Lecture 20 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY

Size: px
Start display at page:

Download "Lecture 20 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY"

Transcription

1 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY Lecture 20 Learning objectives: should be able to apply mixed layer temperature equation to explain observations; understand buoyancy forcing & salinity budget 1. Mixed layer temperature equation: cold tongue formation, etc.; 2. Ocean surface salinity budget; 3. Ocean surface buoyancy flux.

2 z Previous class: x Unit:

3 Previous class: mixed layer temperature equation: H(w) step function; 1 for w>0; 0 for w 0. Positive: into the ocean.

4 Horizontal advection w T m T d h m It includes the effects of both upwelling & entrainment cooling. Entrainment: turbulent mixing effect that entrains water from the thermocline into the surface mixed layer. Upwelling: vertical advection due to surface mass divergence; it involves isotherms tilting upward

5 In the above equations: c pd = 1004J/kg/ C is specific heat of air; C DE is close to C DH under ordinary conditions. Va is 10m wind speed, Vo us oceanic surface current in the wind direction, Ta us surface air temperature, and To is SST and is Tm if the surface layer is well mixed. Llv = J/kg is latent heat of evaporation. q va is surface air humidity, and q vo is saturation specific humidity when Ta = To. C P = 4186 J/(kg C) (at 15 C, kpa) Note: potential temperatures should be used but at the oceanic surface, potential temperature is equivalent to in situ temperature so people often use T instead of θ.

6 In a surface mixed layer model, however, the effects of entrainment and upwelling can not be separated, and their effects present in one term: the last term in the following equation. T m t = Q net ρ w c pw h m! V m T m w (T m T d ) h m Where Q net = Q nr +Q s +Q l +Q pr and w = ( h t +! V h m + w hm ) w hm is the upwelling velocity (Ekman pumping velocity). It is this equation that is used to calculate mixed layer heat budget in many research studies.

7 Questions (1)When wind speed reduces, the ocean increases or decreases its heat loss? Through what possible processes? (2) When SST is colder, does the ocean increase Or decrease heat loss? Why? (3) Both upwelling and entrainment can cool the SST; physically, what s the major difference between the two processes?

8 1: Cold tongue: TAO data in the eastern Pacific: Color: SST; black arrow: winds;white arrow: Ekman transport Cold tongue: has an annual cycle

9 (1) Upwelling & entrainment: w (T m T d ) h m (2) Advection: Zonal and meridional (air/sea interaction: enhance cold tongue) (3) Qsw: shortwave flux/stratus cloud, cools SST; (Ql, wind-evaporative effect plays minor role) (4) Eddy heat transport - diffusion (Swenson & Hansen, 1999: JPO)

10 Mean SST and (a) Mean SST+wind surface wind USA Fig. 1. (a)observed long-term mea surface temperature (SST; color c (b) Linear trend of satellite observ (color contour) for the SST trends below 90% significanc (c) Linear trend of satellite observ period, with global mea areas show SSH trend below 90% Question: (b) trend: SST&wind (c) trend: SSH (1)For an intensified surface wind pattern, will US west coast become colder or warmer? Through what USA processes? (2)How about sea level?

11 2. Ocean Surface salinity budget: [4] Marine species of upper ocean Importance: ocean s rain gauge: an indicator of global hydrological cycle

12 Importance: In the coupled climate system, salinity is also an indicator of global hydrological cycle Satellite: sea salinity mission June 2011 A Delta II rocket launches with the Aquarius/SAC-D spacecraft payload from Space Launch Complex 2 at Vandenberg Air Force Base, Calif. - Image credit: NASA/Bill Ingalls

13 E-P ( Aquarius Salinity

14 Ocean surface salinity budget (for a water parcel)

15 z y P E R Sea ice x entrainment Salt: ρ w h m ΔxΔy S m, Salt change: ρ w h m ΔxΔy ds m dt

16

17 S m t = ρ r Ṗr S m ρ s Ṗs S m + ρ w Ė 0 S m ρ rv Ṙ S m + ρ i dh i dt (S m S i ) ρ w h m! V S m w S m S d h m

18 Processes for local (Eularian) salinity change: (1) Precipitation (rain or snow); P (2) Evaporation; E (3) River runoff; R (4) Sea ice freezing/melting; (5) Horizontal advection; (6) Entrainment & Upwelling. P-E plays a deterministic role in open ocean; R can be important in coastal regions where river discharge is large; Sea ice: important in high latitude: say arctic ocean; Advection, entrainment, upwelling can be important in any regions.

