ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

347
The Finite Element Method Fifth edition Volume 3: Fluid Dynamics

Transcript of ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Page 1: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Page 2: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 6: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Preface to Volume 3.......................................................Acknowledgements....................................................................

1 Introduction and the equations of fluid dynamics...1.1 General remarks and classification of fluid mechanicsproblems discussed in the book.................................................1.2 The governing equations of fluid dynamics..........................1.3 Incompressible (or nearly incompressible) flows..................1.4 Concluding remarks.............................................................

2 Convection dominated problems - finite elementappriximations to the convection-diffusionequation...........................................................................

2.1 Introduction...........................................................................2.2 the steady-state problem in one dimension..........................2.3 The steady-state problem in two (or three) dimensions.......2.4 Steady state - concluding remarks.......................................2.5 Transients - introductory remarks.........................................2.6 Characteristic-based methods..............................................2.7 Taylor-Galerkin procedures for scalar variables...................2.8 Steady-state condition..........................................................2.9 Non-linear waves and shocks..............................................2.10 Vector-valued variables......................................................2.11 Summary and concluding...................................................

3 A general algorithm for compressible andincompressible flows - the characteristic-basedsplit (CBS) algorithm......................................................

3.1 Introduction...........................................................................3.2 Characteristic-based split (CBS) algorithm..........................3.3 Explicit, semi-implicit and nearly implicit forms....................3.4 ’Circumventing’ the Babuska-Brezzi (BB) restrictions..........3.5 A single-step version............................................................3.6 Boundary conditions.............................................................

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3.7 The performance of two- and single-step algorithms onan inviscid problems...................................................................3.8 Concluding remarks.............................................................

4 Incompressible laminar flow - newtonian andnon-newtonian fluids......................................................

4.1 Introduction and the basic equations....................................4.2 Inviscid, incompressible flow (potential flow)........................4.3 Use of the CBS algorithm for incompressible or nearlyincompressible flows..................................................................4.4 Boundary-exit conditions......................................................4.5 Adaptive mesh refinement....................................................4.6 Adaptive mesh generation for transient problems................4.7 Importance of stabilizing convective terms...........................4.8 Slow flows - mixed and penalty formulations.......................4.9 Non-newtonian flows - metal and polymer forming..............4.10 Direct displacement approach to transient metalforming.......................................................................................4.11 Concluding remarks...........................................................

5 Free surfaces, buoyancy and turbulentincompressible flows.....................................................

5.1 Introduction...........................................................................5.2 Free surface flows................................................................5.3 Buoyancy driven flows..........................................................5.4 Turbulent flows.....................................................................

6 Compressible high-speed gas flow...........................6.1 Introduction...........................................................................6.2 The governing equations......................................................6.3 Boundary conditions - subsonic and supersonic flow...........6.4 Numerical approximations and the CBS algorithm...............6.5 Shock capture......................................................................6.6 Some preliminary examples for the Euler equation..............6.7 Adaptive refinement and shock capture in Eulerproblems.....................................................................................

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6.8 Three-dimensional inviscid examples in steady state..........6.9 Transient two and three-dimensional problems...................6.10 Viscous problems in two dimensions.................................6.11 Three-dimensional viscous problems.................................6.12 Boundary layer-inviscid Euler solution coupling.................6.13 Concluding remarks...........................................................

7 Shallow-water problems.............................................7.1 Introduction...........................................................................7.2 The basis of the shallow-water equations............................7.3 Numerical approximation......................................................7.4 Examples of application.......................................................7.5 Drying areas.........................................................................7.6 Shallow-water transport........................................................

8 Waves...........................................................................8.1 Introduction and equations...................................................8.2 Waves in closed domains - finite element models...............8.3 Difficulties in modelling surface waves.................................8.4 Bed friction and other effects................................................8.5 The short-wave problem.......................................................8.6 Waves in unbounded domains (exterior surface waveproblems)...................................................................................8.7 Unbounded problems...........................................................8.8 Boundary dampers...............................................................8.9 Linking to exterior solutions..................................................8.10 Infinite elements.................................................................8.11 Mapped periodic infinite elements......................................8.12 Ellipsoidal type infinite elements of Burnnet and Holford...8.13 Wave envelope infinite elements........................................8.14 Accuracy of infinite elements..............................................8.15 Transient problems8.16 Three-dimensional effects in surface waves......................

9 Computer implementation of the CBS algorithm.....

Page 9: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

9.1 Introduction...........................................................................9.2 The data input module..........................................................9.3 Solution module....................................................................9.4 Output module......................................................................9.5 Possible extensions to CBSflow...........................................

Appendix A Non-conservative form ofNavier-Stokes equations................................................

Appendix B Discontinuous Galerkin methods inthe solution of the convection-diffusion equation......

Appendix C Edge-based finite element forumlation...

Appendix D Multigrid methods......................................

Appendix E Boundary layer-inviscid flow coupling....

Author index....................................................................

Subject index..................................................................

Page 10: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 14: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 17: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 18: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 19: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 23: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 26: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 28: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 29: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 30: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 31: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 32: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 33: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 34: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 35: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 36: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 37: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 38: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 39: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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&- % % > %%= & % '(.B 1 % 1 5' N > %%= #% %% 3L %& %& D & " 1.'.; 6 & % & % 6%% = $

0 ; -'/ 6' '7

#

%% H1 2 > 3L K % %& % & # K > K 7.48

B ./)

i–2 i–1 i i+1 i+2

hh

Ni Ni+1

# 0> * (

) -'/

Page 40: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

B ./)&

& "& %& % >

% 6 %& %% %%&

)6!% + "# %$ )6"#+

# & % 3H1 % ... K 7..'8 7..98 1 % 5 > %

-

.-

'.

./4

C< K % & C <# + & %

% 3H1 & % - & + & & %*(

6 & 2 & & L % & ..; 7 8 > - % & % & % N L 2 # & $1./.9 'B

& % & 1

.

'' ..-

.

-

./*

& % =% 7...8 A

% '

./(

-.

.9B

- .' ..'.

.9B&

; -'/ 6' '7

Page 41: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & =% %%% % ' . % & 2 & & + , .* & & K

- 2 =% 7.9B8 & , .* % = 2 # K 7./*8 C > < 2

L % 2 # & L 7 8 - # & + K 7./)8 7 8

B .9'

2 C& L < S& + & K 7./*8T &

.9'&

-

..9'

# % L 2 N %'B./.9 % 3H1 %# L

%%& + %%= & % % =& C1 1<& , L 1 %%% .).(

h

h

U

U1

U2

U

# 05 ! * + ,

) -'/

Page 42: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# % & & & @ ;B ' % H1 % % % & K 7./(8, .( % K 7./)8

C> L < %% D & ;'

6 C%< & & %% =% 1 %& >- # % % ../ % & =%

.9. & 1 # %% & + % & %;' & %&

z

yx

z

yx

(a)

T (y ) T = 0

T = 0

T = 0x

y

Boundary conditions for test problem

U

θ

(b) Solutions for θ = 45° (top) andθ = 60° (bottom)

# 0? %-& ! . /

; -'/ 6' '7

Page 43: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& & 3H1 %

# )#*+ . )/01+ !

& %% C < 3H1 K 7./*8 & K H1 % ../ = > K % = K 7.;)8 7./.8 K 7./*8= H: 7

8

B .9;

& K > 1 % 6 7K ./B8

.- .9/

& &2 3H1 % 7K .9'8# + & '4

.

B .99

% # & > &2 % %-

- .9)

6 3H1 &2 & 7K .9'8 # & H: ,! % K & 3H1

08 " 9 # ''

.. .; % % > 3L K & 6 3H1 2

) -'/

Page 44: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

+ & K >- ../ % 6$ % % & % = % % %& & % >%% % > % L

% % & % = % & % &2 > % % 7 8

1 & & % & + % & & > $ % K

%% & > K 7.''8

! B .94

K % K 7.'B8 & % , % %

.9* &

B .9(

& %=# 3H1 % K 7.948 7.9(8

& % %% ../

78 K >- P

7&8 %% % 7 ..;8 3 % %%

6 & % K %& C % < %& >%% % K % K # % A

' % 7 B8 & 3 3 & %+ & , .. H1

" 9 # ''

Page 45: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

. %+ & B K % 2 D= K %& H1 K &

&' (( '

0< ' 9 ' ' ''

$

# &- % % %%& & >%% K 7.'8

A

B .)B

% > & % % & % K SK 7.'B8T

B .)'

& # % K 7.)B8

.)'&

# %& + > > > K 7.)'8 % K # & % & K & &

% &

.).

.);

# > K 7.)'8 & %

B .)/

) -'/

Page 46: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K % & 2 >- % % & % % % F '# K 7.).8 &

& 6 B B %

B

7.)98

S & & T# % K %% , .'B # %& > 7L 8 2

" 2 !

% % %%& > K # % L > # 3H1 %% & >1 &K -+ & > % # H1 K 7H:8 % & % K K & % & & 1& & & 3H1 & # 1 & + 7,!8 %& > K , & + %% &

% >

φ(x ); t = 0 φ(x – Ut)

x

# 0.@ 0 ! ! ! *

' 9 ' ' ''

Page 47: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& .)// 3H1 & K= & %% 3H1 > & N =% % & & N H1 K 7H:8 %

% & %> + # %% %& & 5 ;. ! @ ;;;/ @ 1;B;9;) ;4;* %> =% =% % & %E & %%

& E # K % L %% & -+ % + L & %& 3H1 & K # & A 7'8

% & > H1 .)P 7.8 % %% %& > %%= #3H1 " %% + &

% & & & # K & & & %%

% # & D K !% ; & =% % % & K

L & %% D K > 3L K & % 7K .'8 # %% % #3H1 % & K >% %& D %& % %% + % %& % % K %& 1 % # & %% H H: %& F '!% '. % H: % &2 N %& & # - % & !% ;, % % &

= = >% &

) -'/

Page 48: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

0= '';/

, $ ! ! $

& % C < % & K 7.).8 %& +> %% %& % L 2 % H1 % %%= % 7 8# & + = % %

% , .''78 % > %& K 7.)'8 ,

.))

t

t

Characteristic

Updated nodeposition

Initial nodeposition

h

∆t

∆t

(a) Forward

x

x

tn+1 = tn + ∆t

tn–1 = tn – ∆t

tn

tn

(b) Backward

# 0.. 1 " ' #$ 2!) #$ . !

'';/

Page 49: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% %

' '

.)4

C< & % & K 7.)98 , %

' .)* % % # % & & " % >% L %& &

F ' # # % % L %&

%& %% > > > + N & , & % % & & >% % % # % & &1>

, .''7&8 %%% % # & & & &

6 $&&/9 '(4/ % K # % & 2 % & > 3H1 /)

# L % % + % %%= % L % # =% % =

, 1$# !

K L > 7.)'8 % %

.)(

B .4B

%

B .4B&

) -'/

Page 50: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% >- S T$ & %%= & =%

& & .4' % '

B .4. H1 2 L K ' &

+= & K

% . .4;

'

%& , .'. % & % S K 7.4'8T & # &

' & .4/6 K ' & %%= & %

%- &#&' & B .49

%' &#& .4)

& & %

% &#& .4)&

# & %= % % = # % & %

N (y )

x

N (x )

1

1

∆tt

tn + ∆ty = x + u∆t

tn

# 0.0 3

'';/

Page 51: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/) # & = % = 7 & 8 & & & L %%= &

, ' ! (! $# !

& % %& K 5 /939) % %% %= % > , % % N =% & # + %& '(*/94 & %& 9*)' # =% , .'; K 7.)'8

B .44

6 %% L K > K >- H1 % %%= % # 2 & K 7, .';8

'

'

'

'

.4*

K 2 =% & 2 > % 6 1 & K % % N

t

x

δ ≈ U∆t

φn + 1

φnφn(x – δ)

# 0.

) -'/

Page 52: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, # =%

.

.

.

."; .4(

B9'

.

'

.

.

". .*B

'

.

.

.

.*B&

& % > 7, .';8

.*' L %%= L &2 # ).);

.*.

K 7.4(837.*.8 K 7.4*8

'

'.'.

.

.

.

.

.

.

.*;

'. '.

' '.

.*;&

'. '

..*;

& K > 7 K .*B8 # #3H1 % & = &2 L , %& K 7.*;8 & %%= '. 7 =% 8

'

.

.

.

.*/

'';/

Page 53: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 %%= ).

' .

.*9

# =%

". .*)

K 7.4*837.*'8 K 7.*98 7.*)8 K B9

'

' '.

.

.'.'.

.

.

'.

.'.

.'.

.*4

'. '

..**

%%= '. =% #

'. " .*( L %%= # + =%3H1 &

'

.

.

.(B

H 2 & K K 7.98A

.

.

.('

# L &2 & & L %%= L & & %%= &2 &1 %%= K 7K .('8

) -'/

Page 54: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 % H1 % %%= -+ 3H1 % %%=

& .(. &# =% # &

%' / / # .(;

=% > &K

% &#&

&#

&

/

&#

&

&# &

.(/

/ # & 2 6 & % =% / #

/ '.

&

#

& .(9

# '.

&

# & .()

& & > & K # %%= K

% > K , & & % %%= & % =% K 7.(;8 & ,

> %& & 7 L 8

.(4

> %& % & % ).);

.(*

& K 7.(48 .. L > %, > 78

L & & % % % % # > &- % & /

'';/

Page 55: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 % =% %% '. L 7 8 % &

.((

% %%& & +, .'/ & %& & K 7.(48

% = & = &

3 >%% K 7.(;8 % + & 1

'

// # B .'BB % .. .; &

3H1 %%= = =/ & L &

'. 1

'. .

..'B'

# & K

.'B.

! &

1.0

0.8

0.6

0.4

0.2

00 1 2 3 4 5 6 7

Pe

Unstable

C = αopt = coth Pe – 1/Pe

Stability limit C = 1/Pe + 1 – 1/Pe

U∆t

/h

# 0.8 -* !

) -'/

Page 56: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, .'/ % % K 7..98 7 ! ! * &5' % + & H1 > 2 & & % 1 % & = K 7.(;8 H1

& & & %% 3H1

&#

.

&#

K 7.)B8 = H1 &# !% & > %& K 7./*8 > &6 > %% 3H1 %

, .'9 % & D 1& % % # % & & + L := L)/ > 3H1 =% = % + L L %%

= % % % = % =% % = & % K 7.(;8

% .'B; & > K 7.(;8

'

& % =% % A

$ %' %$' $' .'B/

$ & # % % , .') % > %% % 6 & =

'';/

Page 57: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, &

6 3L %& & %

.'B9

(a) Original form

(b) Form after one revolution using consistent M matrix

(c) Form after one revolution using lumped mass (Lax–Wendroff)

# 0.< " " 4 * ' #$ 5") #$ 2 " ) #$ 2 " #67$

) -'/

Page 58: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

.'B9&

7 8 & % % K L % % L K

+ % & N & =% , .. = & % & K 7.'B98 % > % & & P = & & %& %, %& % %+

% % #

B .'B) %& & %+ %& L

Lumped

C = 0.5, 1/T

Lumped

C = 0.1, 1/T

C = 0.5, 2/T C = 0.1, 2/T

Consistent

C = 0.5, 3/T

Consistent

C = 0.1, 3/T(a) Courant number = 0.5 (b) Courant number = 0.1

Lumped/consistent M Courant number = 0.5 Courant number = 0.1

# 0.= ! " + "

'';/

Page 59: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%+ C & < K %

B .'B4

= & , .'4 1 )9

%+ %& , .'9 +)')9 & %

Initial configuration

# 0.> " * .* 4

) -'/

Page 60: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

0> '9,' -' ' ' ' )'/

#3H1 % # =% % H1 % 2 , & =% & # 9*))

'

.

.

.

."; .'B*

, K 7.)'8

.'B(

.

.

.''B

& K 7.'B(8 7.''B8 K 7.'B*8

'

.

.

.'''

6 &

'

.

.

.''.

K 7.'B(8 K 7.''.8 >

'

.

.

.

"; .'';

6 & K K 7.*;8 %% ! & & #3H1 % &2 # & -+ 3H1 & # #3H1 % 3L K >

&

'

.

.''/

'9,' -' ' ' ' )'/

Page 61: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% %%% 3H1 # #3H1 + K :=3 L % + L> =)/

05 " ;

$ #3H1 3H1 % H H: L 7> 8

.

.

.''9

% N 3H1 & -+ %& & %%% K

0? %;' )

# % % % % % & & > %& 7 =% % %% & % N 8 U % K

B .'')

% #

.''4

> & K %

B .''*

% > 6 % %& $ + &

'..

