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ELEMENTARY FLUID MECHANICS REVJEW(基本的流体力学REVJEW)
ELEMENTARY FLUID MECHANICS REVJEW
The subjectoffluid mechanicsis usuallydividedinto fluid staticsand fluid dynamics. In static
fluids, the only force exertedbythe fluid is a pressureforce~nonnalto the surface. The basic equation
is F ==f areapd~ and the pressure may be found by the fundamental equation of hydrostatics:
dp = .:ydz. Fluid dynamicsproblemsaresolved using con!;ervationof mass,energy, and momentum.
Elementaryfluid mechanicsproblemsusuallydealonly with incompressiblefluids in either the
static or the steady,one-dimensionalflow condition. There are five general categoriesof problems:
three types of forces (hydrostatic,dynamic,and viscous)andtwo types of flow (confinedand
unconfined). Many complicated problemsinvolve several categories.
Almost all equationsfound in fluid mechanicste~:tbooksand handbookswere derived using
certain simplifying assumptions. Do not use an equation unlessyou are sure that in making these
assumptionsyou arenotintroducinganintolerableerrorto the accuracyof your answer. Checkthe
answerto insure the assumptionwasvalid. For example,if you use a laminar flow equationto find
the velocity in a pipe, checkthe Reynolds number usingthat velocity to be sure that it is within the
laminarrange.
HYDROSTAllC FORCESAND PRESSURES
A For incompressible fluids, the fundamental equation (dp = -ydz) simplifies to:
p + yz = constant.
The only force exerted by a static fluid is a pressure force normal to the surface:
F = f areapdA = volume of pressureprism. Itthe fluid is incompressible,the f
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