Hydrostatic Pressure: p =  gz z = depth g = grav. Acc.  = density of seawater PGF per Unit Mass: 1/  x dp/dx = g x tan(  )

Slides:



Advertisements
Similar presentations
Earth’s Waters Chapter 4.4 Pages
Advertisements

Chapter 16 The Dynamic Ocean.
Introduction to Oceanography
Ocean Currents of the Eastern Gulf of Mexico Robert H. Weisberg Professor, Physical Oceanography College of Marine Science University of South Florida.
Crest- highest part of a wave Trough- lowest part of a wave Wavelength- horizontal length between crests. Wave height- vertical distance from crest to.
Wind-Driven Circulation in a Stratified Ocean Consider the ocean in several isopycnal layers that can be separated into two groups: Layers that outcrop.
Air Pressure and Winds III
Air Pressure and Wind Pressure: the amount of force exerted per unit of surface area Pressure can be increased in 2 ways 1.By increasing density or decreasing.
Ch. 22 Ocean Currents.
D A C B z = 20m z=4m Homework Problem A cylindrical vessel of height H = 20 m is filled with water of density to a height of 4m. What is the pressure at:
Density - density is a key property of seawater - one of the most important parameters in ocean dynamics - the ocean forms layers by density (denser waters.
Tropical storms and the First Law of Thermodynamics ATMO 435.
Ocean Currents and Climate
Wind and Ocean Currents Global winds Ocean Currents Local winds.
Warning! In this unit, we switch from thinking in 1-D to 3-D on a rotating sphere Intuition from daily life doesn’t work nearly as well for this material!
Hans Burchard Leibniz Institute for Baltic Sea Research Warnemünde Coastal Ocean Dynamics First course: Hydrodynamics.
More Climatic Interactions
* Reading Assignments:
Surface wind stress Approaching sea surface, the geostrophic balance is broken, even for large scales. The major reason is the influences of the winds.
Basic dynamics  The equations of motion and continuity Scaling Hydrostatic relation Boussinesq approximation  Geostrophic balance in ocean’s interior.
Ocean Circulation Winds and Currents. The __________________ and the ___________________ interact The ocean and atmosphere transport heat from the ______________________________.
VERTICAL STRUCTURE OF THE OCEAN – from Knauss Chapters 1 and 2 Oceanographers divide the ocean into zones.
Conservation of mass If we imagine a volume of fluid in a basin, we can make a statement about the change in mass that might occur if we add or remove.
Water and Wind Unit Chapter 13 Sections 2 & 3 Pages
Tuesday February 26, 2013 (Ocean Water Circulation)
OCEAN CURRENTS.
Section 5.4 Gravity Waves. Gravity Waves Gravity acts as the restoring force on parcels displaced from hydrostatic equilibrium. Pure gravity exists when.
Physical Oceanography SACS/AAPT Spring Meeting March 29, 2003 Coastal Carolina University.
Internal Tide Generation Over a Continental Shelf Summer 2008 internship Gaёlle Faivre Flavien Gouillon, Alexandra Bozec Pr. Eric P. Chassignet.
Ocean Currents and Climate Study Guide. Ocean water The ocean water never stands still. Ocean currents are like rivers that move within the ocean. This.
HYDROS TATIC. HYDROSTATIC branch of fluid mechanics that studies fluids at rest. It embraces the study of the conditions under which fluids are at rest.
For a rotating solid object, the vorticity is two times of its angular velocity Vorticity In physical oceanography, we deal mostly with the vertical component.
Basic dynamics ●The equations of motion and continuity Scaling
Overview of Open Channel Flow Definition: Any flow with a free surface at atmospheric pressure Driven entirely by gravity Cross-section can vary with location.
Tuesday April 5, 2011 (The Gulf Stream; Importance of Surface Currents; Deep Ocean Circulation)
The Causes of Weather May Air Masses  The air over a warm surface can be heated causing it to rise above more dense air.  Air Mass: A very large.
OCN 5401 Chapter 5 Equations of Motion Instructor: Dr. George A. Maul / X 7453.
Lecture Guidelines for GEOF110 Chapter 5 ( 2 hours) Chapter 6 (2 Hours) Ilker Fer Guiding for blackboard presentation. Following Pond & Pickard, Introductory.
An example of vertical profiles of temperature, salinity and density.
UNIT 2: OCEAN CIRCULATION. CHARACTERISTICS OF WATER ACTIVITY.
Properties of Seawater Density review Mixing Dissolved Gases.
Ekman pumping Integrating the continuity equation through the layer:. Assume and let, we have is transport into or out of the bottom of the Ekman layer.
WIND Movement of air in the atmosphere.. Remember Convection Principles Solar energy strikes the _____________________, heating the air, land and water.
Level of No Motion (LNM)
Geopotential and isobaric surfaces
What are ocean currents?
Ocean Motions Chapter 4.
Observed Structure of the Atmospheric Boundary Layer
A stable atmosphere. An absolutely stable atmosphere exists when a rising air parcel is colder and heavier (i.e., more dense) than the air surrounding.
What causes the wind to blow?
Osmosis (Revisited) Video. Density mass per volume of seawater Determined by temperature and salinity Density of seawater increases all the way to its.
 p and  surfaces are parallel =>  =  (p) Given a barotropic and hydrostatic conditions, is geostrophic current. For a barotropic flow, we have and.
Currents and Chemistry. Chemistry The oceans have high salinity: the total amount of dissolved salts in a liquid Sodium chloride (the same salt you put.
Ocean Currents. The water in the ocean is constantly moving The water in the ocean is constantly moving Broad bands of ocean water that flow in one direction.
Ocean Circulation Winds and Currents. The atmosphere and the oceans interact The ocean and atmosphere transport heat from the equatorial regions to the.
For a barotropic flow, we have is geostrophic current.
Define and we have • At the sea surface (z=0), the surface current flows at 45o to the right of the wind direction Depends on constant Az => • Current.
Lesson 8: Currents Physical Oceanography
Atmosphere and Climate
For a barotropic flow, we have is geostrophic current.
Unit 6 – Part I: Geostrophy
Frictionless Motion In addition assume no horizontal pressure gradients (no surface slopes) and homogeneous fluid.
Ocean Circulation.
Today’s Agenda…2-17 Bellringer: Explain what happens to temperature and pressure as you go deeper in the ocean. Review this week’s topics Notes on Oceans.
Opening! Brain pop!
Ocean Currents.
Global Ocean Conveyor Belt
Ocean Currents.
Ocean Circulation Page 42 in Notebook.
The Transfer of Heat Outcomes:
Presentation transcript:

Hydrostatic Pressure: p =  gz z = depth g = grav. Acc.  = density of seawater PGF per Unit Mass: 1/  x dp/dx = g x tan(  )

The potential temperature of a parcel of fluid at pressure P is the temperature that the parcel would acquire if adiabatically brought to a standard reference pressure P 0, usually 1000 millibars. Image is potential temperature at 5m depth (7/1/04)parceladiabatically

The stream function can be used to plot streamlines, which represent the trajectories of particles in a steady flow. Streamlines are perpendicular to equipotential lines. Considering the particular case of fluid dynamics, the difference between the stream function values at any two points gives the volumetric flow rate (or volumetric flux) through a line connecting the two points.streamlinesequipotentialfluid dynamicsvolumetric flux

Hysteresis: The dependence of the state of a system on the history of its state. Physics the lag in a variable property of a system with respect to the effect producing it as this effect varies

In oceanography, dynamic topography refers to the topography of the sea surface related to the dynamics of its own flow. In hydrostatic equilibrium, the surface of the ocean would have no topography, but due the ocean currents, its maximum dynamic topography is on the order of two metershydrostatic equilibriumocean currents Dynamics: The forces and motions that characterize a system

Entrainment is the movement of one fluid by anotherfluid

Diapycnal: definition. In the ocean, density always increases with increasing depth. However, surfaces of constant density (called "isopycnals") are not always level. Wind, the rotation of the Earth, and other processes cause density surface to slope. For example, a wind blowing along the coast can cause cold water which is usually deep to rise up to the surface, leading to water that is too cold to swim in, even in summer. The direction at right angles to the local isopycnal surface is called the “diapycnal” (i.e., across-isopycnal) direction. The angle between the diapycnal direction and vertical (i.e., directly out from the Earth) is always very small, a fraction of a degree at most. However, the difference between the two coordinates is very important to oceanographers, because the slope of isopycnals tells us a great deal about how the ocean is moving, and how it can interact with the coast and the atmosphere."isopycnals" Stochastic resonance is observed when noise added to a system changes the system's behavior in some fashion. More technically, SR occurs if the signal-to-noise ratio of a nonlinear system or device increases for moderate values of noise intensity. It often occurs in bistable. Strictly speaking, stochastic resonance occurs in bistable systems, when a small periodic (sinusoidal) force is applied together with a large wide band stochastic force (noise). The system response is driven by the combination of the two forces that compete/cooperate to make the system switch between the two stable states.signal-to-noise rationonlinearnoiseintensitybistablesinusoidal