B .''(

, .'* K L % %% % % + % 1 # & % > !% ) 1 % %& D %

) -'/

Page 62: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

φ t1 t2 t3

x

Creation of a shock

# 0.5 " ! ! *

A B C D E F G

A B C D E F G

(a) Profile at time t = 0

φ

φ

(d) Profile at time t = 2

(c) Profile at time t = 1 x

t = 2

t = 1

(b) Characteristics

Shock

2

1

φt = 0

x

t

x

x

# 0.? 3 #." ($

%;' )

Page 63: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# % 1 %%> %+ , .'(78 1 , .'(7&8 # L %% % . 1 %% # 1 %% + %7 = 8 1 L K &

#

#

# ## # B .'.B

B .'.'

# % 1 %% % K 7.'.'8 1 5 1 3 + 1 % K = %&

D > D 7!% ) 48 = % L K 1 %+ & % ! %%= + 1 % B & & % , ..B N %

%& % % K %& & %&+ L K # + L > A

' 2 2. L &

6 % L + &:%)4 + L & & %%)*)( # L

:%.

.'..

= , ..' %& %% $

K % :% N 1 % > & =% %

) -'/

Page 64: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, %& % & %& =% 2 7.'..8

:%. %%

0 .'.;

%

" %& % 1 &- C1 %< %& !% ) % >% D %

0.30 0.35 0.40 0.45 0.50 0.55 0.60 0.65 0.70Normalized length

1.3

0.8

0.3

–0.3

Adve

cted

sca

lar

(b)

θ = 1/2

θ = 0

0.30 0.35 0.40 0.45 0.50 0.55 0.60 0.65 0.70Normalized length

1.3

0.8

0.3

–0.3

Adve

cted

sca

lar

(a)

# 00@ " ! * 0* ' #$ + 8 ! 8) #$ + ! 8

%;' )

Page 65: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

&' ((( ';)

0.@ ';) )'/

7 -$ -# $ 5

# % & #3H1 % % % .* & > K % 7K .'8 % % =% & # ))4B

'

.

.

.

.

.'./

& B ', K 7.'8

*

+

.'.9

C = 0.1, CLap = 0

C = 0.1, CLap = 1

# 00. " ."& ( ! " 6 6

) -'/

Page 66: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

L .

.

*

+

.'.9&

&

1

*

+

.'.9

1 + + +

+

+

*

+

.'.9

%%= K 7.'./8

'

*

+

.

.

1

*

+

*

*

+

.'.)

" * % & '

'

+

*

'

*

'

.

.

1

+

+

'

.

.

1

+

+

' .'.4

6 H1 %%= %% % >%% & '

. 6 =% % >2 % B

&

&#&

&#

*

+

.

&#

1

*

+

.

&#

*

+

.'.*

';) )'/

Page 67: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & % = K 7.(;8

% / / .'.(

*

7 L 8 K 7.(/8

&#1

&

/

&#

11

.

&

/

&#

&

&#

.1

&#

+ &

% &#&

.'.(&

'; & %%=

% %&4' = % & '

; ' '

; %% K % K 7.'B/8 % & K

7 -%5! ! $ -%5!-# !

# % % %%%= # =% % % & % = 1 & %3 7 5 3 %8 = =%# + H1 % %%= & %%

& K 7.'8 #

%

% & .';B

) -'/

Page 68: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% = %& C<

&#

.';'

% C<

& &#

*

.';'&

L =%

% %' .';. > K = % % > 1 & %" % %

& & L = # > %&

> K L '

' & + '

, ...78# & >% %3 %

& % A

# 2 !% '. =% %%= K 7.';.8

'.

.%' .';;

t

xi – 1 i i + 1tn

tn + ∆t

(a) Single-step explicit

t

xi – 1 i i + 1tn

tn + ∆t

(b) Standard predictor–corrector

t

xi – 1 i i + 1tn

tn + ∆t

(c) Local prediction–corrector(c) (two-step Taylor–Galerkin)

tn + 1/2∆t

tn + 1/2∆t

# 000 " !

';) )'/

Page 69: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# 3 !% ' % '. > K 7.';.8

' %''. .';/# % K > 5 3 & %%

L K 7.';B8 , ...7&8 > =% C%< '

&% . . & L

%6 %& >% #3H1 %

K 7.'8 % A

# 2 , % '. #

'.

.

+

.';9

'.

%%= =%

'.

.

.1

.1

*

+

.';9&

#

1

*

+

.

'.

.';9

# 3 & & #3H1 %%= K 7.'.*8

%

&#

*

+

&#

'.

&#'.

.';9

& % % & %

%

&#

'.

*

&#+ '.

&#'.

*

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) -'/

Page 70: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

A

' # & =% 5' / (2 71288 =% % % & % K 7.';98

. # + K 7.';)8 K 1

& % K 7.'.(8 %& %

6 % % & A

; > %& % +

&

% #

'. & K 7 8

% '.

& K 7.';98 % , '. '. 1 '. '. %%% % % > =% %

, ...78 # &%%% #* * 94)94.*B %& >% D K & & % !% ) !% ; & % 1 #3H1 % & = D # % & N & *'*. %&

7 ! % !

& % & & L & % % & & K 7.'8

1

*

+ , .';4

1 = 2 % & # K % ' %&

1

.';*

';) )'/

Page 71: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & %&$ % &

K 7.'8 & L 1

& %

1 44' .';(

& = 4

4 4 .'/B K 7.';48 & 7 & L 8

44

'

, .'/'

% & 4' & 7 5 8

4' .'/. & % K % % A

B .'/;

% >% K % 6 % =% & > %& & &

B

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B

# & K 7.'8

# & K 7.'/.8 &

' .

K % 7.'/;8

'

'

B

.

.

B

% %

) -'/

Page 72: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K 7.'/B8 % > % %& % # = % % %& & $ !% ; % >& % % = -+ %%

0.. "' # ''

# & & %% %% % # & = & % & + %% % - %& > %& > - # - % % & >

3L K # % % > K 3H1 % %& &2 & 3H1 H: % % & , %& % % & % %& >- % H1 %%= % 1 & += %= % % & &

% % #3H1 =P -+ %& , K D % % % 3L %& & = % !$ !

!'

' 6 $1 #@5 % O3H1 D % % %& 1 K "2 2 2 2 2 53 '((3.9( '(*.

. 5 ! 5 " > %& L K & + L "2 2 2 0 ./;399 '(9.

; 6 5 %

31 K 2 2 2 #2 22 //939; '()(/ $ % 6 + L L K & + 2 2 2 2 2 6 99'3( '(4.

9 $ # %& & %&92 2 2 2 2 37 943)* '(4/

) "! 0 12 5 H >

%& D #% D +

!'

Page 73: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, 7 @ 8 F 6 : '(4) 7$ '(498

4 ! , HN 65 "! 0 12 , L K + + 2 2 2 22 2, ';*(3() '(4)

* "! 0 12 @! 1 65 6 % + % K 2 2 2 22 22 ';'3// '(44

( @! "! 0 12 U + 3 % %& 2 2 2 2 2 22 '*;'3// '(44

'B 12 "! 0 12 6 % & %> + %%= L %& 2 2

2 2 2 28 '4B9>'' '(*B'' $ : 6 + L %

% & K , "

- ,* 7 #@5 8 6 F ;/ 6 '(4('. H: H F :5 6

L 3 K & + 7 +

+2 9 ')''3'4 '(4B'; #@5 @ 61 6 & C% < +

# 7 >8 %% ;*43('

"= '(*B'/ H, ! =% % 2 "2

2 2 2 2 943)B '(*9'9 @ # $1 1 6 2 H1

3L %& %% K % "2 22 2 2 6: .93/; '(*9

') #@5 : , H & 0 @ , 1& # H1

K L K + - "! , 7 # #2 #@5 8 6 (9 6'(**

'4 " J &2 K 3L % D D %& "2 2 2 2 2 282 .;;3)9'((*

'* 12 @, "! 0 12 D

% , , 7 5 H 8 F /% '; %% .9'3*; ! '(*.

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Page 74: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

.9 #@5 6 $1 6 1 3H1 , , 7 5 H

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Page 75: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/4 5 #, 5 % H1 3L %& " - 7

5 F 1 5 % 8 F F 6! %% .*3;) 5 $ 1 @ '(*'

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%% K D , ! 7 @5 8 F F %% /4'3* 6 : '(*.

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% = K K + : "22 " #2 2 F '.3') '(*;

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% # 2 2 2 56 44(3() '((49) " @ : ## #2 ! H1 H1

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94 "! 0 12 5 :Q 12 , D

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Page 76: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

)) @ 6 #3H1 % %& 2 2 22 2 3, 'B'3'( '(*/

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2 "2 2 52 ;;93). '(4(

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49 @ @ : , "! 0 12 , % 1: # %% 666>*4>BB;. 5 6 @ '(**

4) @ @ : , "! 0 12 ,

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%& "2 2 2 2 2 68 ;';3.( '(*/

4( 5 :Q 6 % %& 2 2 2 2 2 36 'B'3'9 '(*4

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H & '((B*' " @ 6 %%

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Page 77: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1 #' #' '-'/ -'/3 9 '';/

- 6 "7 #'

. ('

+ % D K %%& & %& %& D # K %& % K K + %%& %2 %& D % %% %& > K & & L D !% /34 %2 # K & !% '

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;'

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.

;.

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.

;;

&1 % %% %%% .

Page 78: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

( ;/

& + D D=

;9

;)

& % P %+ % & % ( % & % & 7K ''.&8

.;

;4

1 ' B &K % %%% & # K % & D % %&A

;* # & - L >

K 7;/8 % & & 7F '8 % # % H1 %%= K >>- & & % % 3H1 % & &%% % >- & 3L K % % 3H1 % % K % K &

6 %& > K % O 76%% = 68 % & %

& D & %% % %% & D % D %% % & % % % & #3H1 % & % % 7 .'B8 % K L %& D =% % & & ,

('

Page 79: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%& D + & %& + =% > %%= %& > 7 > $&M 13$22 8 !% '. F ' %& &2 %& !% '. F ' & # K & & K 7;'837;*8 >

# > 2 K % D & & %& D % A

.

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Page 80: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(

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;'9

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'.

. ' ;')

' '.

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0 '';/ - 6 "7 #'

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6 ! %'. & =% %%& %& D & =% >% # % % =% %& > %& C+< %& L > %& = D % =% % % % + H & % %& && % %& & &

-$ ! ! 2

2 K 7;/8 3H1 % =% % K 3L K

'';/ - 6 "7 #'

Page 81: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

7.''8 # & 1 7 %8 K % % % $ % K 7;/8 & >3H1 & %%

( . ;'4

. & 1 K . & K

. .

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# = &

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Page 82: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# K & &K & =% % %% 2 % %& # C < & & % A

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78 K 7;.;8 & P

7&8 K 7;.)8 & P78 K 7;./8 & &

'

6 % & 7 8 K % ' & & 3H1 % %% K 7;)8 % 1 K

K 7;'8 7;/8 7;)8 N K % K # % % %& 1 & % % K

# % = &

1

(

.

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Page 83: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%% & %%=

'

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&- &-

&-

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#

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7 &8 & 7 & ' !8$ & 1

K 7;.;8 H1 %%= 7 % 8

(

.

.

$$

(

;;.

& & K % H1 %%= 6 &2 & % &

1 #' #' ' -'/ -'/ 3

Page 84: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& % & & & & & &2 & K 7.('8 %% &2 > & K 6 !% ' = +

K 7'48 !% ' % &

. ;

;;;

K &1 &

'

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;;/

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= ' +

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;''#

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;/B

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B B B ; B B

B B B B ; B

B B B B B ;

;/'

'' .. ;; '. .; ;' # ;/. '' K K '' =% '. '.

'';/ - 6 "7 #'

Page 85: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%% K 7;;;8

* $* $B* $B .

;''#

;/; = $B

$B

.

.

.

'

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;/9

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'B B

B

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B

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& ;/* K 7;;B8 7;;.8 7;/;8

= A

# 8

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;/( K 2 + !% . 3L K 7K .(/

1 #' #' ' -'/ -'/ 3

Page 86: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

.(98

% &#&

&# &

/ # $B .

;''#

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Page 87: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% # 1 % K 7;.98

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=

#

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1 #' #' ' -'/ -'/ 3

Page 88: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

#

% &#&

&## &

&## &

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Page 89: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

:- ;- ' - '

# =% % + 3H1 % % % & =% % %& = % . L & %% & =% >% % % . 2 >2 % %& + % % %

% % K> 7 8 % =% %& %& D

/ (!

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;)4

L & # % %& D %

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Page 90: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1 6 % & &

;4'

# & %%% % , %& %& %& % 2

>% N & = . K 7;9/8 7;)98 % % # . & % %> 6 & + % % % %K & - %

85 )+ !

# % & L 7 8 & % # % %

% K & % & > D &D';'9.;/B % %% & & %

! * !

# + 2 % & , ;' 2 & 2 K % & % &

h3

h2

h2

1

2

3

# . + , "

:- ;- ' - '

Page 91: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%& & & &% %& % + > % % & %& : %% & %% %& 7'8 = % 7.8 > % =# %% % % # K % %& % - % %& - % % 1 & & > %& 2 %%

= & %%

&2 & 3H1 % 1 % % L P %% % > %& & 1 78 % % 7&8 % % # & %& % , %& & A 7'8 = % & & P 7.8 % = & % & % # 3= & % %&

L 6 = &2 > %& % 2 % % + N % %& , %& = % L 9.

8 A')#B /C9 ' 6 7 ''

% % % & & % % $$ %& !% '.F ' 7!% / %& % 8 % %& %& & % >+ & & % 6 % $ % 6 % & % % % : =

1 #' #' ' -'/ -'/ 3

Page 92: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K & > , % 1 K %% , 1 D %& % K % K 7;/(8 7;9/8 7;948

- %' /

# '

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;4.

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K 7;4.8 + &

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6 # - , K A

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A')#B /C9 ' 6 7 ''

Page 93: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

- 2 K 7;4)8 6 % 6

/ *#

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#

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1 #' #' ' -'/ -'/ 3

Page 94: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%% % = ! & % > % ;B

%+ K 7;*'8 L & K % ;B & L & ;4 # % >% K - # - & & >% %& % >%

1 K % 6 2 L 7K ;*.8 K 62

/ *#

* '.

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#

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%

= '

, /

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D D + # % & , ;. 6 = L L & 1 %& %& & % 1 1

' D & %+ K =% & & &

'

Page 95: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

. % D & & %& = & % % & & + & & & %

& = %= %& = , ;.

" A & %

" A 6 % 2 = %% = %& D ! $ + & 0 12 /4 & % 99 # % 1&

% & %& &1 % 1 L %& D L = " & % %

&

, 9

$ & D % + L %& =

SIDE(Free-stream)

INLET(Free-stream)

EXIT

SIDE(Free-stream)

SLIP or NO-SLIP

X1

X2

a b

u2 = 0t1 = 0

(parallel flow)

tb = (τ11, τ12)a

(A)

(B)

# 0 2

1 #' #' ' -'/ -'/ 3

Page 96: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

' # * A " & D 1 & % &2 "& %& D

. # )* 7 8A D %% & % %+ K 2 > & & & % %& D %& %&

; A # %& # 2 D %& & & %

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, '!! $ 2 $ 1& !

+ & & 7'8 7.8 % " &

B 2 ;*/

# B 2

7;*98

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%% !$ %% %>

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Page 97: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & K > K 2 K 7;./8A

'

.

B ;*4

K 7;*/8 , >2 % & %+ # % &W %

B ;**

& = 5 & &

+

;*(

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;(B

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K 7;(B8 % ; + % & % & % . S K 7;*)8T # 7 '.4) F ' %% !$ %&8 & % % , D & % %%= & &

1 #' #' ' -'/ -'/ 3

Page 98: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

> -'' ; #;- #' ) -'/

% > >% %& & D % 6!6BB'. # %& + , ;;78 7&8 # 2> + % & ()( '*./

1.500

1.250

1.000

0.750

0.500

Den

sity

L.E

.

0 500 1000 1500 2000 2500Iterations

Multi-step1.500

1.250

1.000

0.750

0.500

Den

sity

L.E

.

0 500 1000 1500 2000 2500Iterations

Single step

(d) (e)M = 1.2

1.5001.4501.4001.3501.3001.2501.2001.1501.1001.0501.000

Den

sity

at L

.E.