19

20 E-P (solid) and salinity (dashed)

21 3. Ocean surface buoyancy flux ( )

ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY. Lecture 19. Learning objectives: develop a physical understanding of ocean thermodynamic processes

ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY. Lecture 19. Learning objectives: develop a physical understanding of ocean thermodynamic processes ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY Lecture 19 Learning objectives: develop a physical understanding of ocean thermodynamic processes 1. Ocean surface heat fluxes; 2. Mixed layer temperature

More information

Chapter 7: Thermodynamics

Chapter 7: Thermodynamics Chapter 7: Thermodynamics 7.1 Sea surface heat budget In Chapter 5, we have introduced the oceanic planetary boundary layer-the Ekman layer. The observed T and S in this layer are almost uniform vertically,

More information

C

C C 0.8 0.4 0.2 0.0-0.2-0.6 Fig. 1. SST-wind relation in the North Pacific and Atlantic Oceans. Left panel: COADS SST (color shade), surface wind vectors, and SLP regressed upon the Pacific Decadal Oscillation

More information

The Ocean-Atmosphere System II: Oceanic Heat Budget

The Ocean-Atmosphere System II: Oceanic Heat Budget The Ocean-Atmosphere System II: Oceanic Heat Budget C. Chen General Physical Oceanography MAR 555 School for Marine Sciences and Technology Umass-Dartmouth MAR 555 Lecture 2: The Oceanic Heat Budget Q

More information

( ) = 1005 J kg 1 K 1 ;

( ) = 1005 J kg 1 K 1 ; Problem Set 3 1. A parcel of water is added to the ocean surface that is denser (heavier) than any of the waters in the ocean. Suppose the parcel sinks to the ocean bottom; estimate the change in temperature

More information

SIO 210 Final examination Wednesday, December 12, :30-2:30 Eckart 227 Name:

SIO 210 Final examination Wednesday, December 12, :30-2:30 Eckart 227 Name: SIO 210 Final examination Wednesday, December 12, 2018 11:30-2:30 Eckart 227 Name: Please put your initials or name on each page, especially if you pull pages apart. Turn off all phones, ipods, etc. and

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

Ocean Mixing and Climate Change

Ocean Mixing and Climate Change Ocean Mixing and Climate Change Factors inducing seawater mixing Different densities Wind stirring Internal waves breaking Tidal Bottom topography Biogenic Mixing (??) In general, any motion favoring turbulent

More information

Upper Ocean Circulation

Upper Ocean Circulation Upper Ocean Circulation C. Chen General Physical Oceanography MAR 555 School for Marine Sciences and Technology Umass-Dartmouth 1 MAR555 Lecture 4: The Upper Oceanic Circulation The Oceanic Circulation

More information

An Introduction to Coupled Models of the Atmosphere Ocean System

An Introduction to Coupled Models of the Atmosphere Ocean System An Introduction to Coupled Models of the Atmosphere Ocean System Jonathon S. Wright jswright@tsinghua.edu.cn Atmosphere Ocean Coupling 1. Important to climate on a wide range of time scales Diurnal to

More information

OCN/ATM/ESS 587. Ocean circulation, dynamics and thermodynamics.

OCN/ATM/ESS 587. Ocean circulation, dynamics and thermodynamics. OCN/ATM/ESS 587 Ocean circulation, dynamics and thermodynamics. Equation of state for seawater General T/S properties of the upper ocean Heat balance of the upper ocean Upper ocean circulation Deep circulation

More information

The Atmospheric Boundary Layer. The Surface Energy Balance (9.2)

The Atmospheric Boundary Layer. The Surface Energy Balance (9.2) The Atmospheric Boundary Layer Turbulence (9.1) The Surface Energy Balance (9.2) Vertical Structure (9.3) Evolution (9.4) Special Effects (9.5) The Boundary Layer in Context (9.6) What processes control

More information

Lecture 17 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY. Learning objectives: understand the concepts & physics of

Lecture 17 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY. Learning objectives: understand the concepts & physics of ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY Lecture 17 Learning objectives: understand the concepts & physics of 1. Ekman layer 2. Ekman transport 3. Ekman pumping 1. The Ekman Layer Scale analyses

More information

Atmospheric Sciences 321. Science of Climate. Lecture 20: More Ocean: Chapter 7

Atmospheric Sciences 321. Science of Climate. Lecture 20: More Ocean: Chapter 7 Atmospheric Sciences 321 Science of Climate Lecture 20: More Ocean: Chapter 7 Community Business Quiz discussion Next Topic will be Chapter 8, Natural Climate variability in the instrumental record. Homework

More information

The Arctic Energy Budget

The Arctic Energy Budget The Arctic Energy Budget The global heat engine [courtesy Kevin Trenberth, NCAR]. Differential solar heating between low and high latitudes gives rise to a circulation of the atmosphere and ocean that

More information

Fast and Slow Response of Sea ice and the Southern Ocean to Ozone Depletion

Fast and Slow Response of Sea ice and the Southern Ocean to Ozone Depletion Fast and Slow Response of Sea ice and the Southern Ocean to Ozone Depletion Annual Minimum Sea ice extent 1979-2013 10 6 km 2 Arctic September Antarctic February Data from in passive microwave satellite

More information

Atmospheric Sciences 321. Science of Climate. Lecture 14: Surface Energy Balance Chapter 4

