Potential Flow Theory

Содержание

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Elementary fascination Functions

To Create IRROTATIONAL PLANE FLOWS
The uniform flow
The source and

Elementary fascination Functions To Create IRROTATIONAL PLANE FLOWS The uniform flow The
the sink
The vortex

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THE SOURCE OR SINK

source (or sink), the complex potential of which

THE SOURCE OR SINK source (or sink), the complex potential of which
is

This is a pure radial flow, in which all the streamlines converge at the origin, where there is a singularity due to the fact that continuity can not be satisfied.
At the origin there is a source, m > 0 or sink, m < 0 of fluid.
Traversing any closed line that does not include the origin, the mass flux (and then the discharge) is always zero.
On the contrary, following any closed line that includes the origin the discharge is always nonzero and equal to m.

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The flow field is uniquely determined upon deriving the complex potential W

The flow field is uniquely determined upon deriving the complex potential W
with respect to z.

Iso ψ lines

Iso φ lines

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A Combination of Source & Sink

A Combination of Source & Sink

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THE DOUBLET

The complex potential of a doublet

THE DOUBLET The complex potential of a doublet

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Uniform Flow Past A Doublet

The superposition of a doublet and a uniform

Uniform Flow Past A Doublet The superposition of a doublet and a
flow gives the complex potential

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Find out a stream line corresponding to a value of steam function

Find out a stream line corresponding to a value of steam function is zero
is zero

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There exist a circular stream line of radium R, on which value

There exist a circular stream line of radium R, on which value
of stream function is zero.
Any stream function of zero value is an impermeable solid wall.
Plot shapes of iso-streamlines.

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Note that one of the streamlines is closed and surrounds the origin

Note that one of the streamlines is closed and surrounds the origin
at a constant distance equal to    

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Recalling the fact that, by definition, a streamline cannot be crossed by

Recalling the fact that, by definition, a streamline cannot be crossed by
the fluid, this complex potential represents the irrotational flow around a cylinder of radius R approached by a uniform flow with velocity U.
Moving away from the body, the effect of the doublet decreases so that far from the cylinder we find, as expected, the undisturbed uniform flow.

In the two intersections of the x-axis with the cylinder, the velocity will be found to be zero.
These two points are thus called stagnation points.

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To obtain the velocity field, calculate dw/dz.

To obtain the velocity field, calculate dw/dz.

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Equation of zero stream line:

Equation of zero stream line:

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Cartesian and polar coordinate system

Cartesian and polar coordinate system

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V2 Distribution of flow over a circular cylinder

The velocity of the fluid

V2 Distribution of flow over a circular cylinder The velocity of the
is zero at = 0o and = 180o. Maximum velocity occur on the sides of the cylinder at = 90o and = -90o.

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THE VORTEX

In the case of a vortex, the flow field is

THE VORTEX In the case of a vortex, the flow field is
purely tangential.

The picture is similar to that of a source but streamlines and equipotential lines are reversed.
The complex potential is

There is again a singularity at the origin, this time associated to the fact that the circulation along any closed curve including the origin is nonzero and equal to γ.
If the closed curve does not include the origin, the circulation will be zero.

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Uniform Flow Past A Doublet with Vortex

The superposition of a doublet

Uniform Flow Past A Doublet with Vortex The superposition of a doublet
and a uniform flow gives the complex potential

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Angle of Attack

Angle of Attack

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The Natural Genius & The Art of Generating Lift

The Natural Genius & The Art of Generating Lift

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Hydrodynamics of Prey & Predators

Hydrodynamics of Prey & Predators

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The Art of C-Start

The Art of C-Start

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The Art of Complex Swimming

The Art of Complex Swimming

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Development of an Ultimate Fluid machine

Development of an Ultimate Fluid machine

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The Art of Transformation

Our goal is to map the flow past a

The Art of Transformation Our goal is to map the flow past
cylinder to flow around a device which can generate an Upwash on existing Fluid.
There are several free parameters that can be used to choose the shape of the new device.
First we will itemize the steps in the mapping:

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Transformation for Inventing a Machine

A large amount of airfoil theory has been

Transformation for Inventing a Machine A large amount of airfoil theory has
developed by distorting flow around a cylinder to flow around an airfoil.
The essential feature of the distortion is that the potential flow being distorted ends up also as potential flow.
The most common Conformal transformation is the Jowkowski transformation which is given by

To see how this transformation changes flow pattern in the z (or x - y) plane, substitute z = x + iy into the expression above to get

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