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Dynamical Balance in the Earth’s Atmosphere

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Presentation on theme: "Dynamical Balance in the Earth’s Atmosphere"— Presentation transcript:

1 Dynamical Balance in the Earth’s Atmosphere
Lisa Goddard 15 Sept 2005 9/18/ Sept. 2005

2 Outline Newton’s laws of motion
Pressure gradients and hydrostatic balance Coriolis force Equations of large scale horizontal motion Geostrophic balance Surface friction Vertical motion 9/18/ Sept. 2005

3 Synoptic Map 9/18/ Sept. 2005

4 Sir Isaac Newton 9/18/201815 Sept. 2005
Born: 4 Jan 1643, Lincolnshire, England Died: 31 March 1727, London, England “A plague closed the University in the summer of 1665 and he had to return to Lincolnshire. There, in a period of less than two years, while Newton was still under 25 years old, he began revolutionary advances in mathematics, optics, physics, and astronomy ...” 9/18/ Sept. 2005

5 Newton’s Laws of motion
A mass in uniform motion – relative to a coordinate system fixed in space – will remain in uniform motion in the absence of any forces The rate of change of momentum of an object – relative to a coordinate system fixed in space – equals the sum of all the forces acting ... these two laws, together with conservation of mass and heat, form the basis of general circulation models of the atmosphere and ocean ... using the differential calculus! 9/18/ Sept. 2005

6 ... consider forces acting on a small (”differential”) volume of fluid
Atmospheric forces pressure gradient force gravity Coriolis/centrifugal force friction height north east 9/18/ Sept. 2005 ... consider forces acting on a small (”differential”) volume of fluid

7 Vertical pressure gradient force
Due to random molecular motions, momentum is continually imparted to the walls of the volume element by the surrounding air. The momentum transfer per unit time, per unit area, is the pressure In the absence of atmospheric motions the gravity force must be exactly balanced by the vertical component of the pressure gradient force. “Hydrostatic Balance” 9/18/ Sept. 2005

8 Sea-level pressure 9/18/ Sept. 2005

9 Horizontal pressure gradient force
... eastward pressure-gradient force per unit mass 9/18/ Sept. 2005

10 Sea Breeze 9/18/ Sept. 2005

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13 Newton’s Laws A mass in uniform motion – relative to a coordinate system fixed in space – will remain in uniform motion in the absence of any forces The rate of change of momentum of an object – relative to a coordinate system fixed in space – equals the sum of all the forces acting 9/18/ Sept. 2005

14 Deflection due to the Earth’s rotation: The Coriolis Force
Newton’s laws can only be applied in a rotating frame if the acceleration of the coordinates is taken into account Most satisfactory way of including coordinate acceleration is to include “apparent” forces into the statement of Newton’s 2nd law: the Coriolis force Pierre Simon Laplace (1778); Gaspard Gustave de Coriolis (1835) In 1848, Jean Foucault discovered that when a large pendulum swings, the earth appears to "move under it.” 9/18/ Sept. 2005

15 East-west motion Centrifugal force
Ω 9/18/ Sept. 2005

16 North-south motion Conservation of angular momentum
Ω Ω 9/18/ Sept. 2005

17 ... more on the Coriolis Force
Fco vanishes at equator Fco is proportional to velocity of parcel Fco is negligible for motions with timescales very short compared to the period of Earth’s rotation 9/18/ Sept. 2005

18 ... back to Newton’s 2nd Law following our fluid element ...
acceleration = sum of forces acting per unit mass height north east 9/18/ Sept. 2005

19 Atmospheric scale analysis
9/18/ Sept. 2005

20 Large-scale dynamical balance
To within about 15% in mid & high lats The horizontal pressure gradient force is in approximate balance with the Coriolis force for synoptic-scale motions at mid and high latitudes. The result is that winds tend to blow parallel to the isobars. “the geostrophic approximation” 9/18/ Sept. 2005

21 9/18/ Sept. 2005

22 Surface friction 9/18/201815 Sept. 2005
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23 Vertical motion Vertical scales are much smaller than horizontal ones; the atmosphere is “shallow.” For synoptic-scale motions, the pressure field is in hydrostatic balance to a very high degree of accuracy. Vertical velocity cannot be determined from the vertical momentum equation. But it can be determined indirectly. 9/18/ Sept. 2005

24 Summary The vertical component of the pressure gradient force is in hydrostatic balance with the gravity force to a very high degree of accuracy. On synoptic scales, the horizontal component of the pressure gradient force is in approximate geostrophic balance with the Coriolis force. Friction makes an important contribution near the earth’s surface, to give a 3-way balance Scale is key: “synoptic” means ~day, ~1000km 9/18/ Sept. 2005


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