Atmospheric Sciences 321. Science of Climate. Lecture 14: Surface Energy Balance Chapter 4 Atmospheric Sciences 321 Science of Climate Lecture 14: Surface Energy Balance Chapter 4 Community Business Check the assignments HW #4 due Today, HW#5 is posted Quiz Today on Chapter 3, too. Mid Term

More information

The World Ocean. Pacific Ocean 181 x 10 6 km 2. Indian Ocean 74 x 10 6 km 2. Atlantic Ocean 106 x 10 6 km 2

The World Ocean. Pacific Ocean 181 x 10 6 km 2. Indian Ocean 74 x 10 6 km 2. Atlantic Ocean 106 x 10 6 km 2 The World Ocean The ocean and adjacent seas cover 70.8% of the surface of Earth, an area of 361,254,000 km 2 Pacific Ocean 181 x 10 6 km 2 Indian Ocean 74 x 10 6 km 2 Atlantic Ocean 106 x 10 6 km 2 Oceanic

More information

isopycnal outcrop w < 0 (downwelling), v < 0 L.I. V. P.

isopycnal outcrop w < 0 (downwelling), v < 0 L.I. V. P. Ocean 423 Vertical circulation 1 When we are thinking about how the density, temperature and salinity structure is set in the ocean, there are different processes at work depending on where in the water

More information

Air-Sea Coupling in an Eastern Boundary Current Region

Air-Sea Coupling in an Eastern Boundary Current Region Air-Sea Coupling in an Eastern Boundary Current Region Eric D. Skyllingstad CEOAS, Oregon State University Roger M. Samelson D. B. Chelton, A. Kurapov CEOAS, Oregon State University N. Perlin RSMAS, University

More information

Lab 12: El Nino Southern Oscillation

Lab 12: El Nino Southern Oscillation Name: Date: OCN 104: Our Dynamic Ocean Lab 12: El Nino Southern Oscillation Part 1: Observations of the tropical Pacific Ocean during a normal year The National Oceanographic and Atmospheric Administration

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

Ocean Dynamics. The Great Wave off Kanagawa Hokusai

Ocean Dynamics. The Great Wave off Kanagawa Hokusai Ocean Dynamics The Great Wave off Kanagawa Hokusai LO: integrate relevant oceanographic processes with factors influencing survival and growth of fish larvae Physics Determining Ocean Dynamics 1. Conservation

More information

5. General Circulation Models

5. General Circulation Models 5. General Circulation Models I. 3-D Climate Models (General Circulation Models) To include the full three-dimensional aspect of climate, including the calculation of the dynamical transports, requires

More information

MAR 110 LECTURE #10 The Oceanic Conveyor Belt Oceanic Thermohaline Circulation

MAR 110 LECTURE #10 The Oceanic Conveyor Belt Oceanic Thermohaline Circulation 1 MAR 110 LECTURE #10 The Oceanic Conveyor Belt Oceanic Thermohaline Circulation Ocean Climate Temperature Zones The pattern of approximately parallel oceanic surface isotherms (lines of constant temperature)

More information

Lecture 8. Lecture 1. Wind-driven gyres. Ekman transport and Ekman pumping in a typical ocean basin. VEk

Lecture 8. Lecture 1. Wind-driven gyres. Ekman transport and Ekman pumping in a typical ocean basin. VEk Lecture 8 Lecture 1 Wind-driven gyres Ekman transport and Ekman pumping in a typical ocean basin. VEk wek > 0 VEk wek < 0 VEk 1 8.1 Vorticity and circulation The vorticity of a parcel is a measure of its

More information

Decadal variability in the Kuroshio and Oyashio Extension frontal regions in an eddy-resolving OGCM

Decadal variability in the Kuroshio and Oyashio Extension frontal regions in an eddy-resolving OGCM Decadal variability in the Kuroshio and Oyashio Extension frontal regions in an eddy-resolving OGCM Masami Nonaka 1, Hisashi Nakamura 1,2, Youichi Tanimoto 1,3, Takashi Kagimoto 1, and Hideharu Sasaki

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

Ocean Circulation. In partnership with Dr. Zafer Top

Ocean Circulation. In partnership with Dr. Zafer Top Ocean Circulation In partnership with Dr. Zafer Top Samantha Hampton Honors Science December 15, 2014 Ocean Circulation is the large scale movement of waters in the ocean basins. Dr. Zafer Top studies

More information

SD 13: The Indian Ocean s Influence on Regional Hydroclimate

SD 13: The Indian Ocean s Influence on Regional Hydroclimate SD 13: The Indian Ocean s Influence on Regional Hydroclimate Caroline C. Ummenhofer, WHOI, USA NASA (2015) Halosteric component of ITF transport Felton et al. (2014) Hu & Sprintall (2017) Variability in

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Figure S1. Summary of the climatic responses to the Gulf Stream. On the offshore flank of the SST front (black dashed curve) of the Gulf Stream (green long arrow), surface wind convergence associated with

More information

SIO 210 Final examination Answer Key for all questions except Daisyworld. Wednesday, December 10, PM Name:

SIO 210 Final examination Answer Key for all questions except Daisyworld. Wednesday, December 10, PM Name: SIO 210 Final examination Answer Key for all questions except Daisyworld. Wednesday, December 10, 2008 3-6 PM Name: This is a closed book exam. You may use a calculator. There are two parts: Talley (weighted

More information

What you need to know in Ch. 12. Lecture Ch. 12. Atmospheric Heat Engine. The Atmospheric Heat Engine. Atmospheric Heat Engine

What you need to know in Ch. 12. Lecture Ch. 12. Atmospheric Heat Engine. The Atmospheric Heat Engine. Atmospheric Heat Engine Lecture Ch. 1 Review of simplified climate model Revisiting: Kiehl and Trenberth Overview of atmospheric heat engine Current research on clouds-climate Curry and Webster, Ch. 1 For Wednesday: Read Ch.

More information

1 Introduction to Governing Equations 2 1a Methodology... 2

1 Introduction to Governing Equations 2 1a Methodology... 2 Contents 1 Introduction to Governing Equations 2 1a Methodology............................ 2 2 Equation of State 2 2a Mean and Turbulent Parts...................... 3 2b Reynolds Averaging.........................

More information

What you need to know in Ch. 12. Lecture Ch. 12. Atmospheric Heat Engine

What you need to know in Ch. 12. Lecture Ch. 12. Atmospheric Heat Engine Lecture Ch. 12 Review of simplified climate model Revisiting: Kiehl and Trenberth Overview of atmospheric heat engine Current research on clouds-climate Curry and Webster, Ch. 12 For Wednesday: Read Ch.

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

Warm Up Vocabulary Check

Warm Up Vocabulary Check Warm Up Vocabulary Check Surface current Coriolis Effect global winds upwelling Gulf Stream deep current climate El Nino convection current continental deflection 1.The apparent curving of the path of

More information

Chapter 2 Solar and Infrared Radiation

Chapter 2 Solar and Infrared Radiation Chapter 2 Solar and Infrared Radiation Chapter overview: Fluxes Energy transfer Seasonal and daily changes in radiation Surface radiation budget Fluxes Flux (F): The transfer of a quantity per unit area

More information

3. Midlatitude Storm Tracks and the North Atlantic Oscillation

3. Midlatitude Storm Tracks and the North Atlantic Oscillation 3. Midlatitude Storm Tracks and the North Atlantic Oscillation Copyright 2006 Emily Shuckburgh, University of Cambridge. Not to be quoted or reproduced without permission. EFS 3/1 Review of key results

More information

Radiative-Convective Models. The Hydrological Cycle Hadley Circulation. Manabe and Strickler (1964) Course Notes chapter 5.1

Radiative-Convective Models. The Hydrological Cycle Hadley Circulation. Manabe and Strickler (1964) Course Notes chapter 5.1 Climate Modeling Lecture 8 Radiative-Convective Models Manabe and Strickler (1964) Course Notes chapter 5.1 The Hydrological Cycle Hadley Circulation Prepare for Mid-Term (Friday 9 am) Review Course Notes

More information

Ocean dynamics: the wind-driven circulation

Ocean dynamics: the wind-driven circulation Ocean dynamics: the wind-driven circulation Weston Anderson March 13, 2017 Contents 1 Introduction 1 2 The wind driven circulation (Ekman Transport) 3 3 Sverdrup flow 5 4 Western boundary currents (western

More information

SIO 210 Problem Set 2 October 17, 2011 Due Oct. 24, 2011

SIO 210 Problem Set 2 October 17, 2011 Due Oct. 24, 2011 SIO 210 Problem Set 2 October 17, 2011 Due Oct. 24, 2011 1. The Pacific Ocean is approximately 10,000 km wide. Its upper layer (wind-driven gyre*) is approximately 1,000 m deep. Consider a west-to-east

More information

ATS 421/521. Climate Modeling. Spring 2015

ATS 421/521. Climate Modeling. Spring 2015 ATS 421/521 Climate Modeling Spring 2015 Lecture 9 Hadley Circulation (Held and Hou, 1980) General Circulation Models (tetbook chapter 3.2.3; course notes chapter 5.3) The Primitive Equations (tetbook

More information

Interannual variability of top-ofatmosphere. CERES instruments

Interannual variability of top-ofatmosphere. CERES instruments Interannual variability of top-ofatmosphere albedo observed by CERES instruments Seiji Kato NASA Langley Research Center Hampton, VA SORCE Science team meeting, Sedona, Arizona, Sep. 13-16, 2011 TOA irradiance

More information

Energy transport and transfer in the wake of a tropical cyclone

Energy transport and transfer in the wake of a tropical cyclone Energy transport and transfer in the wake of a tropical cyclone Claudia Pasquero Department of Earth and Environmental Sciences Università degli Studi di Milano - Bicocca Agostino Meroni, Francesco Ragone

More information

Tropical Pacific responses to Neogene Andean uplift and highlatitude. Ran Feng and Chris Poulsen University of Michigan

Tropical Pacific responses to Neogene Andean uplift and highlatitude. Ran Feng and Chris Poulsen University of Michigan Tropical Pacific responses to Neogene Andean uplift and highlatitude sea ice expansion Ran Feng and Chris Poulsen University of Michigan Reconstructions of Neogene equatorial Pacific SSTs SST difference

More information

What is a system? What do the arrows in this diagram represent? What do the boxes represent? Why is it useful to study and understand systems?

