Lecture 20 ATOC 5051 INTRODUCTION TO PHYSICAL OCEANOGRAPHY

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

Chapter 7: Thermodynamics

C

The Ocean-Atmosphere System II: Oceanic Heat Budget

( ) = 1005 J kg 1 K 1 ;

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

Lecture 1. Amplitude of the seasonal cycle in temperature

Ocean Mixing and Climate Change

Upper Ocean Circulation

An Introduction to Coupled Models of the Atmosphere Ocean System

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

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

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

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

The Arctic Energy Budget

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

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

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

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

Air-Sea Coupling in an Eastern Boundary Current Region

Lab 12: El Nino Southern Oscillation

Chapter 4 Water Vapor

Ocean Dynamics. The Great Wave off Kanagawa Hokusai

5. General Circulation Models

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

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

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

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

Ocean Circulation. In partnership with Dr. Zafer Top

SD 13: The Indian Ocean s Influence on Regional Hydroclimate

SUPPLEMENTARY INFORMATION

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

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

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

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

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

Warm Up Vocabulary Check

Chapter 2 Solar and Infrared Radiation

3. Midlatitude Storm Tracks and the North Atlantic Oscillation

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

Ocean dynamics: the wind-driven circulation

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

ATS 421/521. Climate Modeling. Spring 2015

Interannual variability of top-ofatmosphere. CERES instruments

Energy transport and transfer in the wake of a tropical cyclone

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

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?

Lecture 3 questions Temperature, Salinity, Density and Circulation

Link between Hurricanes and Climate Change: SST

The Hydrologic Cycle

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

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

ESCI 485 Air/sea Interaction Lesson 5 Oceanic Boundary Layer

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

Homework 5: Background Ocean Water Properties & Stratification

CHAPTER 2 - ATMOSPHERIC CIRCULATION & AIR/SEA INTERACTION

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

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

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

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

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

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

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

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

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

Léo Siqueira Ph.D. Meteorology and Physical Oceanography

Forecasting. Theory Types Examples

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

Capabilities of Ocean Mixed Layer Models

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

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

Water mass formation, subduction, and the oceanic heat budget

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

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

Ocean and Climate I.

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

Lecture 9: Climate Sensitivity and Feedback Mechanisms

Climate Change or Climate Variability?

Thermohaline and wind-driven circulation

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

Oceans I Notes. Oceanography

Where is all the water?

Oceanic Eddies in the VOCALS Region of the Southeast Pacific Ocean

Regional Oceanography: an Introduction

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

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

Chapter 6. Antarctic oceanography

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

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

Investigation A: OCEAN IN THE GLOBAL WATER CYCLE

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

Dynamics and Kinematics

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

Large-Scale Circulation with Locally Enhanced Vertical Mixing*

Lecture 10: Climate Sensitivity and Feedback

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

Lecture 7: The Monash Simple Climate

Geophysics Fluid Dynamics (ESS228)

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

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

Transcription:

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.

z Previous class: x Unit:

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

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

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 = 2.44 10 6 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, 101.325 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.

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.

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?

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

(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)

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 1993-2010 SST trends below 90% significanc (c) Linear trend of satellite observ 1993-2010 period, with global mea areas show SSH trend below 90% Question: (b) 1993-2010 trend: SST&wind (c) 1993-2010 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?

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

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

E-P (http://www.whoi.edu/sbl/litesite.do?litesiteid=18912&articleid=28407) Aquarius Salinity

Ocean surface salinity budget (for a water parcel)

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

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

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.

E-P (solid) and salinity (dashed)

3. Ocean surface buoyancy flux ( )