0 250 500 750 1000 1250 1500No. of iterations

Multi-stepSingle step

(c) M = 0.5

(a) (b)

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-'' ; #;- #' ) -'/

Page 99: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & & K B9 & =% %& # % = $ % & & % K 2 6 %% & %& !$ L & , ;;78 % %

& L & > >% & , & '. D & % L & 7;49;8 74;9'8 & %+ = 6 , ;;78 78

1.250

1.000

0.750

0.500

0.250–50.00 –40.00 –30.00 –20.00 –10.00 0

Distance X

Den

sity

T–G scheme (Cs = 0.0)T–G scheme (Cs = 0.5)Present schemes (Cs = 0.0)

(a) (b)

(c) (d)M = 0.5

# 8 - 4! : ! 8' #$ 3 * ! 0 ! *) #$ 3 * ! 0 ! *)#$ 3 * ! .- ! *) #$ * " "

1 #' #' ' -'/ -'/ 3

Page 100: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

>% % % # >% & >% & D %& , ;/ % >% &

7+ B98 & & #3H1 & !$ % + L #3H1 % & & & L !% % & 7, ;/8 #3H1 L !$ + L

5 # ''

# !$ % K D !% & > >% D % %% >% L D%% 6 % % & % 6 & % !$ = % D %& >% #3H1 % %& %& %& D %& > %&

!'

' 6@ ! 31 K 2 "2 33 4/93).'()*

. 6@ ! " %%= 31K 2 "2 35 ;/'39; '()(

; H ! H , %& 31K 2 . 8 /);34* '(4.

/ H H 5& ? , %& D D % K % % ! # !6 $&& 78 0

,* '(4*9 @ H : : U% , 31 K & % "2 2 2 2 2

55 9;34; '(*.) H # ! 5: : ! % 6 + + %& 31 K 2 2 2 2 ,

6 9943(* '(*/

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Page 101: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

4 " , D 2 2 2 2 , 8 (*'3(; '(*9

* @H 5 5@ %1 6 K> 3% =& % % "2 2 2 2 2 8: ';93/( '(*)

( $ 5 #1 : +

%& 2 2 2 2 , 9 )9(34B '(*)'B $ 5 , D"2

, 29 ;/(3** '(**

'' # + D % #2 2;(' 2 8 .993); '(**

'. H5 66 $ 5 : D % 2 2 2 2 , ;

'')9344 '(*('; $ 5 #! @ @ 61 >% =% +

% D %& 2 2 2 2 2 56 )493() '((.

'/ 5 5 " ! %- %& 31K 0 285, ')43*; '((;

'9 $ 5 # % >% +

%& D "2 , 33 4.93/4 '((;') !$ ? 6 % + %>

& D "2 2 22 ;9934B '((;

'4 H 5 # 6 + % %&31 K + 2 2 22 , 27 ;/(3)/ '((;

'* $F 66

K & =% + 2 . 38 9(;3)B( '((/

'( 5 1 6 6 ,

D # & 2 2 2;4*93*') '((/

.B H # ! 6 ! 6! 6 &2

U7'8U7'8 %& D 2 2 2 , 32 *;439)'((9

.' ?# H 66 = % > 2 . 52 99'3). '(()

.. 65 ! # - + "2 2 2 2 25 (B(3.' '((4

.; # - ,

>% 2 2 2 2 . , ,* :'((3..B '((*

./ - H $ #> D %

& L H1 "2 22 2 2 297 ')43(B '((*

.9 H 6 1 %

%& D "2 2 2 2 26 ;;93/) '((*.) @ $ 5 ! 6 6 >% %&

31 K %3 2 2 22 , 3: ';('3/'( '((*

.4 $F 1 66 = % D & 2 2 . 63;/(939B4 '(((

1 #' #' ' -'/ -'/ 3

Page 102: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

.* "! 0 12 5 ! D , " , - 6 ! 2 @

?1 'B'3'; '((9.( "! 0 12 5 ! 6 %& %&

D # % & 2 2 2 2 , 3, *)(3*9

'((9;B "! 0 12 $F 5 ! FR 2K2 6

%& %& D 3 # =%

2 2 2 2 , 3, **43('; '((9;' "! 0 12 "2 6 % & +

K 2 2 2 2 , 3, 'B)'3*B '((9;. "2 "! 0 122 % +

" / < !G '((9;; "! 0 12 6 D !%& %&

& 2 = 2 "2 , , & * /(3

99 F 2 " '((9;/ 5 ! FR 2K2 "! 0 12 6 % %&

DA $ %& 2 = 2 "2 ,

, & * /B(3'* F 2 " '((9;9 "2 "! 0 12 # & %% &

2 = 2 "2 , , & * '9/;3

9. F 2 " '((9;) "! 0 12 $F 5 ! % & >

% O& %& D 2 2 2 2 ,35 '3.; '(()

;4 "2 "! 0 12 6 % + %& H, H 78 , ?1 )'3*/ '(()

;* 5 ! FR 2K2 "! 0 12 H %& %& D 3 6 >% 2 2 2 2 , 37';3;. '((*

;( $F "! 0 12 # 2 5 : H %% % % D 1 2 2 2 2, 37 943*B '((*

/B 5 ! FR 2K2 "! 0 12 6 %

%& 31 K 2 " ", - +* 8==> 0 2 ;;'3/4 + & '((*

/' "! 0 12 !>&>% 7!$8

%& D %& 2 2 2 2, : ()(3(B '((*

/. "! 0 12 5 ! FR 2K2 "2 !>

&>% P # 0 2 ""<# ",- 8==> 03 % %% /3') 6 H

/; "! 0 12 !>&>%

P %& D %& 0 2 ""<# ",- 8==> 03 % %% '43.' 6 H

// "! 0 12 "2 # !$ 7>&>%8 D # 2 #2 + # 2 .

;3'. '((*/9 "! 0 12 @ 5-1 5: # # =%

2 2 2 2 65 9)93*; '(((

!'

Page 103: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/) "! 0 12 5 ! FR 2K2 # & %%A 6 N D %& 2 2 2 2

, 52 ;9(3(. '(((/4 "! 0 12 @ 2 @ !%& %& DA

"2 2 2 2 2 7: 'B93.' '((B

/* "! 0 12 =% >=% %& >%& D K + % + =?;4 ! # '((B

/( "! 0 12 , % D > # " 9)3)' H ! '(('

9B "! 0 12 @ %& Y = 2 2 2 2 2 53 ''*/3.B; '(('

9' "! 0 12 @ 6 =% >=% %& %& D 2 2 2 2 2 58 /9434( '((.

9. "! 0 12 " &2 !$

= % 2 2 2 2 2 7 %89; 6 @ @ % ,

K !>4!?34 '(*9

9/ , $22 @ 1Q " &2 + %%= 1 %& @ # 1& 2, F & & '(*/

99 #! % 6 D & 2 2 2 2 , 26 9*43)B* '((.

1 #' #' ' -'/ -'/ 3

Page 104: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(-'/ ' 3 9 ; 3

8. (' / 2

# %& %& D % D , % &1 % &- % % > D & %%% % & = % D & %%% % >& &% 6 &D % &- & F ' N

%& % K + = %& D% D & 7> 1 D8 !% 7 !% '. F '8# L K %& D

%& D % & K K 1 K K & % % % %& D K # % K D

& !% ' ;P % & %& %&

"

'

.

/'

. &1 %& & > % 2

Page 105: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

"

( /.

& + D D=

/;! % & % A

//

& % P %+ 78 % & % ( % & % & 7K ''.&8

.;

/9

& & + K & % = % & 1 % % %& %& K & !% '. F ' !$ & &1 %

% %& 1 1 K & % # K %& & &>

% %+ # K & %

/)

3L K % !% . & % 1 & K 1 % %& D & K 7%+ 8 & % %& %

1 % K % N !% 9 & L % > & & % L % & % % &

% %> 1 & % % %& & %% + %

(-'/ ' 3

Page 106: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% % > D !$ & !% ; % K %% & $$ & !% '. F ' %& & = % > % % & % %

2 & % = % D %% + K & >- , %& H1 %%= & !% 4 F '

80 () -'/ 3 6- 37

& %& K K 7/'8 7/.8 &

B /4

'

( B /*

# K % +

'

'.

.;

;/(

% = 7/(8 7/48 K

.

. B /'B

%%% & & & !% 4 F ' , D % & A

/''

() -'/ 3 6- 37

Page 107: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1 F ' % & %% +

% K F ' &' , /' =% % % " & % =

= & + %& % > K 7/*8 + > % %

.

.

/'.

+ 7/(8

' '.

.'

B . .;

;.

B ; ;'

';

B /';

# D % & = % + % + K 7/*8 K

7/48 7/';8 K

'

.

B /'/

% &

(

/'9

#

B /')

'.

% %+ &%

'.

/'4

# & 1 = % = > D % >1 $ K % & % + &

(-'/ ' 3

Page 108: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# 8. 4! 1

() -'/ 3 6- 37

Page 109: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%& %+ D ./ :% K % & % & , /. =% D ;

%& & % %

(;

% K 7 8

'. .' .; (; B

> & =% D . & % K >-

% >%% N

Movinggrid

V /Vj r0

s

R0

R0/r0s /r0

β

= 1.6 = 0.8 = 50.5°

β

# 80 2 4! " * @ "" # - * A/$

(-'/ ' 3

Page 110: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

8 $ " #' ' -'/ ' '-'/ 3

-$ 5!

, %& %& & K + =% % > % !$ >% 7!% ; ;;.8# =% K & % % % 7 K 8# & & % % &

!% ; % &K & % % L > # % %

% & ! &

'

/'*

%& %&

. .

./'(

K & & = %# =% % + & + # %& 1 - %

& 94 # & & % 7> % 8

# & L 5 & % # %& & & %&&

H 9 K L 5 & % + + , /; & +

# %

1 % 2 %&

2

$ " #' ' -'/ ' ' -'/ 3

Page 111: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & > L 5 & B % 1 D 5 & 9BBB , // % & 2 , /9 L 5 & , /) %

5 & , /4 % % & >

L 5 & K 2 71 D8# & & & !$

H 9 + L + 7'.' '.'8

85!

1 !% ; =% % & K & % + # =% % 5 & & & % & & & % & K 7/'*8 %& 5 & 9BBB K>% * =% # & , /* # &

u1 = u∞, u2 = 0

u1 = u2 = 0 u1 = u2 = 0

u1 = u2 = 0p = 0

# 8 6 * * *

(-'/ ' 3

Page 112: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& K 5 & 5 & 'B BBB , /(

/ (! . !

%& %& %& =% & % % 2 & > + K

'

.

/.B

> & . + # + & % ( %

1.0

0.8

0.6

0.4

0.2

0

x2

–0.4 –0.2 0 0.2 0.4 0.6 0.8 1.0u1

'CBS'

(a) Stokes flow, viscosity 1

1.0

0.8

0.6

0.4

0.2

0

x2

–0.4 –0.2 0 0.2 0.4 0.6 0.8 1.0u1

'Ghia''CBS'

(b) Re = 400

1.0

0.8

0.6

0.4

0.2

0

x2

–0.4 –0.2 0 0.2 0.4 0.6 0.8 1.0u1

'Ghia''CBS'

(c) Re = 1000

1.0

0.8

0.6

0.4

0.2

0

x2

–0.6 –0.4 –0.2 0 0.2 0.4 0.6 0.8 1.0u1

'Ghia''CBS'

(d) Re = 5000

# 88 6 * ' * " B* # $

$ " #' ' -'/ ' ' -'/ 3

Page 113: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 !% ; % =% %> 1 % N > & & =% % & & & %& L = = # & 'B =% % L %

88 ';:

# = & & % % 7!% ; ;)8 D % &1 % # & , /'B78 , /'B /'' & = & !% ; , 1

1.5

1.0

0.5

0

–0.5

–1.0

–1.50 0.2 0.4 0.6 0.8 1.0

x1

p'CBS'

(a) Stokes flow, viscosity 1

–0.01–0.02–0.03–0.04–0.05–0.06–0.07–0.08–0.09–0.10–0.11

0 0.2 0.4 0.6 0.8 1.0x1

p

'CBS'

(b) Re = 400

–0.02–0.03–0.04–0.05–0.06–0.07–0.08–0.09–0.10–0.11

0 0.2 0.4 0.6 0.8 1.0x1

p

'CBS'

(c) Re = 1000

–0.02

–0.03

–0.04

–0.05

–0.06

–0.07

–0.08

–0.09

–0.100 0.2 0.4 0.6 0.8 1.0

x1

p

'CBS'

(d) Re = 5000

# 8< 6 * " , B* # $

(-'/ ' 3

Page 114: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Streamlines Pressures

(a) Stokes flow, viscosity 1, 9600 iterations

(b) Re = 400, 4400 iterations

(c) Re = 1000, 6100 iterations

(d) Re = 5000, 48000 iterations

# 8= 6 * - B* # $

';:

Page 115: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% % & 1 % 6 % & =% !% ; ;)

8< 1 -) '4

% + !% '/ '9 F ' & & K # % & = D % %& % + % % # % & & % %& D 5 ''3)( & + % % D

)+ .

L %%

1.5

1.0

0.5

0

–0.5

–1.0

–1.50 0.2 0.4 0.6 0.8 1.0

x1

p

'10x_uniform''40x_unifom'

40x_non-uniform'

# 8> , - 4! * # $ *

(-'/ ' 3

Page 116: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

+> 7 8 > + % & 2 # + % =% %& & + & + # & & " ;.;;9'9. & & + %

x

u

u

# 85 6 * C B* 8

1 -) '4

Page 117: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% D %& =% > %%# & >

> # 1 > ".

x

u

u

# 8? 6 * C B*

(-'/ ' 3

Page 118: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& 7 .. 8

..

. .

.

./.'

+

2 % %& .. # 1 & =

h

h

hh

u

u

u

u

tn

u

# 8.@ 2! ! " + * B

# 8.. 2! ! " - ! " B

1 -) '4

Page 119: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% 7 , /'.8

= '

*..

./..

5 %

5 ''.B

..

./.;

=% 7/..8 7/.;8 = 6 F ' % % K & & > %& K & # 1 &

..

. /./

# %% & =% 7/./8 % %& % %

..

. /.9

X >%+ % &

N K # 2 +> > % & % $ %

x1

x2

n1 n2

emax

Exact φ

Linear φ

hn1, n2, nodesh, element size

# 8.0 9 !

(-'/ ' 3

Page 120: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# = % %& 7 >8

.

/.)

+ K # % % =% # 7 8

& 7 % 8 %

& /.4 2 & + & # & %%= L $ !% '/ F ' & %

+ % % % & % % > % % % % & %% K + % % & %%= % , K + & % & # % K !% '/ F ' & % & & & % & % K" % +

K & 6 = & % % %

% = %%=

.

&

.

/.*

1 -) '4

Page 121: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# %%= & K %%= &

&# &

.

.

B /.(

& % .

%'

&#

.

%'

&#

&

/;B

% = &

% &#& /;'

& C%<

K C > <% 1 & # + %% % '(*4 & .. & D %&4B4; $ %& & % & 6 1 & % # & = & ;(9;9) 0 12 9B )9 %& D = & % & "& % % D % = & + + = 2 & & # %% 1 . K = , /'; ,' ,. = % %

# K & %

.

.,..

.=

.,.'

/;.

#

# =

.,..

.,.'

#$$$$$$% /;;

% & % % & =

(-'/ ' 3

Page 122: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& % %+ A

' , . & % & =

; ! 2 = K 7/;.8

/ ! = 2 7K /;;8 & = &

9 5 & 2

# & % N K % &1 % %.. =% % # % 2 % &1 & % %

7% %& D8 = &2 % # = & %% & 1 2 D & % % 2# % - & & %%

% % & 1 = % # & >

& &1 & & >% K & % %

x1

X 1

X 2

hmin

s hmin = hmax

α

# 8. + " ,

6 & # & & 9/ 9(3). )93)4 4/3*9

1 -) '4

Page 123: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/ ) + .

# D D %& % & > & & K & %& , %& %& %& =% %% % &

/;/

= 2 7 28 # & =% & 2 % = K 6 % = 2 & " + 6 % = 2 && 0 12 9B =

= /;9

& B ' & = 2

1$

& + % & & + # K & & % & %% # % % & N % & & %& %& D %& %& D + % 7F %& D & K & 8" & & & &

% % & ! % & & %& & 9().)( =% &

(-'/ ' 3

Page 124: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# 8.8 6 * B 8 " "

1 -) '4

Page 125: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(!

