climate going

More information

Current Status of COMS AMV in NMSC/KMA

Current Status of COMS AMV in NMSC/KMA Current Status of COMS AMV in NMSC/KMA Eunha Sohn, Sung-Rae Chung, Jong-Seo Park Satellite Analysis Division, NMSC/KMA soneh0431@korea.kr COMS AMV of KMA/NMSC has been produced hourly since April 1, 2011.

More information

7 The General Circulation

7 The General Circulation 7 The General Circulation 7.1 The axisymmetric state At the beginning of the class, we discussed the nonlinear, inviscid, axisymmetric theory of the meridional structure of the atmosphere. The important

More information

Section 20: Arrow Diagrams on the Integers

Section 20: Arrow Diagrams on the Integers Section 0: Arrow Diagrams on the Integers Most of the material we have discussed so far concerns the idea and representations of functions. A function is a relationship between a set of inputs (the leave

More information

Page 1. Name:

Page 1. Name: Name: 1) As the difference between the dewpoint temperature and the air temperature decreases, the probability of precipitation increases remains the same decreases 2) Which statement best explains why

More information

P3.11 A COMPARISON OF AN ENSEMBLE OF POSITIVE/NEGATIVE PAIRS AND A CENTERED SPHERICAL SIMPLEX ENSEMBLE

P3.11 A COMPARISON OF AN ENSEMBLE OF POSITIVE/NEGATIVE PAIRS AND A CENTERED SPHERICAL SIMPLEX ENSEMBLE P3.11 A COMPARISON OF AN ENSEMBLE OF POSITIVE/NEGATIVE PAIRS AND A CENTERED SPHERICAL SIMPLEX ENSEMBLE 1 INTRODUCTION Xuguang Wang* The Pennsylvania State University, University Park, PA Craig H. Bishop

More information

MATRIX DETERMINANTS. 1 Reminder Definition and components of a matrix

MATRIX DETERMINANTS. 1 Reminder Definition and components of a matrix MATRIX DETERMINANTS Summary Uses... 1 1 Reminder Definition and components of a matrix... 1 2 The matrix determinant... 2 3 Calculation of the determinant for a matrix... 2 4 Exercise... 3 5 Definition

More information

A global modeler looks at regional climate modeling. Zippy:Regional_Climate_01:Regional_Climate_01.frame

A global modeler looks at regional climate modeling. Zippy:Regional_Climate_01:Regional_Climate_01.frame A global modeler looks at regional climate modeling I come in peace. Global climate models, 1 All global climate models must include representations of the ocean, sea ice, and the vegetated land surface,

More information

Thickness of the Atmosphere

Thickness of the Atmosphere Lecture 1: A Brief Survey of the Atmosphere Origins of the atmosphere Vertical structure of composition Vertical structure of air pressure Vertical structure of temperature The ionosphere Thickness of

More information

Introduction to Climate ~ Part I ~

Introduction to Climate ~ Part I ~ 2015/11/16 TCC Seminar JMA Introduction to Climate ~ Part I ~ Shuhei MAEDA (MRI/JMA) Climate Research Department Meteorological Research Institute (MRI/JMA) 1 Outline of the lecture 1. Climate System (

More information

Chemical Reaction Engineering Prof. Jayant Modak Department of Chemical Engineering Indian Institute of Science, Bangalore

Chemical Reaction Engineering Prof. Jayant Modak Department of Chemical Engineering Indian Institute of Science, Bangalore Chemical Reaction Engineering Prof. Jayant Modak Department of Chemical Engineering Indian Institute of Science, Bangalore Lecture No. #40 Problem solving: Reactor Design Friends, this is our last session

More information

Lecture 1. Amplitude of the seasonal cycle in temperature

Lecture 1. Amplitude of the seasonal cycle in temperature Lecture 6 Lecture 1 Ocean circulation Forcing and large-scale features Amplitude of the seasonal cycle in temperature 1 Atmosphere and ocean heat transport Trenberth and Caron (2001) False-colour satellite

More information