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<div class="definition"><div class="short_definition">A set of hydrodynamical equations representing the application of Newton's  second law of motion to a fluid system.</div><br/> <div class="paragraph">The total [[acceleration]] on an individual fluid [[particle]] is equated to the sum of the forces acting  on the particle within the fluid. Written for a unit mass of fluid in motion in a [[coordinate system]]  fixed with respect to the earth, the [[vector]] equation of motion for the [[atmosphere]] is  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee40.gif|link=|center|ams2001glos-Ee40]]</blockquote></div> where '''u''' is the three-dimensional [[velocity]] vector, '''&#x003a9;''' the [[angular velocity of the earth]], '''k''' a unit  vector directed upward, &#x003c1; the [[density]], ''p'' the [[pressure]], ''g'' the [[acceleration of gravity]], and '''F''' the  [[frictional force]] per unit mass. The usual form for the [[scalar]] equations of motion in [[spherical  coordinates]] (&#x003bb;, &#x003c6;, ''r''), with &#x003bb; the longitude, &#x003c6; the latitude, and ''r'' the radius from the center of  the earth, is as follows:  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee41.gif|link=|center|ams2001glos-Ee41]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee42.gif|link=|center|ams2001glos-Ee42]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee43.gif|link=|center|ams2001glos-Ee43]]</blockquote></div> Most global [[numerical weather prediction]] models and [[general circulation]] models use an approximate  version of the above nonhydrostatic [[primitive equations]]. This version involves the  approximation of the vertical equation of motion by the [[hydrostatic equation]] and the selective  approximation of ''r'' = ''a'' + ''z'' by ''r'' &asymp; ''a'', where ''a'' is the constant radius to [[mean sea level]] and ''z''  is the height above mean sea level. These approximations result in the quasi-static primitive equations  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee44.gif|link=|center|ams2001glos-Ee44]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee45.gif|link=|center|ams2001glos-Ee45]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee46.gif|link=|center|ams2001glos-Ee46]]</blockquote></div><br/>''See'' [[Newton's laws of motion]], [[vorticity equation]].</div><br/> </div>
<div class="definition"><div class="short_definition">A set of hydrodynamical equations representing the application of Newton's  second law of motion to a fluid system.</div><br/> <div class="paragraph">The total [[acceleration]] on an individual fluid [[particle]] is equated to the sum of the forces acting  on the particle within the fluid. Written for a unit mass of fluid in motion in a [[coordinate system]]  fixed with respect to the earth, the [[vector]] equation of motion for the [[atmosphere]] is  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee40.gif|link=|center|ams2001glos-Ee40]]</blockquote></div> where '''u''' is the three-dimensional [[velocity]] vector, '''&#x003a9;''' the [[angular velocity of the earth]], '''k''' a unit  vector directed upward, &#x003c1; the [[density]], ''p'' the [[pressure]], ''g'' the [[acceleration of gravity]], and '''F''' the  [[frictional force]] per unit mass. The usual form for the [[scalar]] equations of motion in [[spherical coordinates|spherical  coordinates]] (&#x003bb;, &#x003c6;, ''r''), with &#x003bb; the longitude, &#x003c6; the latitude, and ''r'' the radius from the center of  the earth, is as follows:  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee41.gif|link=|center|ams2001glos-Ee41]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee42.gif|link=|center|ams2001glos-Ee42]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee43.gif|link=|center|ams2001glos-Ee43]]</blockquote></div> Most global [[numerical weather prediction]] models and [[general circulation]] models use an approximate  version of the above nonhydrostatic [[primitive equations]]. This version involves the  approximation of the vertical equation of motion by the [[hydrostatic equation]] and the selective  approximation of ''r'' = ''a'' + ''z'' by ''r'' &asymp; ''a'', where ''a'' is the constant radius to [[mean sea level]] and ''z''  is the height above mean sea level. These approximations result in the quasi-static primitive equations  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee44.gif|link=|center|ams2001glos-Ee44]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee45.gif|link=|center|ams2001glos-Ee45]]</blockquote></div>  <div class="display-formula"><blockquote>[[File:ams2001glos-Ee46.gif|link=|center|ams2001glos-Ee46]]</blockquote></div><br/>''See'' [[Newton's laws of motion]], [[vorticity equation]].</div><br/> </div>
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Latest revision as of 16:55, 25 April 2012



equations of motion

A set of hydrodynamical equations representing the application of Newton's second law of motion to a fluid system.

The total acceleration on an individual fluid particle is equated to the sum of the forces acting on the particle within the fluid. Written for a unit mass of fluid in motion in a coordinate system fixed with respect to the earth, the vector equation of motion for the atmosphere is
ams2001glos-Ee40
where u is the three-dimensional velocity vector, Ω the angular velocity of the earth, k a unit vector directed upward, ρ the density, p the pressure, g the acceleration of gravity, and F the frictional force per unit mass. The usual form for the scalar equations of motion in spherical coordinates (λ, φ, r), with λ the longitude, φ the latitude, and r the radius from the center of the earth, is as follows:
ams2001glos-Ee41
ams2001glos-Ee42
ams2001glos-Ee43
Most global numerical weather prediction models and general circulation models use an approximate version of the above nonhydrostatic primitive equations. This version involves the approximation of the vertical equation of motion by the hydrostatic equation and the selective approximation of r = a + z by ra, where a is the constant radius to mean sea level and z is the height above mean sea level. These approximations result in the quasi-static primitive equations
ams2001glos-Ee44
ams2001glos-Ee45
ams2001glos-Ee46

See Newton's laws of motion, vorticity equation.


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