=% %& D %& &> % % + %& D % = /*' **B , & & & & % , /'/ > & % & + %7, /'/8 & + % & + 7, /'/&8 $ = % & 1 H 9 7, /'/8

(a) Final adapted mesh, Nodes: 1514, Elements: 2830

(b) Streamlines

(a) Final adapted mesh, Nodes: 1746, Elements: 3293

(b) Streamlines

(c) Pressure contours

II Gradient based refinement

I Curvature based refinement

(c) Pressure contours

# 8.< 2! ! " B > " "

(-'/ ' 3

Page 126: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 = & D &1 % % , /'9 + & & % 6 & & % % &

+ & % N F ' & % K %&

8= 1 -) #' ' ' -'/

% % % % 1 "& + & 7 ) + 8 % & % %& %" K L % & /B & A = & % , /') %& +=

& !% '9 F ' % & &

1/'/.

8> (-' /# )) '

% L &2 & !$ 5 & D # %&D % %% L %& D %& # D &2 D L 5 < &'BB 9BBB % , /'4 & 5 & # L &2 5 'BB 5 9BBB % & &2 # % &2 S %% . K 7;.;8 7;./8T %& 5 < & %& % &2

85 " 3 9 : - '

: ' %$ !

%& D % = %& /. 7 8

" 3 9 : - '

Page 127: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

#8.=

0

4

!

*

B

8

*

%

"

&

(-'/ ' 3

Page 128: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K 7/'8 7/.8

B /;)

( B /;4

# & % &

.

;

/;*

%& %& %A

78 % &

With stabilization Without stabilization

With stabilization Without stabilization

(a) Re = 100

(b) Re = 5000

# 8.> + ," * B*&

" 3 9 : - '

Page 129: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

7&8 & 78 & %

K !% ' ;

: ( ! 2

# 2 & / % %%=>

& &# /;( & % K 7/;)8 & % %

'#

B //B

& % % %%& K = 2 & & & & *) 7 !% '. F ' 86 % =

% % % % 2 & = 2 # % D '(4B*4*(

(B(.

# 2 K &

/ *

*# .$

#

,

//'

% 2 $ =

/ #$B &

* &#&

&#

&#

//.

% & % # 1 (B(.

'B4'B*# & & % % >

%& D # %%& D D & & %% % = & & & % & # !% '. F ' & % , /'* &

(-'/ ' 3

Page 130: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

+

+

O (h ) (T3B1/3C)

O (h2) (T6/3C)

+ O (h2) (Q9/4C)

(a) Continuous p interpolation

+ O (h2) (T6 B1/3D)*

+ O (h) (Q4/1D)*

+ O (h2) (Q9/4D)*

+ O (h2) (Q9/3D)

+ O (h) (T6/1D)

(b) Discontinuous p interpolationVelocity nodePressure nodeDenotes elements failingBabuska–Brezzi test butstill performing reasonably

*

# 8.5 - * * "* "

" 3 9 : - '

Page 131: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% (; D (/() & % % & K B %

% D % % % % % %

1 %& % # & = %& 1

D & + + D %%

8? %; 3 9 -' '#

; 5% % ! !

D % & % & % #% & % =% %

B !' //;

B B 3 % ! % & + K7;;/8 7&8 % # & & & % &

K 7;;;8 %+ & %%% % , /'( #& =% K 7//;8 1 " , /'(7&8 & % %

% & %& 1 , , /'(78 % $ D & = & & # >% D > & # &

!

///

(-'/ ' 3

Page 132: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# % % % D % B %

//9

" & % D

//)# 7 D8 & & &

% K 7//'8 & & = /& %

/ / / / //4 & %

σ

ε•

µ

(a)Linear, newtonian, fluidε•

σ ∝ εm

σ

ε•

µ

(b) Non-newtonian polymers

σ

ε

|m | < 1

µ = σ/3ε

ε•

σ

ε•

µ

(c) Viscoplastic-plastic metals

σ ∝ (σy + γεm)(Bingham)

γ = 0(Ideal plasticity)

σy γ = 0

γ > 0

ε•

# 8.? - *

%; 3 9 -' '#

Page 133: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# % & % 7 F .8 # K 7//'8

1

#

,

//*

1 1 #

#

' 1'

,

1 1 # //(

& % & % % 7 % %

2 + 8 % + + K & L ' ' % 7 8 # + > D %% %

'(4B(4(( 6%% % &K & %*('BB'.4

%% N 2 & D & & % 'B) % = 7 % + 8 -+& # & & % % & )* % %> =% # % & C>%<'B9'B) %= %# % %

% %% & # ''9 '.* '.( % +

; 5 !

# %& #! )* + D , /.B78 %% & & += % % % , /.B7&8 % % > %& % + % 1 + & % &

(-'/ ' 3

Page 134: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

C< D %& , /.' % = % & #& /' , = = & ';B & & D L , /'* (; # + % %& > D % &

% 7 % 8 % & %& K # & %%% K K 7/)8 K + , 1 & %&

%+ %

/9B %+ & 1 %

Prescribedvelocity

Prescribedtraction

Extrusion

Rolling

(a) Steady rate

# 80@ 2" **

%; 3 9 -' '#

Page 135: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Moving mesh

Extrusion

Rolling

Forging

Cutting

Sheet forming(deep drawing)

(b) Transient

# 80@

(-'/ ' 3

Page 136: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& &

/9B&

& K 7'(8

/9B

62 !% % = , /.' % => %& 7 % 8(;

' 78 . 7+ 8

% = , Z !78 = , Z !78

#)O' .* (B'B '.B. )4*' .9 ((BB B4; 94(4'#)$'O; ;' B/;B .B;. 494) .) .9*B '4* 4*B';#)$'O; .( B;'B '.9. 4;B* .) ..(B ')) )';(.#)O;! .4 (B.9 *'9 *4). .9 (49B B)4 *99;*

= .9 *BBB BBB [ .9 *BBB BBB [

CL

MESH I

CL

MESH I

v = 0u = 1specified

Slip boundary

Free boundary

# 80. # '$ ! *

%; 3 9 -' '#

Page 137: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& K 7'.8

./9B

% L % K 7/9B8 & & & %&

7 K /)8

( B /9'

# % %& & &1 & % 1 D + &1 % 1 K % % !% . % + '(4;

'(4*'B.'B; & % 'B(''B , /.. % % > %& 'B; %& & % %

& & 1 N % % '') # % % = N %

; - ! %$ $

# % %&& %& #%=% % & , /.; /./ % %% # & %

+ % % & 1 # + & & & & & =%

/9. % % % &

K 7/9'8 %+ %%

( ( B /9;

% 1 %> % =% % % !% ;

(-'/ ' 3

Page 138: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

9 1x

= 2.

25cm

9 1x

= 3.

25cm

9 1x

= 4.

9575

cm

9 1x

= 5.

915

cm

9 1x

= 6.

15cm

T = 400K

T =

460

K

Tem

pera

ture

con

tour

s fo

r ent

ry T

= 4

00K

at in

terv

als

∆T =

4.0

K

T = 700K

T =

722

K

Tem

pera

ture

con

tour

s fo

r ent

ry T

= 7

00K

at in

terv

als

∆T =

1.5

K

y,ν

30.2

ν tan

g =

ν tro

ll = 2

8.73

cm/s

k∂T

/∂n

= α 2

(T–3

22)

k∂T

/∂n

= α 1

(T–2

95)

T =

T1

0.88

9

2.25

3.66

52.

25ν

= 0

∂T/∂

n =

0x,

u

0.633

∂T/∂

n =

0

All d

imen

sion

s in

cm

k∂T

/∂n

= α 2

(T–2

95)

C L

Hor

izon

tal

Verti

cal

(a) G

eom

etry

Nodal points

20

301.

0 –1

.0–3

.0cm

/s(b

) Vel

ocity

pro

files

(c) T

empe

ratu

re d

istri

butio

n fo

r diff

eren

t ent

ry te

mpe

ratu

res

#800

-

*

"

!

"

>/

%; 3 9 -' '#

Page 139: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& % 1 % & % %& =% , /.;*( %

& 1% 1 & 6% & %& & % 3 & 1% % =% , /./ %&';'';.

% % % %& & 2 %+ & % %& % %&

!% '9 F ' % =% & % ';;';/ , /./ %

U

(a) t = 0

u∆t

U

(b) t = 15∆t

30%

U

(c) t = 30∆t

60%

U

(d) t = 45∆t

90%

# 80 #* $<> ; != 9* ) #$ #$ #$ #$ ! # " $

(-'/ ' 3

Page 140: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Initi

al m

esh

Upd

ated

mes

h 63

6 D

OF

η =

15%

Upd

ated

mes

h 12

00 D

OF

η =

18%

Adap

tive

refin

emen

t 808

DO

F η

= 11

%Ad

aptiv

e re

finem

ent 1

242

DO

F η

= 10

%

t = 0

t = 1

.1s

t = 7

.7s

#808

#$

"

!

#

"

"*

$

%; 3 9 -' '#

Page 141: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% % & # %% & =

&- # % % % " % > 6: 7& 3 8';9';( %& < + & K

644

CL‘Effective’ strain (ε) t = 2.9 s

CLTemperature (T ) t = 2.9 s

0.4

0.3

0.2

0.1

2 4 6 8 10 12 14 16Time (s)

Load

(MN

)

(c) Load versus time

(b) Contours of state parameters at t = 2.9 s

0.20.2 0.8 0.8

624

623624624 624643

649

# 808 #$ ! */ 0?D3 2" =<

(-'/ ' 3

Page 142: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

r b =

1.9

625

in

Punc

h

r c =

1.9

25in

Blan

k ho

lder

1.94

375

in

(Initi

al) 3

.60

in

0.035inRA =

1.

875

inµ 1

=

0.20

r d =

0.2

5in

Die

Geo

met

ry a

nd fi

nite

ele

men

tdi

scre

tizat

ion

of th

e bl

ank

usin

g lin

ear e

lem

ents

H =

445

T

µ 2 =

0.2

0

60 50 40 30 20 10 0

Stressσy (kips/in2)

0.05

0.15

0.25

0.35

0.10

0.20

0.30

Stra

inε

Dis

cret

ized

stre

ss-s

train

cur

ve

100 80 60 40 20 0

Punch load (kN)

20

40

60Pu

nch

trave

l (m

m)

0 Punc

h lo

ad –

pun

ch tr

avel

Num

eric

al

Expe

rimen

tal

0.5

0.3

0.1

–0.1

–0.3

–0.5

–0.7

Strain

20

40

60

800 Orig

inal

radi

al d

ista

nce

(mm

)St

rain

dis

tribu

tions

for p

unch

Trav

el =

60

mm

Expe

rimen

tal

Rad

ial s

train

Thic

knes

s st

rain

Circ

umfe

rent

ial

stra

in

z =

9.20

mm

z =

17.9

mm

z =

28.7

mm

z =

34.7

mm

z =

48.5

mm

The

arro

ws

indi

cate

the

velo

city

vec

tor

at e

ach

noda

lpo

int

µ 1 =

µ2

= 0.

20

Flat

bot

tom

pun

ch. D

efor

mat

ion

atdi

ffere

nt s

tage

s

#80<

3

!

"*

4

=

%; 3 9 -' '#

Page 143: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K 7/9.8 %

% 7 %% P % % %8 & D K & %%

& % % + %%& $ %& %& & % # %% & & '/B3'9; %% & & & , /.9 /.) % %&

(a) Mesh of 856 elements for sheet idealization

X

Y

(b) Mesh for establishing die geometry

# 80= 2 " * 0 " ! 0 " 4 ! 8 0 0 " ! 1 ! 8/) ?> ! ! <8:!B # ( $=/

(-'/ ' 3

Page 144: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

; !

/(' L %& % & -+ & # & # & %& % " %& C% >&1< % %=

t = 900 s

t = 2400 s

t = 4280 s

(c) Deformed shapes of various times

# 80=

%; 3 9 -' '#

Page 145: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% % %& L & % '') '(*/ & D D & %& %& % D && # % %& K %= & &- = 1 ! # ,&'9/'); & "& &- & % % &1 & &

8.@ ' - --' ' '#

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%& % % & % 1 %& & % % # % % & & %%% % & N & 0 12 ')) , /.4 % & % & % = + % 7, /.4&8 % % K> 7, /.48 % # + K !$ + 7, /.4 8

(-'/ ' 3

Page 146: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, /.* & > %& & % & $ $ ')4

8.. # ''

# =% %& %% % =% & & 1 % % !% 9 %& %& & & %

(a)

(b)

(c)

(d)

(e)

CL

CL

CL

CL

CL

# 80> * ' #$ ) #$ " ") #$ ( ") #$ " .- ") #$ ( .- "

# ''

Page 147: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

!'

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Page 148: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

( "! 0 12 $F 5 ! FR 2K2 6 > %& %& D 3 # =% 2 2

2 2 , 3, **43('; '((9'B "! 0 12 " &2 !$

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Page 149: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 150: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

9B "! 0 12 @ 6 + % %& D 2 2 2 2 2 57 .'*(3.'B '((/

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Page 151: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

4' ! 5& "! 0 12 @ F & % A D " 5 7

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(-'/ ' 3

Page 152: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(; "! 0 12 ?! : H! %& 2 2 2 2 2 3: .'('3.B. '(*(

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Page 153: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

''/ " H : 6# 6 6%% + % 2 "2 , %% '/)39;

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Page 154: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

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Page 155: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

'9; H 2 @ : 6 = & & L % 2 2 2 & 2 #

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Page 156: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

' ' / '/ -'/ 3

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D #%=% & & & & % & " %& 1 % !% 4 D & %> %+ & %& % L % D % % # % % " + K % D % % + &D =% % % % %& & 9; 1 %& & %

7 8 D L

Page 157: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& & %& & %> + =% % K %& & %

<0 ' ' 3

#

%& % % D7K8 % 1 %& , 9' % %& P D D

Water levelSluice gate

Free surface

Floor

WaterWater

Overflow

Free surface

Dam

(a) (b)

Sea

Ship

(c)

Free surface waves

Sea floor

(d)

(e)

Free surface

Sea floor

SeaHydrofoil

Free surface

Core

Metal inlet Die

Mould cavity

Free surface

Feeder

(f)

# <. 0* !

' ' / '/ -'/ 3

Page 158: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% % + 6 D %& L &% & # L % %& % % % 1 & % " 7'8 % 7

%%= 8 2 %+ 7.8 % D & "& & > %& &

% % & # %& & 2 %& % & %%& L %%

/ % ! $! $

, 9. % %& % &

u0

x2

x1

Ship

Datum

Free surface

η

Ω

# <0 *

' ' 3

Page 159: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

31 K L % % %%= $ % & % % & 1 & & + ! L % & %

L & > & % % ''' + + % % D K '. 6 % %% % L > N % % % & = % & L K K & # % /' % % !$% & & N % & 1 7 28 # N & % D: + % &

% 1 7, 9.8 # & 2 & & % & % ;

' . ; ; 9' % % &

'

'.

.;

; 9.

K 79'8 +

;

'

' .

.

# 9;

' .#

'

.

#9/

& & % K 7 !% .8 & ' . ; ; 6 1 K & 1 % & % L % > & . !% . % & + & K % 3H1 % & %% L

' ' / '/ -'/ 3

Page 160: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% & %

; '

' .

.99

# %& &

0 !

6 % %&

# + % 6 1 2 % % 2 D %& & %% !$ 1 + & ' ' 6 K % %- ' .6 & % %

& % & %

"& % % & = % & 6 % & & - % &

( 9) $ K & & % = " %%= & %%= & K %% % % & D %&

& & & & % - % %

6 & & % K =% % %& & K & & % - =% # 1

:Q " J ';'* # =

' ' 3

Page 161: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% % & %& & & % % - & %> '( = + .B..

(!

