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Oceanography

Igor Tchouiko Inglés 34 fichas

Oceanography

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  1. 1ThermoclineThe range of depths where the rate of change, the gradient of tempereature, is large.
  2. 2PycnoclineSince temp and density are closely related, the thermocline also tends to be the layer where density gradient is greatest.
  3. 3Equation of MotionEquation of Motion
  4. 4After Approximation Equation of Motion, Momentum in uAfter Approximation Equation of Motion, Momentum in u
  5. 5After Approximation Equation of Motion, Momentum in vAfter Approximation Equation of Motion, Momentum in v
  6. 6After Approximation Equation of Motion, Momentum in wHydrostatic ApproximationAfter Approximation Equation of Motion, Momentum in w
  7. 7f-plane approximationIs a cartesian coord system in which the Coriolis force is assumed const.
    -Useful for describing flow in regions small compared with the radius of the earth and larger than a few kilometers.
    f-plane approximation
  8. 8B-Plane Approximation-Coriolis force is assumed to vary linearly with latitude
    Useful for describing flows that extend over large distances and in numerical calculations of basin and global scale flows
    -winds effect the bottom layer due to B-effect
    -Where B_y = B(y-y0)
    B-Plane Approximation
  9. 9Rossby Number-Ratio of inertial forces to Coriolis forces
    -dimensionless number used in describing fluid flow.
    -it characterizes the importance of Coriolis accelerations arising from planetary rotation.
    -A small Rossby number (low-pressure system) signifies a system which is strongly affected by Coriolis forces, and a large Rossby number (tornados) signifies a system in which inertial and centrifugal forces dominate.
    R_o=u/Lf
  10. 10Geostrophic Balance-The balance between the Coriolis force and the pressure gradient force.
    -Results in geostrophic winds/flows which are directed parallel to isobars
    -Ocean flow is in geostrophic balance
    Geostrophic Balance
  11. 11Geostrophic Balance: Northern HemiGeostrophic velocity is parallel to isobars such that the high-pressure level is to the right of the current velocity
  12. 12Geostrophic Balance: Southern HemiGeostrophic velocity is parallel to isobars such that the high-pressure level is to the left of the current velocity
  13. 13Approximation of non-rotating planef=0
    WOrks for processes like waves, circulation in small harbors with a large Rossby Number
  14. 14Reynolds stressDescribes the impact of turbulent fluctuations on the mean flow.
  15. 15Ekman PumpingThe curl of the wind stress determines the rate of vertical velocity at the bottom of the Ekman layer.
    -Negative W_E are areas of high atmospheric pressure and anticyclonic winds. These are areas of convergence of Ekman transports that pump surface water downwards.
    -Positive W_E, low atmospheric pressure, cyclonic winds, divergence of Ekman transports that pump surface water upward from the ocean interior
  16. 16Ekman Boundary ConditionsSurface- Turbulent friction is caused by the wind. Top Picture
    -At bottom (-D_E) we can assume that u=o, v=o
    Ekman Boundary Conditions
  17. 17Capital U and VTransport: The amount of water moving through the water column
  18. 18DivergentDivergent= du/dx + dv/dy
    div>0 divergent
  19. 19ConvergentConvergent = -divergent
    div<0
  20. 20non-divergentdivergent= 0
    parallel flow
  21. 21Depth Integrated FlowMust be horizontally non-div, div=0
  22. 22Water MassA distinct body of water that originated in a particular area with a particular salinity and temp.
  23. 23How are Ocean Depth Characteristics Changed?Are changed by isopycnal advection, mixing, and diapycnol diffusion
  24. 24Water Mass Mixing Types-Advection (mostly along isopycnal lines) and isopycnal mixing
    -Diapycnal diffusion (along and across isopycnal lines)
    -Interaction with topography
  25. 25dyapicnal mixingMixing across isopycnal lines
  26. 26Isopycnal mixingmixing along constant density isobars
  27. 27Deep Circulation is Driven byvertical mixing, which is largest above mid-ocean ridges, near seamounts, and in strong boundary currents
  28. 28Where does deep convection produce bottom wateroccurs only in the far north Atlantic and at a few locations around Antarctica.
  29. 29Inertial OscillationChanges in wind stress that produce transient oscillations in the ocean
  30. 30Wind StressThe wind friction force per unit area, (tau_sx, tau_sy)
  31. 31Boundary Conditions for Ekman Balance-At the surface the turbulent friction is caused by the wind.
  32. 32Two major forcings which drive the ocean circulationa) Surface winds -> Ekman Pumping
    b) surface heat and freshwater fluxes which determine the surface flux of density (buoyancy)
  33. 33Ekman Pumping: When w_e is -ivHACD
    High Atm_press
    Anticyclonic winds
    Convergence of Ekman transport
    Down pumping
  34. 34Ekman Pumping: When w_e is +ivLCDU
    Low Atm_press
    Cyclonic
    Divergence of Ekman transport
    Uppumping

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Fichas sobre Oceanography , creado por Igor Tchouiko el 22/01/2019.
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Igor Tchouiko
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