ITHACA: First Findings from CTD Profiling Ivica Vilibić, Branka Grbec Institute of Oceanography and Fisheries, Split, Croatia www.izor.hr and ITHACA CTD.

Slides:



Advertisements
Similar presentations
FRESHWATER FLUX FROM BAY OF BENGAL AND SOUTH CHINA SEA AND ITS IMPACTS ON THE ITF R. Dwi Susanto 1,2 & Quanan Zheng 1 1 Department of Atmospheric and Oceanic.
Advertisements

Turbulent Mixing During an Admiralty Inlet Bottom Water Intrusion Philip Orton Hats off to the A-Team: Sally, Erin, Karin and Christie! Profs extraordinaire:
GEF2610 Physical Oceanography Course content The physical structure and circulations of the oceans, and the physical processes influencing them. Learning.
Types of Waves Harmonic Waves Sound and Light Waves
General Wave Properties
Horizontal Pressure Gradients Pressure changes provide the push that drive ocean currents Balance between pressure & Coriolis forces gives us geostrophic.
Internal Tidal Currents in the Gaoping Submarine Canyon I-Huan Lee National Museum of Marine Biology and Aquarium,Pingtung, Taiwan, , R.O.C.
Internal Tidal Hydrodynamics and Ambient Characteristics of the Adriatic Zagreb, 30 November 2006 Sea Level Measurements ITHACA PROJECT Nenad Leder and.
Coastal Ocean Dynamics Baltic Sea Research Warnemünde
Tsunamis and Tsunami Detection Systems December 1, 2010 Physical Oceanography Presentation Jeana Drake.
Water Level Sensor Physical processes related to bio-optical properties on the New York Bight inner continental shelf Grace C. Chang 1, Tommy D. Dickey.
Horizontal Pressure Gradients Pressure changes provide the push that drive ocean currents Balance between pressure & Coriolis forces gives us geostrophic.
Observations of Currents in Gaoping Submarine Canyon I-Huan Lee 李逸環 National Museum of Marine Biology and Aquarium, Pingtung, Taiwan, , R.O.C.
CHRP SPATIAL SURVEYS OF DISSOLVED OXYGEN BROWN UNIVERSITY & NARRAGANSETT BAY ESTUARY PROGRAM.
Exchange Flows Through a Long Shallow Channel Edwin A. Cowen DeFrees Hydraulics Laboratory, School of Civil & Environmental Engineering, Cornell University,
Ekman Transport Ekman transport is the direct wind driven transport of seawater Boundary layer process Steady balance among the wind stress, vertical eddy.
Diego Arcas, Chris Moore, Stuart Allen NOAA/PMEL University of Washington.
Physical Oceanography of the Yellow and East China Sea Dr. Steven R. Ramp Research Professor Naval Postgraduate School.
A Circulation Model to Investigate the Movement of Wastes from an Open Ocean Aquaculture Site David W. Fredriksson U. S. Naval Academy NOAA Research -
Lien, R.-C., and M. C. Gregg (2001), Observations of turbulence in a tidal beam and across a coastal ridge, J. Geophys. Res., 106,
Chapter 16 Section 2 Waves and Tides
Thermohaline and optical properties of the Drvenik-Hvar-Pelješac area Branka Grbec 1 (thermohaline), M ira Morović 1* (optical), Frano Matić 1,
Review Exam 1. Simple Harmonic Motion 11-1 Simple Harmonic Motion The force exerted by the spring depends on the displacement: (11-1)
Little Diomede Island, Bering Strait BERING STRAIT THROUGHFLOW ARC Comparison of Water Properties and Flows in the U.S. and Russian Channels of.
Sundermeyer MAR 550 Spring Laboratory in Oceanography: Data and Methods MAR550, Spring 2013 Miles A. Sundermeyer Observations vs. Models.
L. Padman, R. Muench, A. Orsi; Presentation OS41H-06 at the AGU Ocean Sciences Meeting, Portland OR, January 2004 Observations of Dense Off-Slope Flow.
Waves and Sound. POD Use the pressure vs. time graph below to answer questions # The period of the wave in the diagram above is given by letter.
Vibrations & Waves. In the example of a mass on a horizontal spring, m has a value of 0.80 kg and the spring constant, k, is 180 N/m. At time t = 0 the.
Air-sea fluxes over the ITHACA region Grbec, B. and Matić, F. Institute of oceanography and fisheries - Split.
Wave Vocab. Chapter 19: Harmonic MotionChapter 20: Waves 1.Harmonic motion 2.Oscillation 3.Period (definition and formula) 4.Frequency (definition and.
Evaluation of the Real-Time Ocean Forecast System in Florida Atlantic Coastal Waters June 3 to 8, 2007 Matthew D. Grossi Department of Marine & Environmental.
Simple Harmonic Motion This type of motion is the most pervasive motion in the universe. All atoms oscillate under harmonic motion. We can model this motion.
In situ evidence of deep equatorial layering due to inertial instability M. d’Orgeville, B. L. Hua & R. Schopp Laboratoire de Physique des Océans, IFREMER,
Deep-water Intrusions in the Puget Sound Sally Warner Coastal & Estuarine Fluid Dynamics class Friday Harbor Labs Summer 2006.
Chapter 7 Waves in the Ocean.
XBT Fall Rate Equation – A Review Pankajakshan and Gopalkrishna, National Institute of Oceanography, Goa, India.
ITHACA: thermistor time series Hrvoje Mihanović Hydrographic Institute of the Republic of Croatia, Split, Croatia DART-ITHACA Coordination Meeting,
Modelling activities at Institute of Oceanography and Fisheries (IOF), Split within ADRICOSM-EXT project Gordana Beg Paklar Institute of Oceanography and.
Simple Harmonic Motion Waves 14.2 Simple Harmonic motion (SHM ) 14-3 Energy in the Simple Harmonic Oscillator 14-5 The Simple Pendulum 14-6 The Physical.
Estuarine Circulation and the Knudsen Relation Puget Sound Oceanography 2011.
Oscillations about Equilibrium
High-resolution operational NWP for forecasting meteotsunamis
The Marine System Modelling group (MSM) at the UK's National Oceanography Centre (NOC) maintains and runs various NEMO configurations. Global, ocean-only,
Josh Kohut1, Elias Hunter1, and Bruce Huber2
Speed Formula - Waves.
Janelle Reynolds-Fleming and Rick Luettich
WAVE.
Characteristic Properties of Waves
Glen Gawarkiewicz Andrey Shcherbina Frank Bahr Craig Marquette
AP Physics Section 11-7 to 11-9 Wave Properties
What is a wave? A wave is simply a movement of energy that travels through a medium…
Tsunamis and Tsunami Detection Systems
John Beasley 1/31/2008 Propulsion Group: Solid and Hybrid Profiles
Least Squares Fit to Main Harmonics
LCDR John Hendrickson 17SEP2008
The CTD Data Set. What is Responsible for the Variance Observed in the Structure of the Data?
Combination of oceanographic data with wind data acquired during the cruise to try to draw conclusions on wind stress, Ekman transport and Ekman layer.
Laboratory in Oceanography: Data and Methods
Section 11.7 Probability.
Mid Atlantic Water Property Measurements W. S
This waveform is 35.0 cm long. How long is the wavelength?
The Northern Adriatic Experiment 2015: setup and preliminary results
P6314 / ENGI 9098 : Field Oceanography Cruise Report
An Analysis of San Clemente Basin: Crosshore vs. Alongshore
Hooke’s Law Period of oscillators
Features of A Wave Crest and Trough Crest:
Characteristic Properties of Waves
“Waves & Tides” 16.2.
ADCP-Corrected Absolute Geostrophic Current and Transport
Mazen Abualtayef Associate Prof., IUG, Palestine
Presentation transcript:

ITHACA: First Findings from CTD Profiling Ivica Vilibić, Branka Grbec Institute of Oceanography and Fisheries, Split, Croatia and ITHACA CTD Task Force Team The SettingThe Setting Ambient CharacteristicsAmbient Characteristics Internal WavesInternal Waves

The setting DART-ITHACA Coordination Meeting Zagreb, Croatia, CruiseDate ITHACA0114 February 2006 ITHACA0226 June 2006 DART0320/21 September 2006 ITHACA0428 September 2006 ITHACA0529/30 September 2006 T, S, DO,...

Ambient Characteristics DART-ITHACA Coordination Meeting Zagreb, Croatia, ITHACA01, 14 February 2006

Ambient Characteristics DART-ITHACA Coordination Meeting Zagreb, Croatia, ITHACA02, 26 June 2006

Ambient Characteristics DART-ITHACA Coordination Meeting Zagreb, Croatia, DART03, 20/21 September 2006

Ambient Characteristics DART-ITHACA Coordination Meeting Zagreb, Croatia, ITHACA04, 28 September 2006

Ambient Characteristics DART-ITHACA Coordination Meeting Zagreb, Croatia, TS diagram

Internal Waves DART-ITHACA Coordination Meeting Zagreb, Croatia, ITHACA02, 26 June 2006

Internal Waves DART-ITHACA Coordination Meeting Zagreb, Croatia, DART03, 20/21 June 2006

Internal Waves DART-ITHACA Coordination Meeting Zagreb, Croatia, ITHACA04 ITHACA05

Internal Waves DART-ITHACA Coordination Meeting Zagreb, Croatia, Simple estimates Theoretical wavelength ( it,t ) and velocity (V it,t ) of internal waves, computed through two-layer model and assuming that they are diurnal internal tides (period of 24 h). The depths h and H and densities ρ h and ρ H are estimated from CTD sections. CruisehHρhρh ρHρH V it,t it,t 26 Jun m/s43.7 km 20 Sep m/s54.8 km 28 Sep m/s62.3 km 29 Sep m/s62.3 km Empirical wavelength ( it,e ) and velocity (V it,e ) of internal waves, computed from CTD sections assuming that they are diurnal internal tides (period of 24 h). CTD is the non- transformed wavelength estimated from the transects, Δt is time needed for the sampling of one internal wave, while A is tentatively estimated wave amplitude. Cruise CTD ΔtA (tent.) Tides V it,e it,e 26 Jun km5 h2-4 m neap 0.50 m/s42.3 km 20 Sep km6 h7-8 m neap 0.72 m/s62.5 km 28 Sep km-4 h4/12 m spring 0.27 m/s23.3 km 29 Sep km-5 h8-10 m spring 0.34 m/s29.3 km

Internal Waves DART-ITHACA Coordination Meeting Zagreb, Croatia, But what about internal seiches (21.2 h), internal inertial oscillations (17.6 h),... The true nature of observed internal oscillations will be seen on other data: ADCP, thermistor chain, bottom pressure gauge.