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Significant dimensionless groups in fluid mechanics
Forces encountered in flowing fluids include those due to
inertia, viscosity, pressure, gravity, surface tension and
compressibility
Ratio of any two forces will be dimensionless
Inertia force =ma V2L2
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Inertia forces are important in fluid mechanics problems
The ratio of inertia force to each of the other forces listedabove leads to five fundamental dimensionless groups
Reynolds no.
Re after the name of the scientist who first developed it and is
thus proportional to the magnitude ratio of inertia force to
viscous force
He studied the transition between laminar and turbulent flow
regimes in a tube Re is the criterion by which the flow regime may be
determined
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Later experiments have shown that Re is a key parameter for
other flow cases as well, thus in general
WhereL is the characteristic length descriptive of the flow
geometry
Euler no. Euler is credited with being first to recognize the role of
pressure in fluid motion
The Euler no. is the ratio of pressure forces to inertia forces
Euler no. is often called thepressure coefficient, Cp
(p is the local pressure minus freestream pressure)
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Froude no.
This is significant for flows with free stream effects
Squaring the Froudes no. gives,
Which may interpreted as the ratio of inertia forces to viscous
forces.
The length L is the characteristic length descriptive of the flow
field In case of open channel flow, L is water depth;
Fr < l indicate subcritical flow, Fr > 1 indicate super critical
flow
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The dimensionless termsRe andEu represent the criteria of
dynamic similarity for the flows which are affected only by
viscous, pressure and inertia forces. Such instances, forexample, are
the full flow of fluid in a completely closed conduit,
flow of air past a low-speed aircraft and
the flow of water past a submarine deeply submerged to produceno waves on the surface.
Hence, for a complete dynamic similarity to exist between the
prototype and the model for this class of flows, the Reynolds
number, Re and Euler number, Eu have to be same for the two
(prototype and model). Thus
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Weber no.
Is the ratio of inertia forces to surface tension forces
(named after the German naval architect Moritz Weber who
first suggested the use of this term as a relevant parameter)
Mach no.
Where V is the flow speed and c is the local sonic speed
Key parameter that characterizes compressibility effects in a
flow
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The Mach no. may be written
It can be interpreted as the ratio of inertia forces to
compressibility forces
For truly incompressible flow (under some conditions even
liquids are quite compressible), c= so that M=0
The effects of compressibility become important when theMach no. exceeds 0.33
The situation arises in the flow of air past high speed aircraft,
missiles, propellers and rotary compressors
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