>'# 2 1 '" " > %& , 9; 6!6BB'. %+ & > & % # %& > 1 D 9 , & B9)4. # , & +

) -(

94

, 9/ % & % % %+ =% .; '/ , 9; 9/ & K

# < " * 1 " + 4! 1 >

' ' / '/ -'/ 3

Page 162: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, 99 %& - , %+ >% & - 7, 997&88 >% %1 7, 9/7&88 , 9) %

% L 5 & 6 =% 1 7, 9)7388 6 5 & 79BBB &8 & & & = % , 9)78 9)78 ,9)78 % %+ L 5 &

>'# 3 ' , 94 % & 656 & , & B.9 # > & & & '9BB % % % # %%= ;.' BBB

(a) Surface Pressure Contour

(b) Comparison of Wave Profiles

0.15

0.10

0.05

0

–0.05

–0.10

–0.15

Z/L

–2 –1 0 1 2 3 4 5X/L

Idelsohn et al.18

Hino et al.14

Duncan23

# <8 " * 1 " + 4! #$ #$ !

' ' 3

Page 163: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

>'# 5 # =% % & & .9 / 31 K 3@11 % N 1 K %& , 9*78

1 && 6 'B/ 944 % , 9*7&8 %+ % % 'B 1

–4 –2 0 2 4 6 8Distance

0.2

0.15

0.10

0.05

–0.05

–0.10

–0.15

–0.20

Wav

e el

evat

ion

ExperimentIdelsohn et al.18

(a) Surface pressure contour

(b) Comparison of wave profiles

# << " * A* @ + 4! #$ ! #$ ! /

' ' / '/ -'/ 3

Page 164: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Re = 500Re = 1000Re = 5000

Re = 10000

0.04

0.02

0

–0.02

–0.04

–0.06

Wav

e el

evat

ion

–4 –2 0 2 4 6 8Distance

(e)

# <= " * A* @ :- 4! #$#$ 1" * B* #$ 7 B*

' ' 3

Page 165: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(a)

(b)

# <> -" 3B #$ - #$ 7

' ' / '/ -'/ 3

Page 166: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

< ') 3

#

%& %& D % K K 1 % % & 1 & % &

(a)

# <5 " #$ - #$ 7

') 3

Page 167: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & %& & & & & % & & L & % K 7/.8

( 9*

%%& & # % N =% D %& & + = N =%

'

9(

& % # & K & %%=

'

9'B

5% & K & &

( 9''

, %

9'.

& & K 7 & % 8 K 79(8

'

9';

# > & & D HL & 7 > 2 % ./ .98

) ( ;

9'/

&

)

9'9

1 L % +

9')

' ' / '/ -'/ 3

Page 168: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%+ % & D > & 5 & 7-8 % ) ) % & & D K

= D &> > & 5 & % # & &1 %& .);(

, & D & + # + D &> 753$ 8 !$ & %% %& D % &%&, 9( & K

./ $ 2 & &6 & % 2 7 % 8 # %& , /; %% 5 & 6 & D %

!$ # K % = & & 1 #& 9'./

, 9'B L 5 & 'B);'

# % L 5 & , 9''6 %& &

, 9'..9 C:< % % % & 6 %% 2 % % =

82 K !% & ./

5 K &1

- = =

S/BT S/'T !$ S/BT S/'T !$ S/BT S/'T !$

'B; ''') '''* '''4 ''4/ ''49 '')4 ;)() ;)(4 ;)(.'B/ ../; ../9 ../; 9B*' 9B4/ 9B49 '()/ '(); '();'B9 /9'4 /9.. /9.' ('.' ()'( ('9; )*)* )*)/ )**9'B) *4(4 **.9 **B) ')/' ')*' ')/( ..'; ..B) ..')'B4 3 ')9. ')/B 3 ;B'4 ;B;; 3 )((; 4B.;/ 'B4 3 .;4* .;)/ 3 3 /;'. 3 3 '/'4

') 3

Page 169: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(a)

(b)

(c)

# <? : ( - B*"

' ' / '/ -'/ 3

Page 170: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& ! %

% %& + = & %1 D2 & & D D L >% D D

% % %% += % =&1 % D &/./; % %&

θ =

0.5

θ =

–0.5

θ =

0.5

θ =

–0.5

θ =

0.5

θ =

–0.5

θ =

0.5

θ =

–0.5

θ =

0.5

θ =

–0.5

θ =

0.5

θ =

–0.5

α = 60°

g

α = 60°

g

α = 0°g α = 0°g

α = 0°

g

α = 0°

g

IsothermsStreamlines

# <.@ : ( - "* ?

') 3

Page 171: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(a) (b)

# <.. : ( #$ 8 #$ ?

0 00

11

1 000

000

WR = 0.2 WR = 0.3 WR = 0.4

WR = 0.2 WR = 0.3 WR = 0.4

(b)

ψmax = 7.2, ψmin = –13.9,vmax = 237.3

ψmax = 16.16, ψmin = –20.12,vmax = 248.29

ψmax = 16.11, ψmin = –26.8,vmax = 211.3

(a)

g

# <.0 : %6& #$ - #$ ?

' ' / '/ -'/ 3

Page 172: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

D % , %& &1 & 0 12 //

K & & % /9/) # K &2 & % /)

B 9'4

'' '

& '

'

'

;.

( 9'*

9'(

% % %& =% < /4 7 > > % , &P /*8 % %

' # 9.B & K &% # % D %# %& & % % 2 1

;*.

'9B' . 9.'

* % 2 L D D & K & 6 & K >

% D K %% !$ &/(99 =% >% & N % % % & 7 & & K 8 % K>% /4/( & 6 !$ & &2 & 5 & 75 &8 % D

') 3

Page 173: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

50

(a) Da = 10–6, Ra = 108, ε = 0.8

50

(b) Da = 10–4, Ra = 106, ε = 0.8

10

(c) Da = 10–2, Ra = 104, ε = 0.8

# <. : ( ! 4 * B*" 3*

' ' / '/ -'/ 3

Page 174: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# & > % % D 5 & # & + %

&-

.

9..

7D 8, 9'; % &

K L 5 &/) 6 & 7'B)8 7, 9';788 & 7'B.8 % >% D & 2 = L , 9';7&8 & , 9';78 9';7&8 > D # K %% >% D K

' # K & %& & % >%

<8 '/ 3

#

& D %& & > # =% D % , /') % 6 % > % & >1 %, % & &

D %% & K % & %& & & & D 5 & & % & %%= & 9))/ 78)9)) > 7:8)4)* & , % K & % & % % &1 % &

# & D K % % L % K % %+ + %

'/ 3

Page 175: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& & !$ %&)/

' %

# 5 31 K & & D &

9.; & D % K K &

B 9./

'' '

'

'

( 9.9

7K ;48

.;

9.)

5 & +> $ K % & # & & & L K %% !$ $ K

.;

.; 9.4

& 1 & 1 # & K 7 D8 % K + !$ & $ % + & &

K &

'/ '.$! 9.*

' ' / '/ -'/ 3

Page 176: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K BB( & 1 $! = 7 B/ 8 # = $! &

$!

;&

'/ 9.(

& # & 1 % K

B 9;B

K ,

&

;.

9;'

! K & % K

'

.

.

B 9;.

' & '/9 '99 . '(.3.B K '; & >K

.

9;;

# # L 5 & & % , 19)). 5 & 1 %

" # , >K & 9)

'/ '.$! 9;/

&

;.

9;9

' B')B ' B.);

9;)

, >K N ' . %% >

K & % & % ' .

'/ 3

Page 177: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% ).

' BB')9. ' .B9

9;4

' 'BB9

;9;*

. ' . 9;( . # & B B6 1 > # L

+ & K L %)(

# K 3L K !% . !$ & 6 & ). D % &1 % 5 & ;B.9 , 9'/78 %+ % =% 4B 6 & & # > , 9'/7&8

3.02.52.01.51.00.5

0

Y

0 2.0 4.0 6.0 8.0 10.0 12.0 14.0 16.0U/Uo

1 unit of U/Uo = 1 unit of X/h

(a) Velocity profiles downward of the step

k-ε model (CBS)Exp.

(b) Streamline pattern

# <.8 0 4! ! " * /8

' ' / '/ -'/ 3

Page 178: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

!'

' @F # % 2 2 2 '(4B. ! 6 % % % %& 2

1 2 "2 2 # . 6 '(44; @ $ @ ! 2 - #+-" 7' # 7

+ " $ 6 '(4(

/ , & @ ! 2 - #+-" 7' #7 + " $ 6 '(*;

9 H @ % % , /

, 38 '(*() ? # : > % 2 8> #2 .!

6 '((B4 1 " % % 2 ,

2 328 .9)3** '((B* 5 6 % > % 1 2 8= #2 # . '((.

( 5, $1 ? ! # : , > % 2 2 : #2 2 # . ! 6 '((;

'B 6 % 2 18 #2 . # > '(()

'' ! @ : : 6 %2 %

% 2 18 #2 . # '(()'. !! ! 6 & 2 D

2 2 2 2 2 2, ''9;349 '(4)'; # !% D % & 31

K 2 4 2 "2 2 # . 'B;3'4 @% '(*(

'/ # : 6 @ 6 +

D 2 : 2 "2 2 # . 6'4;3(/ '((;

'9 # 6 %& D

!=B!?>:1 '((4') 5 :Q ! ? " J 5 6 & %

=B!8>? '((4'4 5 :Q ! ? " J ,

3 ""<# ",- "2 6 % 43'' '((*'* 5 " J ! , %

%& 2 2 2 2 2 68 9B;3.* '(((

'( ! $ F D 7F",8 & 2 "2 2 5; .'B3.9 '(*'

.B 5 ! Q " J + + 2 2

2 2 . , ,* 6 .('3;'B '((/.' 5 5 : , + L

+ , - 52 ((3'') '((*

.. 5 : 5 , 2 2 22 2 67 7 %% .BBB8

.; @ # &1 >&1 > 2 , 2 239 9B43') '(*;

!'

Page 179: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

./ "! 0 12 !>&>% 7!$8 %& D %& 2 2 2 2

, : ()(3(B '((*.9 # - ,

>% 2 2 2 2 . , ,* :

'((3..B '((*.) , % , . ;

?1 '((B

.4 6 $- . ?1 '((;

.* ? @ " . % >F ?1 '(*B

.( "! 0 12 5 H > %& D #% D ,

, @ F !% .B %% .;93)46 : '(4)

;B @! 5 "! 0 12 %

0 ,* ! # !6 $&& %% /;93/4 '(4*

;' @! 5

& . 8 *'3(. '(*.;. @! !! ? , & D

% 2 "2 2 2

2 2 9; '3.4 '(**;; $ 5 , D"2

, 29 ;/(3** '(**;/ $ 5 #! @ @ 61 >% =% +

% D %& 2 2 2 2 2 56 )493() '((.;9 $F 66 , L

2 2 22 . , ,*

5 ;B93'* '((;;) ! , =

2 . !

3; ;';3;B '(();4 ! : ! ! , & = >

2 2 2 2 , 35 /43)/ '(();* ! : !? ! ! ! , &

D = > . 52 9.(39B '((4

;( ?# H 66 , =

> & & 2 2 . 62 ')';3'( '((*/B H F K A 6 & 1

2 2 2 2 , 5 ./(3)/ '(*;

/' : U #6 5K !% > !& % 2 "2 2 87 .'B3.* '(*9

/. 6 6 $- " % >F ?1

'((./; . % >F ?1

'(('// "! 0 12 6 ! ! $6 D # "

5 * # + (' ! '(((/9 F !: # $ L D %

2 2 . 36 '(93.B; '(*'

' ' / '/ -'/ 3

Page 180: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/) # - + D & % 2 2 .

6, ;(993)4 '((4/4 , D %1 "2 2 2 6: *(3(/ '(9./* H : F > L %

2 2 . 53 .';93/* '(*(/( # - &>L

+ D % 3 >

%% . 5, /';3.) '(()9B # - L % >

D % 2 2 . , ,* 2; 9)3* '((*9' 5 6 >% %% %

& D D % "2 2 2 22 298 '/439/ '((*

9. # - % &

D D > % 2 2 . 63 '.B93'9 '(((

9; , % 1

& D % 2 "2 3;.43;( '(((

9/ - # - $ D

> D % &- D= 3 "2 2 2 2 28 4)934) '(((

99 "! 0 12 , % % D 7 & %&8

9) % & % - # 2 2 ;3('93.. '(4B

94 $ : $ % 6

? '(4.9* ! # 31 K = % @# "

78 , ,* 6 6: %%

'.'3;. '(4/9( #H ! # 6 = >

K & + 2 2 2;(93( '(44

)B ! # #H , K & D 2 "2 2 3; ');34. '(4*

)' 6@ $1 , & D 2 2 "2 2 2

0 ,* '(4*). !H : $ 6 + %

& 2 , 2 2,5 /9)3)B '(*'

); 5 1 6 6 , D # & 2 2 2;4*93*') '((/

)/ "! 0 12 $F 5 ! % & >% O& %& D 2 2 2 2 ,35 '3.; '(()

)9 @ @R 2 6 L 5 5 #

% & 2 , 2 388 )93(B '((;)) A 6 & 2

+2 , 2 5, 9;(34* '((*

!'

Page 181: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

)4 5 5 & D 2 +2 , 229 ((3';4 '(*/

)* : " R & 2 +2, 2 3: /93*. '(()

)( # 2 " #& D %

; , - 5, ;9;3); '((*4B $ 6 1 6

& D 2 2 A #2 2 : )*'3*; '(49

' ' / '/ -'/ 3

Page 182: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

-'/ #;- # 3

=. ('

& % & >% D & % % 6%%> / )* D )* % & 6 % =% %& % =% % + L + '(*B % L & + 2 + =% %" + %%=

%& + %= % + K % %%= & % %%& > 2 & % %&7'B93'B4 ", K %8, %& & %&

& % & % & & & + L %% & % N % %& 2 & & & + % % 7 + 8 !% ' ; & K D

%& %& D !% / %& %% %+ %& D >% D & = B9 D 1 , > =% !% . ; % 1 + < :Q

& 1 ';* 1 % %

Page 183: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

+ + 1K + % %% #3H1 % .'B

!% . > & = > !$ !% ; % &%%= %& & % &7 8

=0 #)'# 2

# 31 K %& D !% ' % %+ K 7'./8 7'.98 ' . ;

*

+ B )'

# ' . ; ).# ' ' .' . ; ; ).&

*# B'.;

).

+# B ' . ; ). &

.

;

).

# & K & C< & % S K 7'')8 7''48T , D ;( N

);

%+

' )/

% %+ #

'

'

)9

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Page 184: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

'

'

.))

'

.))&

# & 1 K 7).8

& & K 7)'8 & %& & &

* ,

( %& % &

D N %% % &% & 7 )'.8 % % %& L %% % > % D & & & %& 2 C+ < 2 & & %% > && D % =% 31 % %> < ;(

'/9;.

''B 'B) )4

, & & & 5 < % K % 9/ !% 9 & =%

= ' 9 / -' 3

# K & & %& 31 K %& D & & & 12 /B D = K 31 %& % K & !%

; %%= & % % & % %&

' 9 / -' 3

Page 185: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

,

+> & & 31 %&, * % &

%+ 72 8 , 1 D= & 2 7 8 %+ & & & /

# = D , )' 7 ;)!% ;8 .'B; & %

2 5 & % %% K , 2 K %% % &

'

.

;

)*

% %& 7% 8 &

()(

6 & %% K7)*8 % D &

+

' )'B

%&A

78 )*

D = & % & %+P

Γs

Γu

Γu

Γs Γs

External flow Internal flow

# =. . ! *) *

-'/ #;- # 3

Page 186: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

7&8 )*

& % %&

, & & %= & %+ % 5 & K % N &1 % & %%& % + & 7 !% ; ;)8

,

% & K, * % %&

% % %& D D # & %

B, & & % D= & , / # % D 1

K D & %%=> & % 2 1 2 & ;) !% ;

=8 %' --': " #'

F + %%= & %& D %& # + #3H1 % >% >% & !% . .'B %%& !$ % !% ; & % N K & %>& % %& %& D % D %& % #3H1 =% !% ; % K & 7, ;/8 !$ %% % & =% >% >%

!$ $ %& &

%' --': " #'

Page 187: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& >% % =% >% 6 1 > %&

2 % % % & # % % % ;;/ !% ; & =% % ;;/

%% % & = %& 1 L % % # %& %& D

1 &- =

=< " -'

! + %%= & >% B = % 1 %& + % 1 % # & % & >+ 1 & %%= % K , + % % & 1 % %& % + 1 1 %

& 1 =% + 1 # % % N & & > %& & = , ' $ /'/.

# % L % 1 + & 5/; '(9B # &2 & & & + % & 1 + % :%// /9 !1 $ /) @ /4 6 + & % & % & ') /* + % # + % % &>K %& D 5 % 1 % /( & L # % + L % 1 +

% + %%= K

-'/ #;- # 3

Page 188: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& =% >% K & # % % K ' & &

'# ' -

)''

- %%% + L N % - & 1 %& , % * & K % % K - % & $ K %&

# N - & K % & % & % & % /)

- ;

.

)'.

> N % % &% & K % & & & % & !% / /96 % & %%=

& 7 8 /*

..

. %% )';

% % % % # & =% & > + L %%= # = %& & - %%= & % 7K )'.8

-

%%# )'/

- K %%= - A

- . )'9 . % .

" -'

Page 189: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/*

.

)')

& + . ' % = . B % - 7 8 # >%+ N & BB .B# & & H1 +

%%= 7 K )'' )'; )'98

'# ' %'

.