What is a system? What do the arrows in this diagram represent? What do the boxes represent? Why is it useful to study and understand systems? Systems What is a system? What do the arrows in this diagram represent? What do the boxes represent? Why is it useful to study and understand systems? evaporation River & Lake water rain Atmosphere Water

More information

Lecture 3 questions Temperature, Salinity, Density and Circulation

Lecture 3 questions Temperature, Salinity, Density and Circulation Lecture 3 questions Temperature, Salinity, Density and Circulation (1) These are profiles of mean ocean temperature with depth at various locations in the ocean which in the following (a, b, c) figures

More information

Link between Hurricanes and Climate Change: SST

Link between Hurricanes and Climate Change: SST Link between Hurricanes and Climate Change: SST FRIDAY: PROJECT 2 Proposals due! Bring laptops on weds (at least one per group)! Discuss assessment on Weds. Roger Francois will talk on Friday about the

More information

The Hydrologic Cycle

The Hydrologic Cycle The Hydrologic Cycle Monthly precipitation for the central Arctic Ocean based on data from the Russian North Pole manned camps with daily bias adjustments. Raw precipitation totals are shown along with

More information

SIO 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes

SIO 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes NAME: SIO 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes Closed book; one sheet of your own notes is allowed. A calculator is allowed. (100 total points.)

More information

psio 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes Answer key

psio 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes Answer key NAME: psio 210 Introduction to Physical Oceanography Mid-term examination November 3, 2014; 1 hour 20 minutes Answer key Closed book; one sheet of your own notes is allowed. A calculator is allowed. (100

More information

ESCI 485 Air/sea Interaction Lesson 5 Oceanic Boundary Layer

ESCI 485 Air/sea Interaction Lesson 5 Oceanic Boundary Layer ESCI 485 Air/sea Interaction Lesson 5 Oceanic Boundar Laer References: Descriptive Phsical Oceanograph, Pickard and Emer Introductor Dnamical Oceanograph, Pond and Pickard Principles of Ocean Phsics, Apel

More information

Name Date Class. well as the inland, found near the Tropics. 4. In the, or the regions near the Equator, you may find a lush

Name Date Class. well as the inland, found near the Tropics. 4. In the, or the regions near the Equator, you may find a lush WATER, CLIMATE, AND VEGETATION Vocabulary Activity DIRECTIONS: Fill in the Blanks Select a term from below to complete each of the following sentences. CHAPTER 1. The constant movement of water, a process

More information

Homework 5: Background Ocean Water Properties & Stratification

Homework 5: Background Ocean Water Properties & Stratification 14 August 2008 MAR 110 HW5: Ocean Properties 1 Homework 5: Background Ocean Water Properties & Stratification The ocean is a heterogeneous mixture of water types - each with its own temperature, salinity,

More information

CHAPTER 2 - ATMOSPHERIC CIRCULATION & AIR/SEA INTERACTION

CHAPTER 2 - ATMOSPHERIC CIRCULATION & AIR/SEA INTERACTION Chapter 2 - pg. 1 CHAPTER 2 - ATMOSPHERIC CIRCULATION & AIR/SEA INTERACTION The atmosphere is driven by the variations of solar heating with latitude. The heat is transferred to the air by direct absorption

More information

HYCOM Caspian Sea Modeling. Part I: An Overview of the Model and Coastal Upwelling. Naval Research Laboratory, Stennis Space Center, USA

HYCOM Caspian Sea Modeling. Part I: An Overview of the Model and Coastal Upwelling. Naval Research Laboratory, Stennis Space Center, USA HYCOM Caspian Sea Modeling. Part I: An Overview of the Model and Coastal Upwelling By BIROL KARA, ALAN WALLCRAFT AND JOE METZGER Naval Research Laboratory, Stennis Space Center, USA MURAT GUNDUZ Institute

More information

Ocean Circulation Influences on Sea Surface Temperature in the Equatorial Central Pacific

Ocean Circulation Influences on Sea Surface Temperature in the Equatorial Central Pacific University of South Florida Scholar Commons Marine Science Faculty Publications College of Marine Science 9-15-001 Ocean Circulation Influences on Sea Surface Temperature in the Equatorial Central Pacific

More information

Role of Horizontal Density Advection in Seasonal Deepening of the Mixed Layer in the Subtropical Southeast Pacific

