Individual derivative: Difference between revisions
From Glossary of Meteorology
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<div class="definition"><div class="short_definition">( | <div class="definition"><div class="short_definition">(''Also called'' material derivative, particle derivative, substantial derivative.) The rate of change of a quantity with respect to time, following a [[fluid parcel]].</div><br/> <div class="paragraph">For example, if φ(''x'', ''y'', ''z'', ''t'') is a property of the fluid and ''x'' = ''x''(''t''), ''y'' = ''y''(''t''), ''z'' = ''z''(''t'') are the [[equations of motion]] of a certain [[particle]] of this fluid, then the [[total derivative]], <div class="display-formula"><blockquote>[[File:ams2001glos-Ie5.gif|link=|center|ams2001glos-Ie5]]</blockquote></div> (where '''u''' is the [[velocity]] of the fluid and '''∇''' is the [[del operator]]), is an individual derivative. It gives the rate of change of the property of a given [[parcel]] of the fluid as opposed to the rate of change at a fixed geometrical point, which is usually called the [[local derivative]]. The term '''u''' · '''∇'''φ is called the [[advective term]], expressing the [[variation]] of φ in a parcel moving into regions of different φ.</div><br/> </div> | ||
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Latest revision as of 14:28, 20 February 2012
individual derivative
(Also called material derivative, particle derivative, substantial derivative.) The rate of change of a quantity with respect to time, following a fluid parcel.
For example, if φ(x, y, z, t) is a property of the fluid and x = x(t), y = y(t), z = z(t) are the equations of motion of a certain particle of this fluid, then the total derivative, (where u is the velocity of the fluid and ∇ is the del operator), is an individual derivative. It gives the rate of change of the property of a given parcel of the fluid as opposed to the rate of change at a fixed geometrical point, which is usually called the local derivative. The term u · ∇φ is called the advective term, expressing the variation of φ in a parcel moving into regions of different φ.