%% )'4

K 7)'98 % & & & K # & N # >L 2 L L K % 6 &% &> + % 7 K )'' )'.8

'# ' %'

;

..

&#

&

)'*

# %& 6 &

" # - K + '(*) & 9B & 9'9/

6 & ! /( >% 1 % % + N -& & L & 3H1 1 & % 1 % & # & N &

-

)'(

% & & & L> 1 % L %% %&999)

== " -'' :- ' ' 2

# % % & %% > %& % % =%

-'/ #;- # 3

Page 190: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

,, 9 $ !

# > %& % L & & & % B , ). % L % # %& = % & 94 '

,, 0$ % $$ 22

K % & - - >

1.000

0.425

t = 0

ρ

0

u Lumped mass

Consistentmass

2.5

2.0

e

t = 18.5

# =0 0 B 8E 0 " E # 8$ 6 6

" -'' :- ' ' 2

Page 191: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

' 9*

- 'B .9.'.9

B 9 ).B

# % D D D % , ); %&

2.0

1.5

1.0

0.5

00 1.0 2.0 3.0 4.0

x

ρ

(a) Subsonic inflow and outflow

2.0

1.5

1.0

0.5

00 1.0 2.0 3.0 4.0

x

u

2.0

1.5

1.0

0.5

00 1.0 2.0 3.0 4.0

x

ρ

(b) Supersonic inflow and outflow

2.0

1.5

1.0

0.5

00 1.0 2.0 3.0 4.0

x

u

2.0

1.5

1.0

0.5

00 1.0 2.0 3.0 4.0

x

ρ

(c) Supersonic inflow–subbsonic outflow with shock

2.0

1.5

1.0

0.5

00 1.0 2.0 3.0 4.0

x

u

ExactCL = 2.0CL = 1.0

0.75 0.50.0 5.0

a/2u' u2

C1C1

# = 9 4! " ,, 2* ( ,

-'/ #;- # 3

Page 192: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

9BB % , % D & D 1 :%>% + L , );78 C < N :%

(a) Structured uniform mesh

3.00.6

1.0

Inflow

2016 elements1089 nodes

y

x

t = 0.5

t = 1.5

t = 2.5

t = 4.0

(b) Solution – contours of pressure at various times

# =8 0 4! ! = # 7! 8>$ 94!1 / 4!

" -'' :- ' ' 2

Page 193: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

,, -%5 ! % !

# + =% % D % # %& + & !9( / % %& , )/

N % :% :% .B & % 1

=> 1 -) '4 -' '-'/

,3 #

# =% % 1 & > %& >% D ! K + C - < & + % & & & %& %& D % 1 + > 1 , % + & & C% < 1 % % + % % & = 31 K + K & % % % /9 !% /

,3 -$ 5. ! $ $

" %%= & & 2 7 8 & > , %% & % # % /9!% /# % & # &

% = & C< + , )978 & & & N %% # &

-'/ #;- # 3

Page 194: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

+ 6 % % , )97&8 & % + & ( & %% % & %& % &1 % L 2 7 % 8

1 , )) , )) % 1

-% % # & C& < 1 , )) + & 1 % & =% %

K %& % % + % +

N + % %&)B + %& & + % + & &% E # + % %% & %%

K + & % & %% )'

(a) Triangle subdivision

(b) Restoration of connectivity

# =< 1 #$ 0" #$ B *

1 -) '4 -' ' -'/

Page 195: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

,3 5. $ %5 !

N & & & $ & &- %% + &- /9 !% / # %& 2 & & %% & ''') N > %& 7 & % 8 %&

=% = % % , )4 % =%'' 1 D

% C>< %%%

20°CL

Initial configuration Density after 100 steps

20°CL

After 101 steps Density after 200 steps

20°CL

After 201 steps Density after 250 steps

Exactsolution

Q

# == - 1 / 4! !" + * - *

-'/ #;- # 3

Page 196: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(a)

(d)

(b)

(e)

(c)

(f)

Anal

ysis

dom

ain

Wal

l

#=>

B4

!

!+

(

(

#$

'

E>

'=

E<#$

'?

8

'=

E>#$

'<

8

'8

<

"

#$

#$

1 -) '4 -' ' -'/

Page 197: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% # # , )* %= =% )* &

> & A

(c) The corresponding pressure contours

(b) The corresponding density

(a) Sequence of meshes employed

Analysisdomain

22° Flowvelocity

# =5 A* 4! * 1 8 " 9 ' 8=E ' >E<) ' /</ ' ?>?) ' < ' 8E=

-'/ #;- # 3

Page 198: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(c) (d)

(a) (b)

10

5

1

M = 3r = 1

u1 = 1u2 = 0

# =? - 4! *8? / #$ "* * #$ ' ?8 ' = >E> #$ 1 " #$1 "

1 -) '4 -' ' -'/

Page 199: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1.80

1.60

1.40

1.20

1.00

0.80

0.60

0.40

0.20

0

–0.20–3.00 –2.00 –1.00 0 1.00 2.00 3.00

X

Gp

(a)

4.00

3.00

2.00

1.00

0–3.00 –2.00 –1.00 0 1.00 2.00 3.00

X

Mac

h nu

mbe

r

(b)

MUSCLCBS: Anisotropic Shock CaptureCBS: Second Derivative Shock Capture

# =.@ - 4! *8? / #$ #$ 1 " " *

-'/ #;- # 3

Page 200: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

' 6 1 &. 6 N 1 % D C+ < & = 2 %%

; , 2 & + %

, % %& % & 5 ).3)/ % K % >% D , )( )'B % ; D %

9) # 7, )(7&88 % 1 1 # & + % , )(78 )(78 & !$ & 1 %

Analysis domain

# =.. 9 "" ! !E

1 -) '4 -' ' -'/

Page 201: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& 1 % % , )'B N % & & > % & !:). % 1 % 6 % = % % 7>&8 , )'' % =% % 1

& 1 6 = + & % =% '4 % %

=5 '; ) :-

#> %& D > %& & % %%=> %& > !% ; = > %& %% + , & % > %& =% & > & & % 6 % & & 1 % %& & 1 % L % % %

% = %% %

& & & % % & .) & % 2 6%% = !

% & % & % K + 6 & + % + + &K + %%= + % +

-'/ #;- # 3

Page 202: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% % &K # % & % % 6%% = K )9)( % & & & C <

+ # & %% % L

$ # % %2 % % % % %& &-;);*

> %% =% %& )'B > 31K

,: $ % ! !

%% % D + L % & # & % : % %& + % >'(*B + 7 + + & @ 4B8 # + % & # %& & = 14' F % % & ') '(*4, )'. ') % +

% . # % % 7 8 + 2 1 '.9 BBB %%= 4B BBB

;9B BBB & # % & & % D % &6 % % &1

& D

'; ) :-

Page 203: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% %% L + & .) =% & 1 K ' )') BBB + & %

# =.0 4! " #1 $? : ' E ' 8

-'/ #;- # 3

Page 204: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

,: -496- $ ! 3:3

6 %& % & & & # % % & &

# =. - 0AB;-0 --E #$ #$ #9" #$ * -- " 6 " F* B 3*$

'; ) :-

Page 205: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% # % '9 "& '((4 1 %& & % & % 7 & 8 %& >= # % D % & % 6 K & % = 49B , %&# % &

% % & >% % &

(a)

(b)

# =.8 - 0AB;-0 --E #$ " #$

-'/ #;- # 3

Page 206: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1 % %& 1 K + % & & # &- % & & % > % & & & # % %

% =% % + & 1 # & 1 %- 'A.9 1 '; % 1 , )';78 %%.4

% , )';7&8 % > % 7 A ;( 9.* A 4( B)BP A ';/ .4. A **4 );/8 % > > %& % , )'/ % .4 &

&1 , )'9 % !, .4 =%

# 1& =% # % %% % % & & 1 K D 7 8 %% % % % %%

6

4

2

–2

–4

–6

–6 –4 –2 2 4 6 8P.S.L

Pendine tests

CFDresults

KeyM = 0.71M = 1.08M = 0.96M = 1.05

Computerresults

Pendinetest results

# =.< - 0AB;-0 --E

'; ) :-

Page 207: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# % % % %+% & B4' B() 'B9 'B*

,: <$ (!

# > =% & K& > 1') .# , )')

(a) Mesh on analysis surface

(b) Mesh on analysis surface (c) Pressure contours

# =.= 0 * " ? 1 #= $

-'/ #;- # 3

Page 208: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

=? ' '; -'/

% %& %% % > & & L %& &

# =.> ! "E/ - " * ! 9 8<

' '; -'/

Page 209: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% =% #+ =% % 4; > , )'4 % & > % % 1 6 % , )'*

> %&4; " > % &

NE = 7870NP = 4130

NE = 7377NP = 3867

NE = 6847NP = 3580

NE = 8459NP = 4379

# =.5 ! "E/ 1 1 " = =/

-'/ #;- # 3

Page 210: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

+ , )'( > %%=> .( # % + %> 1

=.@ -'/

! % % & 31 K & L 6 %& % % & 7 1 !% /8 % + & + =% & + & & + & % = # % + !% / # & & =% )'B. )'B; K + + & H + % & & 1

(a) (b)

# =.? - " > #$ 9 ) #$

-'/

Page 211: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# % % %& > )'' %% & + & # % + & , ).B

%& K & 7 > %&8 > K % & & 4/4)

,7 ' ! (!

# =% & 1 & % >% D D %44 # %& = & !4* + L % %>% & % + 6 += + & &

, ).' & !$ , ).. % !<4* %

l

d

d

Unstructured, adaptively refinedtriangles

10–15 ‘body’ layers of quadrilateralelements with length l, correspondingadaptive layer thickness d and number of layers decided by user

(a) A two-dimensional sublayer of structured quadrilaterals

‘Body’ layer subdivision in three dimensions joining a tetrahedral mesh

(b) A three-dimensional sublayer of prismatic elements

# =0@ B * *

-'/ #;- # 3

Page 212: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(a)

(b)

(c)

# =0. G 4! 4 # $EE 1 / #$ ' ?E8 ' / E #$ #$ 1

-'/

Page 213: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& !$ %% &

,7 ' ! . $ $

% % % !% / % % + 2 % 6 =% %% , ).; %&

5.00

4.50

4.00

3.50

3.00

2.50

2.00

1.50

1.00

0.50

00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80 0.90 1.00

X/L

P/P

inf

0.80

0.60

0.40

0.20

00 0.25 0.50 0.75 1.00 1.25 1.50

U/Uinf

Y/L

MUSCLCBSCarter

MUSCLCBSCarter

(a)

(b)

# =00 G 4! 4 # $EE 1 / #$ " #$ *

-'/ #;- # 3

Page 214: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Anal

ysis

dom

ain

Wal

l

(a) I

nitia

l and

fina

l (se

cond

) ada

pted

mes

h

(b) I

nitia

l and

fina

l (se

cond

) pre

ssur

e co

ntou

rs

(c) I

nitia

l and

fina

l (se

cond

) Mac

h nu

mbe

r con

tour

s

#=0

-

**

E>2

'=

><

-'/

Page 215: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& & D % = % 1 % 4( %& %% !% / # %+ # %& & %% !$ >% D # D 6!6BB'. # %& = & *B*' , )./ + # % & & & 1*.

%& & % + & 1 + =% =

++ ++

+

–0.50 –0.10 0.30 0.70 1.10 1.50

1.50

1.30

1.10

0.90

0.70

0.50

+ + + + ++

++

++ +

+

+ + +

++

First mesh

Third mesh

Experiment

Surface pressure

X/Xshk

+ + + + + + +

+ ++

++++

++

++

+++ ++

+ First mesh

Second mesh

Experiment

Skin friction

0.30

0.20

0.10

–0.00

–0.10

–0.20

–0.50 –0.10 0.30 0.70 1.10 1.50

×10–2

X/Xshk

CF

+ +

++

(d) Surface pressure and skin friction

# =0

-'/ #;- # 3

Page 216: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

(a)

Density contours(b)

Wake region, density contours(c)

# =08 0 4! : < 1 >8 #$ ' ? /<< ' / 8 #$ * #$ * !

-'/

Page 217: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Initial mesh, 1804 points, 3487 elements Mach number

(a)

Mach number

Mach number

adaptive mesh, 916 points, 1830 elements

(b)

1162 points, 2258 elements(c)

# =0< A* 4! : < 1 1 #$ #$ #$ #$ " # ! $

-'/ #;- # 3

Page 218: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Initi

al m

esh

adap

tive

mes

hSe

cond

refin

emen

t

(d)

#=0<

-'/

Page 219: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

,7 ! ! . $

6 %% N % - & & , & > & %& 1 + & & , ).B K" & 1 %& & K> # %& & )'' %% 6 % % & %+ % % & % += & & = %& & # + %& & =% + & 1 & #

# =0= - " * * ! / " *

-'/ #;- # 3

Page 220: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% & %& & 0 12 *B & & % K & 1 # & & = & & 1 % & % ;B;; % % 1 # & & %% % % + % % , ).9 % D 6!6BB'.

1 *B # , ).) >%

=.. '; ) -'/

# % & % & U 5 & &

(a)

# =0> A* 4! 1 <8 / #$ 9 '8 >> ' /><<

'; ) -'/

Page 221: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, ).4 D 5 & & & % ;' =% & > # =% % &

% = & D "56) & 7, ).*8;/

(b)

(c) (d)

# =0> #$ #$ ' E> / ' == E? #$ #$ 1

-'/ #;- # 3

Page 222: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

=% & 6 & !% 9 % K, ).*78 % N % =% *;

=.0 ' '9) ' -#

1 >% D = & D % % & L + #D & % %& & %%= & % %& & !% & %%=> 1 & % % # & % &

(a)

# =05 0 4! 5:+B 1? !"/= #$ - '=< 8?

' '9) ' -#

Page 223: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% & 1 % 1 % 1 ! & %& & L K & % & 31 K

K %2 & % & % 1 6 K &

%% & K & C % < D*/ C> < *9 & D & %%, = % & & *)(B

% % %> 3 % ('(; 6 3

(b)

# =05 #$ #$

-'/ #;- # 3

Page 224: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% %%& %& & % & % D(/() 3 % K 6%% =

1.5

1.0

0.5

0

–0.5

–1.0

–Cp

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0X/C

1.5

1.0

0.5

0

–0.5

–1.0

–Cp

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0X/C

1.5

1.0

0.5

0

–0.5

–1.0

–Cp

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0X/C

1.5

1.0

0.5

0

–0.5

–1.0

–Cp

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0X/C

1.5

1.0

0.5

0

–0.5

–1.0

–Cp

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0X/C

1.5

1.0

0.5

0

–0.5

–1.0

–Cp

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0X/C

(c)

# =05 #$ #$ H ==H ?8H <H >H >8H !" /= </

' '9) ' -#

Page 225: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

=. # ''

# % & % > %& + %% >% # K & =% % %& = %& K K & L # % 1 % N & % %& > & L N % >%D & & %%= & C < & %& # 1 K & =% & & % & %% , &- % & % # %& = & 31 K % & > = & % &% & % = %% & % 6 % % %& " % & 2 > & %> & L % % D % % & & % %& %

!'

' 5 :Q "! 0 12 # > %&

K & + 2 2 2 2 , 6 'B/;3);'(*/

. 5 :Q "! 0 12 % =% %&

"2 2 2 2 2 68 ;';3.( '(*/; "! 0 12 5 :Q @ % %& D %& D , , 7

5 H H, ! @# " "! 0 128 F ) % . %% /'3** ! '(*9

/ 5 :Q "! 0 12 6 % + % %& % D "2 2 2 2 2 82 //'3)9 '(*9

-'/ #;- # 3

Page 226: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

9 5 :Q @ "! 0 12 : , %& D ",- "2 , - 7

@ $ 8 F %% .439; ! "= '(*)) 5 :Q @ F , D= %7,3,!#8 31 K 2 2 2 2 2 7

'B(;3'B( '(*44 5 :Q "! 0 12 6% + %& 31 K 2 2 "2

+$ , " :& '(*/* 5 :Q @ "! 0 12 , % D >4!848!" '(*9

( "! 0 12 @ F 5 :Q ,

%& D B 2 "2 " # F & '(*9

'B 5 :Q "! 0 12 6% +

%& 31 K +$ , " 7 $&1 "! 0 12 @ H 5 6"8 % '9 %% .*'3(* ! '(*)

'' @ F "! 0 12 6% >%& D % 2 "2 2 73 //(3)) '(*4

'. @ @ "! 0 12 6 % +

% D 14 # 5 666%% *4>B99* '(*4

'; "! 0 12 @0 0 ?! : @ %A % %& D ,

7,0 >B8 7 @5 8 %% /*;39'. 6 : '(**

'/ : , @ % +

2 2 23 '493*' '(**'9 "! 0 12 @ @ : , ,

D !%& D K % #

"2 + - , - 6 (9 6 > & '(**

') @ @ : , "! 0 12 , % ;> 2 2 2 2 2 39 .';939( '(*( 7

A 1: # 5 666 %% *4>BB;.'(**8

'4 @5 55 #- 65 6%% +

K 1 5 666 %% **>B;)* '(**

'* 55 #- @5 " @ 6 % % >

31 K 2 2 2 2 , ;/B93.9 '(*(

'( 5 :Q 6% %& &

, - " " 666 %% **>;4;) '(**.B 5 :Q # N D & +

14 #2 5 666 %% *4>B999 '(*4.' 5 :Q 6% %& "2 2 2 2 2 78

'(93.'/ '(*(.. @ 6 + D >

'(*)

!'

