separation in three-dimensional flow: critical points ... · basic notions and definitions (1) in a...
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SEPARATION IN THREE-DIMENSIONAL FLOW:CRITICAL POINTS, SEPARATION LINES AND VORTICES
Jean DéleryEmeritus advisor at [email protected] Edition 2011
H. Werlé. © OneraFlow above the Concorde wing
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Separation in three-dimensional steady flow
1 - The critical point theory and three-dimensional separation.
2 - The basic constitutive elements: separation lines of detachment and attachment, separation surfaces of detachment and attachment, vortex structures.
3 - Topology of some remarkable three-dimensional flows:
vortex formation over a delta wingvortices of slender bodyvortex wake of a classical wingseparation induced by an obstacle or a protuberanceafterbody without and with propulsive jetvortex formation past a three-body automobile
4 - Two-dimensional separation revisited with 3D concepts or an apparently simple case.
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Separation in three-dimensional steady flow
Part 1: THE CRITICAL POINT THEORY AND THREE-DIMENSIONAL SEPARATION
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Towards a rational definition of 3D separation
Henri WerléRobert Legendre
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The critical point theory and three-dimensional separation
Henri Poincaré, 1854 - 1912
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Some definitions or what we are about to speak
Three-dimensional separated flows are characterized by the existence of vortical structures defined as spatial concentration of vorticity resulting from boundary layer separation.
Once separation has occurred, vorticity tends to concentrate in the vicinity of surfaces – or sheets – whose rolling up forms vortices.
In the reality, such surfaces – or sheets - defined as support of discontinuities (or singularities) do not exist. Such concepts belong to perfect fluid models. In the real world, vorticity is continuously distributed in space and occupies a certain volume in the vicinity of what we call separation or detachment surfaces.
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Structure of a three-dimensional boundary layer
Outer flow streamline
Outer flow velocity
Crosswise profile
YZ
Streamwise profile
Skin friction lineSkin friction vector
XZ
τXτZ
Ve
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Naive conceptions or separation
Lateral evacuation
Two-dimensional flow Three-dimensional flow
In three-dimensional flows, velocity develops a transverse (crosswise)component allowing the flow to laterally escape.
The separated flow is no longer trapped in a closed recirculation bubble, but can be evacuated along the transverse dimension.
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Basic notions and definitions (1)
In a three-dimensional flow, skin friction is a vector.
We call skin friction line a line tangent at each of its points to the local skin friction vector.
Sometimes the concept of limit streamline is used: it is defined as the limit of a streamline when the distance y normal to the wall tends to zero.
It can be shown that the limit direction of the velocity vector when y tends to zero is colinear with the skin friction vector (if the fluid is Newtonian).
Skin friction lines and limit streamlines coincide.
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Basic notions and definitions (2)
Here we will use the physical concept of skin friction line rather than the limit streamline concept which results from a passage to the limit.
The use of the wall streamline concept is still worst since there is no flow on a surface!
The skin friction lines can be visualized by means of a viscous film deposited of the model surface: they have a real existence.
The set of skin friction lines will be called the skin friction line surfacepattern or more shortly skin friction line pattern or surface pattern.
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Skin friction lines visualization on a blunted body
Wind tunnel S2Ch. © Onera
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Wind tunnel S2Ch. © Onera
Skin friction lines visualization on a blunted body
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The flow is assumed steady (not essential).
We consider the two-dimensional space constituted by the surface of athree-dimensional body.
We introduce the skin friction vector field on the body surface.
(1) )z,x(dz
)z,x(dx
zx τ=
τ
We define the lines of force or trajectories of this field. Such lines are solutions of the differential system (x and z are two coordinates in the surface):
The critical point theory (1)(Poincaré, 1882 ; Legendre, 1956 ; Lighthill, 1963)
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In general, by one point on the body goes one and onlyone such trajectory called a skin friction line.
This is not true at a point P0 where the skin friction vector vanishes:then system (1) is singular.
