1 natural strain near welding interface for different collision angles epnm-2008 lisse, netherlands...
TRANSCRIPT
![Page 1: 1 Natural Strain Near Welding Interface For Different Collision Angles EPNM-2008 Lisse, Netherlands H.H. Yan; X.J. Li May 6-9, 2008 Dalian University of](https://reader030.vdocuments.us/reader030/viewer/2022013122/56649f045503460f94c18163/html5/thumbnails/1.jpg)
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Natural Strain Near Welding Interface For Different Collision Angles
EPNM-2008 Lisse, Netherlands
H.H. Yan; X.J. Li
May 6-9, 2008
Dalian University of Technology
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Outline of talk
• Introduction
• Model
• Solutions
• Results
• Discussions
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Introduction
• Where will strain rate and strain be used?• To analyze the acting of mechanics and
thermodynamics• To setup the model of heat transmission• To estimate the thickness of layer melted• And so on
Temperature ?For example:
Base plate
Flyer plate
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Temperature?
Caused by Shock compaction
Caused by deformation energy
dtYdYdUU peq
peq 00
2 2 222 3 2
6 ( )3 2 23
xypx xxyeq
Strain rate?Strain?
VC
UT
0
To research here
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Model
Ideal fluid
Symmetrical collision
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Reason of adopting the model
Detonation of explosive is about 2000~3000 m/s.
Pressure (1.6~3.5) × 1010 Pa
bfv 2/2b
Strength of materials >10
bnegligible
So
compressibility small
+
<6%
IdealLiquidmodel
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Fig. Plane diagram of conjugate
complex velocity
Ψ1
0
Vf? B
u
B’
C’
D’
D
A
A’
C
v
Ψ2
Ψ3
Ψ4
Transforming
holographic function method
2
fV
H
21
1 ;fV
H
21
2 ;fV22H
3 ;fV
H
22
4
iyxz yxiyxzw ,,
Boundary condition:
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Solutions (Strain)
• Strain rate
• Strain
X Horizontal ordinateY Vertical ordinateu Horizontal velocityv Vertical velocity
x
u
,y
u
,x
v
,y
v
x
u
y
uy
u
x
u
E
Eddy factor considered tnn
Tn EEE
1
Along stream line
Points on the line
Steady assumptionIncompressiblityconservation of momentum
model
holographic function method
finite difference method
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solving x,y,u,v• The complex potential yxiyxzw ,,
yx,
yx,
velocity potential
stream function
1 1 1 1
2
2 2 2 2
2
2 2 2 2 1 1
1( , ) 2[(1 cos ) (1 cos ) ] /( (1 cos )) (3.1)
/ 2 1 1
{(1 cos ) ln[(1 ) ] (1 cos ) ln[(1 ) ]/ 2
cos {ln( ) ln( )} 2 sin { }} /( (1 cos )) (3.2 )
f
v v N Ku v tg tg tg tg
V H u u M J
xu v u v
H
N KM N J K tg tg a
M Jy
H
1 1 2
2
2 2 2 1 1
12{ (1 cos ) (1 cos ) sin {ln[( cos )
/ 2 1 1 2
( sin ) ] ln[( cos ) ( sin ) ]} cos { }} /( (1 cos )) (3.2 )
v vtg tg u
u u
N Kv u v tg tg b
M J
Xyuv
solved
For stream line given
With u,v changing
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Stream lines plotted
Fig. Different flow diagrams with differentψ at
β = 130
Y(H
2/2
)
X( H2 /2)
~ = 0.5
~ =0
~ =- 0.5
~ =-1
~ =-2
3
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Solving stain rate (along stream line)
x
u
y
uy
u
x
u
E
0
y
v
x
u
incompressibe
0
y
u
x
v
irrotational
yx y
v
x
u
y
u
x
v
y
uxy
2
)/()(2
)/(2
43124321
4312121
ffffffHH
fffffHH
xy
yx
)sincossincos
(cos})sin()cos(
sin
)sin()cos(
sin{sin
)1(
1)cos1(
)1(
1)cos1(
222222
2222221
KJ
KJ
NM
NM
vu
v
vu
v
vu
u
vu
uf
)sincoscossin
(sin})sin()cos(
1
)sin()cos(
1{cos)cos(
)1(
1)cos1(
)1(
1)cos1(
222222
2222222
KJ
JK
NM
NM
vu
vuu
vu
u
vu
uf
)sincossincos
(sin})sin()cos(
sin
)sin()cos(
sin{cos
)1()cos1(
)1()cos1(
222222
2222223
KJ
KJ
NM
NM
vu
v
vu
v
vu
v
vu
vf
)sincoscossin
(cos})sin()cos(
1
)sin()cos(
1{sin)cos(
)1()cos1(
)1()cos1(
222222
2222224
KJ
JK
NM
NM
vu
vuu
vu
v
vu
vf
solved
second-order tensor
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Strain rate results (For example)
-10 -8 -6 -4 -2 0 2 4 6 8 10-1.0
-0.8
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
Fig. Diagram of strain rate with different angles at ~ = -0.2
x
xy
Ⅱ
Ⅰ
0/ xstrainrate。
X/(H2/2
)
-1.60 -1.55 -1.50 -1.45 -1.40 -1.350.525
0.530
0.535
0.540
0.545
0.550
0.555
0.560
Fig. No. I part magnification in Fig.
0/ xstrainrate。
X/(H2/2
)
β =60
β =200
β =130
45
015.0||
x
015.0||
x
4
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• Results of strain rate
For the same relative streamline, at the points with the same relative horizontal ordinate, calculations showed that the ratio of tensile and shear strain rate to the stagnation point strain rate is very similar for colliding
angles in the range 6–20º. in detail:(the paper)
H.H. Yan, X.J. Li.
Strain rate distribution near welding interface for different collision angles in explosiveWelding
International Journal of Impact and Engineering.2008 , 35 : 3-9.
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Solving stain (along stream line)
Fi g. Di agram of streaml i ne (trace)
nn
On
θ τ n y
x o
ξ
Ψ 1 Δ
θ
nn+1
On+1
τ n+1
When the continuums deform, displacement, eddy and distortion of each infinitesimal among them will change. Its orientation and shape will change at any time. According to the steady assumption, the streamline is same as the trace; that is to say, change of strain along the streamline is same as that along the trace. To calculate the strain distribution, the eddy factor must be eliminated.
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Calculating Process
:
+ +nn
nTn
ttt tt
EEt
EE
nn
1
1
0 1
limlim tnnTn EEE
1 tEEE nnn
1
jlikklnijn mmEE )()(
jlikklnijn EE )()(
)2,1,,,( lkji
22nn vu
lt
To calculate the natural strain by eliminating the eddy factor
In detail
Transformation relation
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Strain results (For example)
-10 -8 -6 -4 -2 0 2 4 6 8 10-1.0
-0.8
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
Fig. Diagram of strain with different angles at ~ = -1.0
X/(H2/2)
β =60
β =200
β =130
Stra
in
E11
E12
-10 -8 -6 -4 -2 0 2 4 6 8 10-1.0
-0.8
-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
Fig. Diagram of strain with different angles at ~ = -2.0
X/(H2/2)
β =60
β =200
β =130
Stra
in
E11
E12
5
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Discussion
• The model adopted is simple and ideal• If the viscous-elastic constitutive equations were used to
analyze stain field, explosive welding mechanics will be explained very well.
• If the geometric non-linearity was considered, the Green’s and Almansi’s strain can be used in the future.
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THANK YOU