Role of Horizontal Density Advection in Seasonal Deepening of the Mixed Layer in the Subtropical Southeast Pacific ADVANCES IN ATMOSPHERIC SCIENCES, VOL. 33, APRIL 2016, 442 451 Role of Horizontal Density Advection in Seasonal Deepening of the Mixed Layer in the Subtropical Southeast Pacific Qinyu LIU and Yiqun LU

More information

Energy Systems, Structures and Processes Essential Standard: Analyze patterns of global climate change over time Learning Objective: Differentiate

Energy Systems, Structures and Processes Essential Standard: Analyze patterns of global climate change over time Learning Objective: Differentiate Energy Systems, Structures and Processes Essential Standard: Analyze patterns of global climate change over time Learning Objective: Differentiate between weather and climate Global Climate Focus Question

More information

For example, for values of A x = 0 m /s, f 0 s, and L = 0 km, then E h = 0. and the motion may be influenced by horizontal friction if Corioli

For example, for values of A x = 0 m /s, f 0 s, and L = 0 km, then E h = 0. and the motion may be influenced by horizontal friction if Corioli Lecture. Equations of Motion Scaling, Non-dimensional Numbers, Stability and Mixing We have learned how to express the forces per unit mass that cause acceleration in the ocean, except for the tidal forces

More information

SIO 210 Final Exam December 10, :30 2:30 NTV 330 No books, no notes. Calculators can be used.

SIO 210 Final Exam December 10, :30 2:30 NTV 330 No books, no notes. Calculators can be used. SIO 210 Final Exam December 10, 2003 11:30 2:30 NTV 330 No books, no notes. Calculators can be used. There are three sections to the exam: multiple choice, short answer, and long problems. Points are given

More information

Transient and Eddy. Transient/Eddy Flux. Flux Components. Lecture 3: Weather/Disturbance. Transient: deviations from time mean Time Mean

Transient and Eddy. Transient/Eddy Flux. Flux Components. Lecture 3: Weather/Disturbance. Transient: deviations from time mean Time Mean Lecture 3: Weather/Disturbance Transients and Eddies Climate Roles Mid-Latitude Cyclones Tropical Hurricanes Mid-Ocean Eddies Transient and Eddy Transient: deviations from time mean Time Mean Eddy: deviations

More information

Pacific Storm Track at Different Horizontal Resolutions Snap-shot of Column Liquid Water Content

Pacific Storm Track at Different Horizontal Resolutions Snap-shot of Column Liquid Water Content Color Plates Pacific Storm Track at Different Horizontal Resolutions Snap-shot of Column Liquid Water Content Fig. 2.8 A snapshot of the cyclone frontal-system by a nonhydrostatic model run with two very

More information

Version2 Fall True/False Indicate whether the sentence or statement is true or false.

Version2 Fall True/False Indicate whether the sentence or statement is true or false. Version2 Fall 2004 True/False Indicate whether the sentence or statement is true or false. 1. Short residence time elements are found in the greatest concentration near their point of removal from the

More information

Léo Siqueira Ph.D. Meteorology and Physical Oceanography

Léo Siqueira Ph.D. Meteorology and Physical Oceanography Léo Siqueira Ph.D. Meteorology and Physical Oceanography Modular Ocean Model (Griffies 2009) from GFDL version MOM4p1: Includes the Sea Ice Simulator (SIS) built-in ice model (Winton 2000). Includes TOPAZ

More information

Forecasting. Theory Types Examples

Forecasting. Theory Types Examples Forecasting Theory Types Examples How Good Are Week Out Weather Forecasts? For forecasts greater than nine days out, weather forecasters do WORSE than the climate average forecast. Why is there predictability

More information

Salinity Processes in the Upper. Ocean Regional Study (SPURS) Ray Schmitt, WHOI

Salinity Processes in the Upper. Ocean Regional Study (SPURS) Ray Schmitt, WHOI Salinity Processes in the Upper Outgrowth of: Ocean Regional Study (SPURS) Ray Schmitt, WHOI CLIVAR Salinity Working Group (May 06 meeting and 07 report) Salinity issue of Oceanography (Mar. 08) NASA Workshop

More information

Capabilities of Ocean Mixed Layer Models

Capabilities of Ocean Mixed Layer Models Capabilities of Ocean Mixed Layer Models W.G. Large National Center for Atmospheric Research Boulder Co, USA 1. Introduction The capabilities expected in today s state of the art models of the ocean s

More information

Large-Eddy Simulations of Tropical Convective Systems, the Boundary Layer, and Upper Ocean Coupling

Large-Eddy Simulations of Tropical Convective Systems, the Boundary Layer, and Upper Ocean Coupling DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Large-Eddy Simulations of Tropical Convective Systems, the Boundary Layer, and Upper Ocean Coupling Eric D. Skyllingstad

More information

ESS15 Lecture 13. End of the oceans (tropical / El Nino, thermohaline circulation) Weather vs. climate.