Page 227: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

.; " @ 6 %3=% %& % D "2 2 2 2 2 79 ./939* '(*(

./ 6 # > @ @ " 6 >% % 2 "229 (';3;; '(((

.9 5 : 6 % % & %& D % A '> +> 2 "2 22 7 '(399 .BBB

.) @ + D +2 2 2 92 9)(3);* '((*

.4 5 6 " # % D # % - <2 2 2 2 F 2

2 4(3(( '(((.* " < % DE

58 ''B3'/ 6 '(((

.( " :$ $ 6 % D & ""<# C=> ?1

;B " @ & @ #

D !=3!13: @ .B3.;! % 6

;' " @ & @ %

%& % D 2 2 22 2 5: ''.;3/* '((9;. " @ & @ >

D 2 2 2 2 2 5; 9/(3)4 '(();; " @ & %

%& D & %> 2 2 2 2 , 37 /'399 '((*

;/ # 2 " #& D %

; , - 5, ;9;3); '((*;9 @ & " 6 % +

%& D & 2 2 2 2 2 53 49'3

)9 '((';) " @ $1 5 @ @ 6 %

1 % % 2 2 2 2 , 52 '9(34; '(((

;4 @ $1 " % %& "2 22 2 2 283 '9434/ '((*

;* 5 6 F & % "2 2 2 2 2 277 'B(3.9 '(((

;( ! " / ,* F !>

'(**/B : 12 @# " 52 6 +

%& 31 K & % % >%

% "2 2 2 2 2 :6 .493;.) '((B/' @ F1 @ L 65 $% , %

1 + $ 2: '/(939B. '(*B/. , 6 + 1 +

K 2 "2 2 :, ')*3.B; '(*(/; @ 5 5 6 >

1 2 2 2 32 .;.34 '(9B

-'/ #;- # 3

Page 228: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

// 6 :% 6 1 & + L 2 "22 3 '9/344 '()4

/9 @: % + L D & 2 29 )4(3*) '(4*

/) 5 !1 $ $ 6 31

K %% 1 & B4!8 '(49/4 6 @ %

D "2 2 2 2 2 82 /)43(; '(*9

/* @ @ "! 0 12 6% %% 1 %& 78" , - ! "= '((B%% ;.43//

/( 5 ! 6 % % + > L K "2 2 2 2 2 22, ;.93/.'((;

9B #@5 6 + D FA 6 % % 3L %&"2 2 2 2 2 8: ;.(3;) '(*)

9' ! @ 6 2% " + %& 2 "2 6; /.43// '(*4

9. 6! HJ H ! 6 %%= % 3

H1 %& "2 2 2 2 2 9:*;3(9 '(**

9; & ! @ 6% L %& D & "2 2 2 2 2 :7 .)43*B '(('

9/ , 1& #@5 0 @ 6 + %> D G # %& 31 K "22 2 2 2 :; '/'3.'( '(('

99 "! 0 12 $F 5 ! FR 2K21 % 8? 2 "2 , , 2 @! ;9B3) @ 93* '((* # 62

69) "! 0 12 $F 5 ! FR 2K2

1 % D 2 2 2 2, 3: ';.939; '((*

94 H 6 + L > %& 2 "2 2 37 '3;' '(4*

9* # #2 #@5 % + K

+ %& % % K %% '(*;

9( ! # D

1 2 "2 2 86 ''934; '(*/)B "! 0 12 @0 0 6 % % % %>

2 2 2 2 2 36 ;;4394 '(*4

)' @# " : 12 6 % % A % % D # # ", 7 6 @# " 8 6 > '(**

). # 2 5: @ 6 ,O!: %& K 2 2 "2 , ,A * '((; %% ;4(3**

!'

Page 229: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

); 5 : @ @ #F >%& K 2 2 22 , 2; *.43/4 '((/

)/ 5 : # 2 " @ % & %& D % 2 2 22 -2 3 '(43.'' '((9

)9 56 " + @5 78 , ,0 8=B> 6 : '(4( %% /9(3))

)) 1& # & 78 : > ()B % >F $ '(*.

)4 5 :Q 6 % %& 2 2 2 2 2 36 'B'3'9 '(*4

)* ! 5 : + % + 2 "2 2 2 59 4(3*( '(('

)( :%2 5 ! 6 % % + >

2 2 2 2 2 6, ('(3;) '((44B 6 @ #@ $1 ! D

% 13 #2 5 666 %% *)>

B'B; '(*)4' F $ @ = $ W . ; % +

0 2 237, )/3*' '(*4

4. 5 & 6 H # ! : .+D# # : '((*

4; @ & , D > '(*)

4/ ? ;> %= > 2 52 '*9B3) '((;

49 ? 6% & % 2 2 2 2 , 3,

'B.;3;4 '((94) 6@ ! ? 6% & 7%>8 %>

& D 2 2 2 2 , 39 'B*93'B9 '((*

44 "! 0 12 5 ! FR 2K2 "2 # !>$>% %A 6 N D %& 2 2 22 , 52 ;9(3(. '(((

4* @ ! 31 K % >

D > % # +!+!>4 '(4.4( " , % % %& D

'((B

*B "! 0 12 @ 6 + % >%& D 2 2 2 2 2 57 .'*(3.'B '((/

*' @ !>2 $1 : H , $ 6 >

% % A %% "A , -C=: & 2 ""<# "2 @>6 R R ! %% '*'3*)

*. "! 0 12 6% D %&>

2 2 2 2 2 67 7 %% .BBB8*; F , !% & "56 )

& 5+- + +!8> '(4(*/ @ : " % 1 2 , 2 6 ;*; '(9*

*9 @ H @ 1 @, $ & & 1 %& D & > + "+2 +2 2 B=8 '(4;

-'/ #;- # 3

Page 230: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

*) $ # & & & D 2 , 2 59 '443(' '()(

*4 @ H # % & & % %& D2 , 2 52 49;34* '()(

** $ K 6 ? # %+

+ " +2 8>> '(;4*( 5 1 55 ! 5 # D

5 & BB!:>? @ '(44

(B @! : $ ! % % R K= K R + < % 0 + 3@ '(*'

(' @ 2 6 F D > %% 0 34 % % >

F $ 7'((/8(. @ 2 F % K &1 "#

"#!=:!82B24 '(()

(; @ 2 6 % ==!?44? @ '((((/ @! : $ F3 % %& D

5+-;,- . 0 5+-!"484

$ L ! "& '((.(9 @! : $ ! > % D

3 4 2 #2

,* : $ !6 768 @ '((.() @! : $ H=>: ! & 3

%>& .# 48 , - , #G 6 '((9

!'

Page 231: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

";' -'/

>. ('

# D & % % # % > % % K % # % D + D 2 %

% %& & & %%= + K 2 & > K % %A

*

+ , ' . 4'

K & 1 %& D 3 % % %& D 78 A

' # % % % %%&. # % % 7 1 8 %>& D

& % L % #&- % & K %%= K & =%# %%= D > &

& D < &- % % # + &1 = &- ' .

Page 232: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 % 2 >K % % & % = % %% ;

>0 / ;' 2

% % 31 K % %& % & %& K A

B 4.

A

'

'

( B 4.&

& ' . ; D , 4'

; ; % > & # K &

H

A

A

h

U1

u1

us1

Average velocity

η

x3

x2

x1

τs13 , wind drag

Hh

A

A

τh13 , bed ‘friction’

Free surfacep = pa

(atmosphere)

Mean waterlevel

(datum)

(a) Coordinates

(b) Velocity distribution

η

# >. 0 !! :

/ ;' 2

Page 233: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

'

; ( B 4;

(; ( 6

( ; - 4/ ; % % 7 -8 7 & & D 8" ; &

7 9; !% 98

; &

'

' .

.49

&

&; &

&'

' &.

.49&

% , D %

&' &. B 4) &

&; B %%= & K &

% ; ! ( K 74.8 ;

;;

;

''

;

..

; B 44

6 ' . 1 , 4'7&8 +

; 4*

' . :& 2 ) #

-

#) # )

#

-

) # ) # #

- # -#

4(

& K 7448 K 74)8 &

;

4'B

";' -'/

Page 234: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

' . # + K 7448 & %

;;

; ; 4''

7498 &

;;

;

4'.

6 K 74'B8 74'.8 %> +

B 4';

% % K 2

'

'

(

; B 4'/

' . & + & % >

%> K &

'

.(. . '

;

' ; &; ( (

-

B 4'9

& & %& = # & K =% & & !R 2 =%

&; (-

.4')

-

' .

!R 2 N K 74'98 ( ! % >

%& +

(' (. (. (' 4'4 ( ! %# K + N

& 1

.;

4'*

/ ;' 2

Page 235: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6%%= K 74'98 &

'

; '

.;

4'(

K 74';8 74'98 > %& K 74'8 %%% + &# ' .

-

'

.

4.B

' ''. (. .

. .'. (. .

4.B&

* B

' .

4.B

74'(8

+

B

(. ( '

-'

' ;'

('-.

(' ( .

-.

' ;.

(.-.

4.B

# & > K + % / 9 %%& > K = %%= % >%%

& K % > %% > & & & % & %% % =% D % & # % > %% & & 2 K 74';8 74'98

> & %%= K

B 4.'

(

B 4.'&

";' -'/

Page 236: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& &

B 4..

(

B 4..&

.

.

(

B 4.;

2 K , % = %# > K %>

D % % % & %& & % %& > & & # = & & D

L # + 2K % > %%= 6 L & & L C < & & 0 12 ) 2 & % % =

> %' --':

$ + L + % & > K # %%= & %% 4 * %% % % % 2 & & >%% %(')

+ %% + &1 '(4. % '4 %% & /9'*/'

6 & =% %& D K & %> > K & & A

% % '

. (. .

%' --':

Page 237: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# >&>% % % % %& D & >K /./;

# = L + >% D > %& & #3H1 /9 >% !$ % % % D - 7 % 8A

- 4./

2 %

(

A

- 4.9

% =% #3H1 %%= /9;. % > %% , & %&% % & &

% % .B 7=%8 % L % D & =% & = /;//

=% %& & !$% #3H1

>8 :- --

3 - 5 ! !

% % =% % %%& # + , 4. % /9

& # K /)/4 %% & & %# =% , 4; > C &1< %&

% % # %& 1 & %& D & K + L# + =% , 4/ 2

C&< % % % & %

";' -'/

Page 238: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

D % C&< 7 (

8 % % >

1 %

3 -%5 !

# = % % % & %& 6

40 elements

80 elements

160 elements

(b) Solution for 40, 80 and 160 elements(b) at various times

(a) Problem statement

Wavepropagation

Hl

a = 0.1

10 1040

η = a sech2 1/2 (3a)1/2 (x–α–1)

u = –(l + 1/2a) η/(αx + η), a = 0.1, g = 1.0, α = 1/30

Initialconditions

# >0 -" !

:- --

Page 239: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% ' . # L > % > %& 1 % N % & = & + + % , % 3 + N + & % N # + =% , 49 % %&

2 = 1 %% /* % # % % & & % + % & 6 %& > & K 1& =% %% /9/.///(

C &< % & $ ! 1 , 4) %&# &- =

7 %& % &K D & & & 8 $

h = 2

H = 1

t = 0

t = 2.5t = 5.0t = 7.5

h = H = 1L

0

40 elements in L

η

t = 0

t = 2.5t = 5.0t = 7.5

0

u

# > " ! 6 = *

8

";' -'/

Page 240: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

= & & & & " & %# >%& & &

% D # L & % > % & 71 % % 8 , % & & %% =% & ;9 ;)# , 44

# % % = & L & & % + # 2 . 9 1 2 + &>

# % %%= 9B & &% % % # $ ! % & %

% & =% >=% /; # % & & " % 7"8 +.

/( % %

1.0

0.5

0

–0.5

u

2

0

40 elements

Hho uo = 1 A

Prescribedwater levelhistory

η

# >8 %& ! ! #$ 6 / / #/ $ 6 8 8

:- --

Page 241: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

10

5

0

Surfa

ce e

leva

tion

η (c

m)

x = L

Analyticaly = 0, ±2 ∆yy = 0, ± ∆y

Computed ∆t = T/40

10

5

0

–5

Velo

city

u (c

m/s

)

x = L

Analyticaly = 0, ±2 ∆yy = 0, ± ∆y

Computed ∆t = T/40

t = T/2

t = 3T/4

∆x

L = 22∆x

∆y

y x

Inlet

h (x)

# >< -* " " 6 /

";' -'/

Page 242: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

7=%8 % 79B 8 / 7.BB 8 * 7/BB 8 % 6 N 7 8 BB;* % ! # % !L % % #& 4' % %> & & % % % L % % % 7, 4)8 L % & & # = % & '/Z % /BB % % 9B & % 7';8 9B 7''8 # & 1& >=% , 4* & L 7=% 8 % 5 %

7 , 4) 4(788 C&< % && 6 %% % & %+ = % % %%= & % H 7H8 7449 1 6 8 && % L & % $ 7 8 % , 4(78 % 6 $ D 6 %% & & & % D

StockpoleQuay

Tenby Swansea

WormsHead

Port Talbot

Porthcawl

Barry

Cardiff

NewportBeachley

Avonmouth

East

ern

limit

Clevedon

Weston-Super-Mare

Hinkley PtWatchet

MineheadLynmouth

Ilfracombe

Port Isaac

Wes

tern

lim

it 1 W

este

rn li

mit

2

0 50 km

# >= 6 . - + *

:- --

Page 243: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

25

6

CL:

164

nod

es, 2

51 e

lem

ents

810

9

74

3

1

FL: 5

78 n

odes

, 100

4 el

emen

ts2

5

68

10

9

74

3

1

FR: 3

82 n

odes

, 664

ele

men

ts

5

68

10

9

74

3

CR

: 111

nod

es, 1

61 e

lem

ents

5

68

10

9

74

3

Stat

ion

Loca

tion

1 2 3 4 5 6 7 8 9 10

Har

tland

Poi

ntTe

nby

Ilfra

com

bePo

rtloc

kSw

anse

aPo

rthca

wl

Wat

chet

Barry

Wes

ton-

Supe

r-Mar

eAv

onm

outh

#>>

2

.

-

+ *

";' -'/

Page 244: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

&& 7# D = .9 8

3 - %

6 %& & K1 2 > # & <

Time = 0 Time = 3 hours

Time = 6 hours Time = 12 hours

1 m/s

# >5 G* #26 $

72 $ ! 3 & , % 7,: 8 >% 7 'B.8

: "& ,

# & .). .)B 7'Z8 ;'9 ;B9 7;Z8!L /B( /'' 7 BZ8 ;'4 ;.4 7;Z8$ ;*. ;(/ 7;Z8 #& ;') ;') 7'Z8% /'; /.B 7.Z8& ;B* .** 7)Z8 ;9* ;). 7'Z8

:- --

Page 245: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& = # % N % %> % % & # % %& - 7 %& 1 + 8

P1P2

P3

Finite element mesh including river

(a)A

BE

E

A

B

B

G

(b)

(c)

# >? -

";' -'/

Page 246: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& & ) % 7,:8 # % , 4'B # %>% 3 " % % & #

& & 5 >% % & & % 1 # & % %% & # , 4'B +

L %

15

10

5

0

–5

–100 5 10 15 20 25 30

t (h)

Elev

atio

n (m

)

MWL

8

6

4

2

0

–2

12 14 16 18 20 22 24 26t (h)

Elev

atio

n (m

)

MWL

ComputedMeasured

10

9

8

7

6

512 14 16 18 20 22 24 26

t (h)

Elev

atio

n (m

)

ComputedMeasured

Point B Point EComputed and measured elevations

ABE

Water elevations for points A, B, E

Severn Bore

(d)

# >?

:- --

Page 247: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Time = 0 Time = 5 min

Time = 10 min Time = 20 min

Time = 30 min Time = 40 min

# >.@ - " " 7 " # "$

";' -'/

Page 248: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

3 5

" > & & % D & =%% % L % %& D & % # + >

, 4'' % =% & &1 % > );B9B "& % % & % % & # C< &1 % # + L &

1 %& & & C%< + & 9B

6 % > 7 8 %& %> D 1 % >% %& D # D %& > & % D , %> D & & C%< -% C < %%% # %+ %%= & & & D % # '9 + )(4( # % D D, & .9 & A > %& D 7 & , 4'.8 % & 7%% & , 4'.8 & D & 7 , 4'.8 # =% % % , 4'.% C<> C < " & C< &

# >.. 7 * 4! /

:- --

Page 249: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

>< '# '

6 % %& % & > # & > % $ ! 3 & & =% & ' 1 , '. 1 ! & L % %& & , 4'; % L & + 2 & % K & > & &&

& % % %

# >.0 - 4! ! * ! 94! 2 8 ' 8

";' -'/

Page 250: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

>= ";' '-'

> K K % % #% % % % # > % K %=9' & % % K %& ! ( & % 6 % K & 3 %

% K 3

B ' . 4.)