Such a point is called singular or critical, the solution of system (1)at a critical point leading to an eigenvalue problem.
In the vicinity of a critical point, the solution lines behaviour dependsof the nature (real or complex) and sign of the eigenvalues.
The critical point theory (2)
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Solution in the vicinity of P0 is looked for via a first order Taylor series expansion:
( ) ( )0P
x0
P
xx zz
zxx
x)z,x(
00
−⎟⎠⎞
⎜⎝⎛∂τ∂
+−⎟⎠⎞
⎜⎝⎛∂τ∂
=τ
( ) ( )0P
z0
P
zz zz
zxx
x)z,x(
00
−⎟⎠⎞
⎜⎝⎛∂τ∂
+−⎟⎠⎞
⎜⎝⎛∂τ∂
=τ
0)z,x(,0)z,x( zx =τ=τ
At point P0 we simultaneously have:
The critical point theory (3)
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For simplicity, the origin of system axis is placed at P0 and index 0 is omitted.
zz
xx
dz
zz
xx
dxzzxx
∂τ∂+
∂τ∂
=
∂τ∂+
∂τ∂
=
∂τ∂+
∂τ∂
=
∂τ∂+
∂τ∂ z
zx
x
dz
zz
xx
dxzzxx
The skin friction derivatives being assumed different from zero, then:
⎟⎠⎞
⎜⎝⎛
∂τ∂+
∂τ∂μ+⎟
⎠⎞
⎜⎝⎛
∂τ∂+
∂τ∂λ
μ+λ=
zz
xx
zz
xx
dzdxzzxx
(2)
The critical point theory (4)
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A solution is looked for by writing (2) in the following logarithmic form:
( )( )zxS
zxd
zz
xx
zz
xx
dzdxzzxx μ+λ
μ+λ=
⎟⎠⎞
⎜⎝⎛
∂τ∂+
∂τ∂μ+⎟
⎠⎞
⎜⎝⎛
∂τ∂+
∂τ∂λ
μ+λ
The solution is of the form:
( )( ) )tS(expAfdt
fSdf
zxSzxd
−=→−==μ+λμ+λ
[ ]tSexpAzx −=μ+λ
problem find λ and μ
t integration dummy variable
The critical point theory (5)
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The previous form is possible if the following conditions are satisfied:
0x
Sx
zx =μ∂τ∂
+λ⎟⎠⎞
⎜⎝⎛ −∂τ∂
0Szz
zx =μ⎟⎠⎞
⎜⎝⎛ −∂τ∂
+λ∂τ∂
xSxx
xx
zx λ=∂τ∂
μ+∂τ∂
λ
zSzz
zz
zx μ=∂τ∂
μ+∂τ∂
λ
First degree homogenous algebraic system for λ and μ:
The critical point theory (6)
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0S
zz
xS
xzx
zx
=−
∂τ∂
∂τ∂
∂τ∂
−∂τ∂
Non trivial solution system determinant must be equal to zero:
Algebraic second degree equation for S
0et0: =μ=λTrivial solution
02 =∂τ∂
∂τ∂
−∂τ∂
∂τ∂
+⎟⎠⎞
⎜⎝⎛
∂τ∂
+∂τ∂
−xzzxzx
SS zxzxzx
The critical point theory (7)
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Jacobian matrix
zx
zxFzz
xx
∂τ∂
∂τ∂
∂τ∂
∂τ∂
=
p = - trace of F et q = determinant of F
⎟⎠⎞
⎜⎝⎛
∂τ∂
+∂τ∂
−=zx
p zx
p and q depend only of the skin friction derivatives at the critical point
0qSpS 2 =++Eigenvalue equation
⎟⎠⎞
⎜⎝⎛
∂τ∂
∂τ∂
−∂τ∂
∂τ∂
=zxzx
q xzzx
The critical point theory (8)
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2q4ppS
2
2,1−±−
=
The solutions of the previous equation (eigenvalue of matrix F) are written:
q4pD 2 −=
The nature – real or complex – of the eigenvalues depends of the signof the discriminant:
The critical point theory (9)
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)1(reigenvecto,Seigenvalue 111 μλ→
)2(reigenvecto,Seigenvalue 222 μλ→
x,
z,
z,
xofdepend,,, zzxx
2211 ∂τ∂
∂τ∂
∂τ∂
∂τ∂
μλμλ
21 A,A are determined bymatching conditions
with the surrounding field
[ ]tSexpAzx 1111 −=μ+λ
[ ]tSexpAzx 2222 −=μ+λ
0P
z1 x ⎟
⎠⎞
⎜⎝⎛∂τ∂
−=λ 1P
x1 S
x0
−⎟⎠⎞
⎜⎝⎛∂τ∂
=μ
2P
z2 S
z0
−⎟⎠⎞
⎜⎝⎛∂τ∂
=λ0P
x2 z ⎟
⎠⎞
⎜⎝⎛∂τ∂
−=μ
Values of λ and μ
The critical point theory (10)
eigenvector
eigenvector
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The critical point theory (11)
( ) ( )1221
212121 tSexpAtSexpA)t(xμλ−μλ
−μ−−μ=
( ) ( )1221
212121 tSexpAtSexpA)t(zμλ−μλ
−λ−−λ−=
The solution in the vicinity of a critical point is of the form:
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The critical point theory (12)
The different critical points:
S1, S2 real and of same sign node
S1, S2 real and such that S1 = S2 isotropic node
S1, S2 real with opposite signs saddle point
S1, S2 complex conjugate focus
S1, S2 imaginary degenerate focus or centre
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Node type critical point
0,100 21 =λ=λ0,1 21 =λ−=λ
4S,1S 21 ==
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Isotropic node type critical point
21 SS =
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Saddle type critical point
1S,1S 21 =−=
100,0 21 −=λ=λ1,1 21 −=λ=λ
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Focus type critical point
4i1S 2,1 ×±= 4iS 2,1 ×±=
centre
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The different critical points
Node Isotropic node Saddle point
Focus Centre Node-saddle pt. combination
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Attachment node Detachment node Isotropic attachment node
Saddle point Focus Centre
The main critical points
The sense of displacement along the trajectories gives a physical meaningto the solution behaviour in the vicinity of the critical points
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Critical point classification in the plane [p,q]
centre
focusfocus
Isotropic nodeIsotropic node
Attachment node Detachment node
col Saddle point
q
p0
Saddle point
q4pD 2 −=
4pq
2
=
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Wind tunnel S2Ch. © Onera
Attachment node at the nose of a blunt body
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Attachment node at the nose of a blunt body
Wind tunnel S2Ch. © Onera
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Saddle point
East & Hoxey
Separation in front of an obstacle
Detachment line
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Spectacular foci
Hugo Mitch
Bonnie Luis
Hurricanes
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Critical points for the rotational at the wall
On a surface, the rotational vector is tangent to the surface.
At a point on a surface, the skin friction vector and the rotational vector are orthogonal.
The skin friction lines and the rotational trajectories are two families of orthogonal curves.
The critical points of the skin friction field are also critical points for the rotational field (in general of different nature).
Well known results:
Ωr
Ωr τ
r
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Centre Isotropic centre
Saddle point
Focus
rotationnalskin friction
Critical points for the rotational at the wall
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Three-dimensional nodes and foci
Body surface Body surface
Skin friction lineFocus Node
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Vortex swallowed by an air intake
H. Werlé. © Onera
The air intake suction effect induces the formation on a vortex springingfrom the ground. Here the vortex is swallowed by the air intake.
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Three-dimensional nodes and foci
Attachment point Detachment point
To a node on the surface is associated a saddle point in the contiguous flow
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Attachment node on the front part of a high speed train
Three-dimensional nodes and foci
H. Werlé. © Onera