ESS15 Lecture 13. End of the oceans (tropical / El Nino, thermohaline circulation) Weather vs. climate. ESS15 Lecture 13 End of the oceans (tropical / El Nino, thermohaline circulation) Weather vs. climate. Please give me feedback through the EEE midterm evaluation survey. I promise to adapt to it. Review

More information

Water mass formation, subduction, and the oceanic heat budget

Water mass formation, subduction, and the oceanic heat budget Chapter 5 Water mass formation, subduction, and the oceanic heat budget In the first four chapters we developed the concept of Ekman pumping, Rossby wave propagation, and the Sverdrup circulation as the

More information

The atmospheric boundary layer: Where the atmosphere meets the surface. The atmospheric boundary layer:

The atmospheric boundary layer: Where the atmosphere meets the surface. The atmospheric boundary layer: The atmospheric boundary layer: Utrecht Summer School on Physics of the Climate System Carleen Tijm-Reijmer IMAU The atmospheric boundary layer: Where the atmosphere meets the surface Photo: Mark Wolvenne:

More information

Chapter 4. Understanding the Weather. Weather is short-term and caused by various air and ocean circulations

Chapter 4. Understanding the Weather. Weather is short-term and caused by various air and ocean circulations Video: Meteorologist Paul Douglas April 2013 Understanding the Weather Weather is short-term and caused by various air and ocean circulations There are natural climate cycle that cause large climate changes

More information

Ocean and Climate I.

Ocean and Climate I. Ocean and Climate I http://www.gerhardriessbeck.de/ Physical Characteristics of the Ocean Surface area: 3.61 10 14 m 2 Mean depth: 3.7 km Ocean volume: 3.2 10 17 m 3 Mean density: 1.035 10 3 kg/m 3 Ocean

More information

2. Can you describe how temperature and dissolved solids changes the density of water?

2. Can you describe how temperature and dissolved solids changes the density of water? Unit 4: Oceanography LT 4.1 Density: I can explain the role density plays to help form some currents. #1 Yes I can: 1. Can you explain what density is and how you calculate it? 2. Can you describe how

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

Climate Change or Climate Variability?

Climate Change or Climate Variability? Climate Change or Climate Variability? Key Concepts: Greenhouse Gas Climate Climate change Climate variability Climate zones Precipitation Temperature Water cycle Weather WHAT YOU WILL LEARN 1. You will

More information

Thermohaline and wind-driven circulation

Thermohaline and wind-driven circulation Thermohaline and wind-driven circulation Annalisa Bracco Georgia Institute of Technology School of Earth and Atmospheric Sciences NCAR ASP Colloquium: Carbon climate connections in the Earth System Tracer

More information

OCEAN MODELING. Joseph K. Ansong. (University of Ghana/Michigan)

OCEAN MODELING. Joseph K. Ansong.   (University of Ghana/Michigan) OCEAN MODELING Joseph K. Ansong Email: jkansong@umich.edu (University of Ghana/Michigan) OUTLINE INTRODUCTION MOTIVATION EQUATIONS OF MOTION INTRODUCTION TO ROMS (Regional Ocean Modeling System) EXAMPLES

More information

Oceans I Notes. Oceanography

Oceans I Notes. Oceanography Oceans I Notes Outlines on the front table Oceanography the science of our oceans that mixes biology, geology, chemistry, and physics (among other sciences) to unravel the mysteries of our seas. Divisions

More information

Where is all the water?

Where is all the water? Where is all the water? The distribution of water at the Earth's surface % of total Oceans 97.25 Ice caps and glaciers 2.05 Groundwater 0.68 Lakes 0.01 Soils 0.005 Atmosphere (as vapour) 0.001 Rivers 0.0001

More information

Oceanic Eddies in the VOCALS Region of the Southeast Pacific Ocean

Oceanic Eddies in the VOCALS Region of the Southeast Pacific Ocean Oceanic Eddies in the VOCALS Region of the Southeast Pacific Ocean Outline: Overview of VOCALS Dudley B. Chelton Oregon State University Overview of the oceanographic component of VOCALS Preliminary analysis

More information

Regional Oceanography: an Introduction

Regional Oceanography: an Introduction 138 Regional Oceanography: an Introduction A characteristic feature of the South Pacific Ocean is the existence of a second region of wind convergence in the tropics known as the South Pacific Convergence

More information

Transient/Eddy Flux. Transient and Eddy. Flux Components. Lecture 7: Disturbance (Outline) Why transients/eddies matter to zonal and time means?

Transient/Eddy Flux. Transient and Eddy. Flux Components. Lecture 7: Disturbance (Outline) Why transients/eddies matter to zonal and time means? Lecture 7: Disturbance (Outline) Transients and Eddies Climate Roles Mid-Latitude Cyclones Tropical Hurricanes Mid-Ocean Eddies (From Weather & Climate) Flux Components (1) (2) (3) Three components contribute

More information

Observation Homework Due 11/24. Previous Lecture. Midlatitude Cyclones

Observation Homework Due 11/24. Previous Lecture. Midlatitude Cyclones Lecture 21 Midlatitude Cyclones Observation Homework Due 11/24 1 2 Midlatitude Cyclones Midlatitude Cyclone or Winter Storm Cyclogenesis Energy Source Life Cycle Air Streams Vertical Structure Storm Hazards

More information

Chapter 6. Antarctic oceanography

Chapter 6. Antarctic oceanography Chapter 6 Antarctic oceanography The region of the world ocean bordering on Antarctica is unique in many respects. First of all, it is the only region where the flow of water can continue all around the

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

Atmosphere-Ocean-Land Interaction Theme. VOCALS Preparatory Workshop - NCAR, May 18-29, 2007

Atmosphere-Ocean-Land Interaction Theme. VOCALS Preparatory Workshop - NCAR, May 18-29, 2007 Atmosphere-Ocean-Land Interaction Theme VOCALS Preparatory Workshop - NCAR, May 18-29, 2007 The Southeastern Pacific Cloud-topped ABLs, with mesoscale structures Influenced by and influential on remote

More information

Investigation A: OCEAN IN THE GLOBAL WATER CYCLE

Investigation A: OCEAN IN THE GLOBAL WATER CYCLE Investigation A: OCEAN IN THE GLOBAL WATER CYCLE (NOTE: Completion of this activity requires Internet access.) Driving Question: What role does the ocean play in the global water cycle within the Earth

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

Dynamics and Kinematics

Dynamics and Kinematics Geophysics Fluid Dynamics () Syllabus Course Time Lectures: Tu, Th 09:30-10:50 Discussion: 3315 Croul Hall Text Book J. R. Holton, "An introduction to Dynamic Meteorology", Academic Press (Ch. 1, 2, 3,

More information

The roles of intra-seasonal Kelvin waves and. tropical instability waves in SST variability along. equatorial Pacific in an isopycnal ocean model

The roles of intra-seasonal Kelvin waves and. tropical instability waves in SST variability along. equatorial Pacific in an isopycnal ocean model The roles of intra-seasonal Kelvin waves and tropical instability waves in SST variability along equatorial Pacific in an isopycnal ocean model ChuanLi Jiang, LuAnne Thompson School of Oceanography, University

More information

Large-Scale Circulation with Locally Enhanced Vertical Mixing*

Large-Scale Circulation with Locally Enhanced Vertical Mixing* 712 JOURNAL OF PHYSICAL OCEANOGRAPHY Large-Scale Circulation with Locally Enhanced Vertical Mixing* R. M. SAMELSON Woods Hole Oceanographic Institution, Woods Hole, Massachusetts (Manuscript received 15

More information

Lecture 10: Climate Sensitivity and Feedback

Lecture 10: Climate Sensitivity and Feedback Lecture 10: Climate Sensitivity and Feedback Human Activities Climate Sensitivity Climate Feedback 1 Climate Sensitivity and Feedback (from Earth s Climate: Past and Future) 2 Definition and Mathematic

More information

Final Exam Answers. b. List the assumptions you made. Steady state heat and uniform temperature

Final Exam Answers. b. List the assumptions you made. Steady state heat and uniform temperature Final Exam Answers 1. [4] A planet in a distant galaxy has a solar constant of 3000W/m2, a radius of 12,000km and an albedo of a=0.6. a. Estimate the surface temperature of the planet. b. List the assumptions

More information

Lecture 7: The Monash Simple Climate

Lecture 7: The Monash Simple Climate Climate of the Ocean Lecture 7: The Monash Simple Climate Model Dr. Claudia Frauen Leibniz Institute for Baltic Sea Research Warnemünde (IOW) claudia.frauen@io-warnemuende.de Outline: Motivation The GREB

More information

Geophysics Fluid Dynamics (ESS228)

Geophysics Fluid Dynamics (ESS228) Geophysics Fluid Dynamics (ESS228) Course Time Lectures: Tu, Th 09:30-10:50 Discussion: 3315 Croul Hall Text Book J. R. Holton, "An introduction to Dynamic Meteorology", Academic Press (Ch. 1, 2, 3, 4,

More information

Module Contact: Dr Xiaoming Zhai, ENV Copyright of the University of East Anglia Version 2

Module Contact: Dr Xiaoming Zhai, ENV Copyright of the University of East Anglia Version 2 UNIVERSITY OF EAST ANGLIA School of Environmental Sciences Main Series UG Examination 2017-2018 OCEAN CIRCULATION ENV-5016A Time allowed: 2 hours Answer THREE questions Write each answer in a SEPARATE

More information

Temperature Change. Heat (Q) Latent Heat. Latent Heat. Heat Fluxes Transfer of heat in/out of the ocean Flux = Quantity/(Area Time) Latent heat

Temperature Change. Heat (Q) Latent Heat. Latent Heat. Heat Fluxes Transfer of heat in/out of the ocean Flux = Quantity/(Area Time) Latent heat Heat (Q) 1 calorie = 4.18 Joule Heat : Total Kinetic Energy Temperature: Average Kinetic Energy Heat that causes a change in temperature: Sensible Heat Temperature Change ΔQ = m c water ΔT Q in Joules

More information