% + % K %%% L N 6 K>% !$ & & L

% 2 7 L % K 8 % % # K>% %> K % % # %% !$ % K >

& & % # % # % % & % ; B ; '# %% 3H1 % +

= 7 8A

% ;! % .

./

! 4.4

P P' ∆η

n

A

A

P

P

Boundary at time tn

Boundary at time tn + ∆tn

# >. @ *

";' '-'

Page 251: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

A

% &#&

&#

&

/

&#

&

!

&#

&

&#&

&

6 % % % %%

Time = 9 hours Time = 18 hours

Time = 36 hours Time = 54 hours

# >.8 A 0 " 4

";' -'/

Page 252: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# %%= 99 1 L /B ' # % 7 > % 8 ;( # B' L =% # % ; B9 # % L & % B' ;( = L ;.Z ;( %% 1 %% /B % # % %%> & % K & % >% %& & )B % K +. L , 4'/ & =% %

& L %

!'

' $ 6&& " .A , # ,* : '(4(

. H@ 5# - ?1 '(*B

; "! 0 12 5 : H 78 <%

! '(4*/ @ 6 + D > '(*)

9 @ "! 0 12 %&A =%

2 2 2 2 2 33 9/434/ '(*)) "! 0 12 @! 6 + 31 K , % %%

"2 2 2 2 2 27?2: )4;3*( '(4(4 " + > > > D

" 7 @# " 8 %% .)'3*4 >

6 '(*B* 6 + K

" < .4;34* $1 5 '(**

( @@ ! !6 $&& ,! ( , ,* >$> : $ '(4)

'B @@ "<$ & 6 % 2 2<2 3 '/3.) '(4.

'' !% ! 52 ! L % 2 2 <2 26 ;)93*. '(*/

'. HH , 6 >% >

2 > K 2 "2 2 82 /9/3*; '(*;'; 5 H 5 : , > > K

& 2 1 "2 ,! 7 + 7 !6

$&& 8 %% ..;3./. '(4*

!'

Page 253: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

'/ # @# >% + > %% > K 2 52 +2 :9 /B.(3/B '(*'

'9 H@ ,= , > > %& # 2 2 2 3;;4'3*4 '(49

') ! # @ # > %% + > %%

" , 5 '.93/* '(49'4 @ ! 6 % + %& 2 2 2

2 22 '93;' '(4;

'* % @ @ % > % K H1 %%= & 2 7' +2 2,, 4;*3/) '(4.

'( , > > K

2 2 5 ;;43/* '(4(.B @ ! # + D

F . % 9 %% ;;B3* "OH65 & '4 >

" H 2 '(4(.' @ ! ! , + >

92 2 +2 2 #2 2,3 94'3(. '(4(

.. 5# 5 H1 + > %% K & ,! ,*! 7 # 8 #1 #1 '(*.

.; 6 3H1 K %% + > >K % 2 "2 2 83 ;';3;( '(*;

./ 5 F H#6, K> 6 ,"5#56 F

% > K : " 52 23 '9'34; '(*)

.9 6 6 %% + >

D ,! ,*! 7 # 8 %% *;93/. #1 #1 '(*.

.) 6 # %% + >

3 2 2 2 2 , 6 '>.. '(*/.4 5# "! 0 12 % + >

K 2 2 2 2 , 2 ('34 '(*'.* HH , 6 > %

> K 2 "2 2 89 .*43;.; '(*/.( ,GA > > + > ,"5#56 %

> K " 52 25 ..93*9 '(*4

;B $ !6 , @! "! 0 12 6 6 % 2 & 8: " "2 & H "& '(4*

;' #1 # ? # % =% + %% 2 2 2 2 2 23 ;;'39' '(4*

;. @ : @ "! 0 12 # H1

%& 3 "2 2 2 2 2 92;9(3)( '(*4

;; 5 : H 6 K + % " , 7 .B43.* '(4(

;/ " & @ 6 @ % %& & D 2 2 2 2 2 37 ;3.B'(*(

";' -'/

Page 254: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

;9 H :& $ := 5 R K >F % R <R R + G , 5% O/' '(*.

;) # # 1 , K % & 2 2 2 2 , 25 (;(39; '(('

;4 $ H ! 6 % & %%

K 2 2 2 2 , 35 .(3/) '(();* $ # #2 #>% =% + %>

D % % 2 2 2 2 ,

32 **93(BB '((9;( !%% ! 2 , , %%=

K ! " + D2 / '((9

/B !%% ! 2 , , %%= K " + D2 / '(()

/' "! 0 12 @ @ 6 >% =% K 2 2 #2 "2 2 ;'3/( '((;

/. "! 0 12 "2 6 %> & +

K 2 2 2 2 , 3, 'B)'3*B '((9/; "! 0 12 "2 # & %

> D 1 2 # .

'((*// "2 "! 0 12 # & %% & D

, ,2 = 2 " '((9/9 5 :Q "! 0 12 # > %& K>

& + 2 2 2 2 , 6 'B/;3); '(*//) 12 "! 0 12 ! 6

=% + %%= K 2

2 "2 , ,* $ L F . %% '34 '(*B/4 #& 1 % +

D 2 2 2 2 , 3 *(3''. '(*.

/* 5 : H H 6 % D 2#" 2 .2 -2 2,67'B8 '/B(3.* '(4*

/( 5 % + H=>4 '(*'9B 6 $ : & 2

2 2 2 , 3 .);34) '(*.9' ! 0 :1 # % +

2 52 7 #2 22 '.;3;. '(**

!'

Page 255: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

*)&'

5. (' 2

# % % 2 & & K K 74.;8 % K & # % % %& % K

=% *' K & %= K 74.;8 &

# .

( B

.

( B *.

%

. . B .

. B *;

& (

# % K 7*;8

2 K 7 !% 4 L K 74.;88 %& # K = '/

, %& & 1 & % & & %% # 2 K 7*;8 & % # & & K % # &

D &1 $ & %% &% # + %% + & H9 # '()( &

% !

Page 256: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K & 0 12 ) + & !4 6 % % & 6* %& =< K &

.

..

. /

.1

..1

. /@

*/

@ 1 % % @ 2 K % K 7*/8 2 K & ,&(

, . % % '.'B'' # K &

#( .

( B

(

.

( B *9

% ( ' . ..

. ( *) 1 K % &

50 *) 9 4

% , & & & > & % % & > % F ' # % & =% % &

& *4= K 7*.8 % & %

&

&

&#

.

(&

B **

# 1 % # & B

& % 2 D & % % D K 7**8 &

*) 9 4

Page 257: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/ .%

, *(

% &#'

(& /

#! *'B

! B

B

%& !% '4 F ' # / % L # K & ! % + + & # 2'. , '49 F ' # & % %'; # + F ' !% .B K CL < C< % %& K & # & & & & %& %& & 2 K 2K N + 6 C &< & &'B % # & % %& > %& 2 K & ';'/ %& N + 2 # & 2 & # % A

# % & % % &

# &

# % % % %& % %& # L & % & % 2 K & 2 + $&V 1 2';'/ + L>

% 2 & # % % & & K & & . 'B % & B) $ 1% N # % ;. $&V 1 2 %% % !% '/ F '

*)

Page 258: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

5 4 # ' )

# % > & & A

' & # K & &1

. 1 & # & &; 1 % > 6 > '

)

# &

% L & & % # D % # L & %%=

% & = K !% '4 F '

58 ' '

# !R 2 & > 1 K N # % L % & && % && !R 2 # 2 & K 7*.8

# .

( + B

.

( + B *''

+ 2 & N & + *=;. !R 2 = = & % & %= & + % % 1 = , + % % CL < C< K 7*''8 % %= = # = > = % # > L >&& %& &1 & & % L % # =% '9 =% D % L

5< ';) -'/

> L %& %& %& % # & % %& & K

';) -'/

Page 259: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

'B & % 1 + %& + # 1 =% ' % 'B % % K>

: - !

# % + + %& & = #%% 2')'4 %& & = # = K

B

. B

.

*'.

. + % #K & =%

-

;'

, -

.

*';

D= % #

' B ; . B ; . #

. ; B ' ; B ' #

; . ' B . ' B #*'/

# 3H1 7 :=3 L8 & !% . %% %&> & 2 % ! N K> & & % & % % & $ % %& & % % & # %& & , *'78 ,*'7&8 7 % F '8 > 75!8 & & .B & &

& & %

: / ! % $!

6 %% % 1 # + % + $ 0 12'''* # + % $ 6'(.B

% %= - *';

*)

Page 260: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, 6< % K !1 $ :.'

% % % + 1 % 6 %% & 1 $&V 1...; %% & % % % % - $ 0 12 +

0 45 90 135 180 225 270 315 360Degrees

RC

S

(b)

# 5. -" !" * * " " < #$ ! " #$ B- 1"E

';) -'/

Page 261: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 % 1 $&V 1 # 2 % + 7 !% ') F '8 1 $&V 1 % 1 % %% K K + &K $ : %% %& - ./.9

# % H1 2 K

# .

# B *'9

# %%= 1

'

!$'

$'$ *')

% %

$ $ $ *'4 & ! & > # % % L % % L % % % % + # > % & & & % # %

'! $

'! $

$

$

! "

$ *'*

# & & -& = # L

)# )## +)#

)# *'(

) # ' . ! >

/$ ''

''

$ $ *.B

# & % $ H3: % #% & 'B % % : $ L %& % L & # , *. 6 &

*)

Page 262: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Cylinder radius: a = 1 m, radius of the meshed region R/a = 7

# 50 - ! * * " 6" . =

';) -'/

Page 263: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%& - * B.9- - ' = ) 4- , + K 'B % /./ ')B $ ;) % .9. (B4. # & & % # &

= & K + %& =

5= *) / 6:'' ' )-'/7

& L += D % L % - % & &1 %& % & %& + % + = & *. & & % % & % % = + # N %& & # !% '( F ' K 7'('*8 > % 1 & $ 2.).4 % & + % # % % + & & % # K & % & % %& & 6 & #& *'

:, & % !

# % % = & %& = # %& # = % = %& 1 &- + + # 1 %& % & & % $ & & % & > % & =% % % > D & & % %

*)

Page 264: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

:, =

%& L & &- #%& &- L , *; & '0 &# & ' & &

L 0 & & % 7 + &8 & % & & + & & 6 & & F ' !% ; 6

%& # % / / # / & 1 , %& = &

0

'

.(# .(

.

*.'

:2 5 = %&

' . ;

H &

#

'

B 0! B! 0! B!

0! )! '

)

. ;.

)

0!

)! '

)

. '

)

'

B

) )

)

B

) )

)

B

0! B! 0! B!

0! )! '

) . ;.

)

0!

)! '

) . '

)

&

#

) '

B

)

.) '

B

)

) '

B

6= %

) B

)'

.)

B

)'

)

B

6= %

*) / 6:'' ' ) -'/7

Page 265: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1 % % > K 7*.8 & B 2 & # H < % 7F '6%% = H8 %% = 0 $ & & & & & =% $.* 6 % + =

'

.(# .(

.

(

'.

*

(. *..

# D C < & 0 , %% = %& 1 & + C% < K 7*..8% & & +

:, 0 %>

%& 1 K % &/ -B =%) 1 % >= ) % -B % " & 0 % & = ! + & K &

ΩA

ΩB

ΩC

ΓDΓCΓB

ΓA

ΓA

ΓA

Objects in water

Boundary of objects

# 5 !

*)

Page 266: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K 7*..8 # & % & & & C> < C < .*

5> $/ -'/

# = %& + & %%& + L # + % 'B & # % & H.( = + % & # &1 & H;B #6 % %>> +# A

& % & % 7 >D & > 8P

1 = & & 7 > %% 8P

+

55 ' -'

# & % %% & !) & 6 !% '( F ' % %% % % & # + D %&& 0 12 ) % % %%& $ 2.).4 & = % & # % % #& *' , ;' , > & %% & )

'

..

.

#

. # *.;

# &

;/). .. ;).) . '

.) . *./

, % % B , % B '.) # % =% > L > & & & =% & % & $ 2;' , */ L & %&

' -'

Page 267: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1 # > % & % % % = % K - %% % %&;. & % 1 $ 2 L #L & % + & L $ 2

:: <$ !5 !!$

6 %% & % % # % &1 & H.( & H;B % # %% H & $1 H 1 1 & 6 % % 7:8 C% < & && & & = & &

1

CylinderIncidentwaves

10

8

6

4

2

0

–2

–4

–6

–8

–10–16

–34–35

Rel

ativ

e er

rors

(%)

2 3 4 5 6 7Outer radiusof finite elementdomain

Plane damperCylindrical damperSecond-order damper

# 58 3 ! * * B

*)

Page 268: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

&& % % %% & 1 ! ;B

5? +# :''

6 1 + = %%& 0 12 2;;;/ % F ' % !% '; # = 1 D 78 = 7&8 =& %& # $1L'B;9 % & ! ;);4

% = 6 %% KL % ;; $ K 7*.;8 = K & &

'.

*.9

& '9;;;/ % = % % K &

/ /#

/ /

,

,

,

*.)

'.

*.4

& % & + % & = % / % + = # %% & & & & = 6 & & %

:; *

$1L'B;9 % % =% % & & + # K % & % %= # & 2 K = = K

1

*.*

+# :''

Page 269: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

7# & & 8 # & = =% %

&

%

*.(

& % K & % &

'.

%#& *;B

& & + & # & 7*.*8 & + +

'.#'1#

%#& *;'

F % & 2

'.

'1%#& '1

%#&

# / *;.

/ CL < = = & & 1 = # & 5 & %& & %& , *9

:; *

! ;);4 1 = 1 =% =% = % / / % % & + # = 1 2K A

!B

) *;;

# & &

/#

.

. B

' '

. B

' . ' .

. B

. ; . ;

. B

' '

*;// ) .B

B ''

'' ##

## * + *;9

*)

Page 270: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

#5<

B

'

(

!

"

*8

Page 271: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

! & 1 ) & & K &

1 " 1 =% &

% %& 1 % % > & = / # & & 0 1 > / & ! ;)

%% %& & L + L & F ' !% '4 , '4)# 2 & ;* %% &

%& : $ & , *)

3000 3000 60000Scale

feetNote: Number of node points = 1701

Number of elements = 2853

(a) Finite element grid, grid 3

# 5= 2 ! " " 6" . A A /<

*)

Page 272: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

:; ? !!

# %% & & & > & 78 %% % & 6;( 6 %% & K & H.(

5.@ (4

+ & &1 & $/B >> % & 6/' H/. # & F ' !% ( &% % L # + & $ 0 12 > C < % L'''* !%> ! ;);4 + %&

6 224

10 26 2 2

2 225

4

2226

266 2

22

218

9

6 6

22

42

662 2

104

22

22 2

25

2

6 12

2

2

(b) Contours of wave height amplification, grid 3. 232-s wave period

# 5=

(4

Page 273: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, '4) F ' : C%%< + % %& =% & &

5.. -- -' 4

# % F ' !% ( + &% .* ;( /;3/4 , % >

B ' .. & B

') .

). *;)

& < - % 2 + B B = %& %

1 ') 7 > 8 %% & % = % %%= '

)

L

6 & & = 7*;)8

: 0 $ % !

> = 2 K && & & 1 % 2 K & B) , ) 2> 1 1 ) ) > )'. 6 ') '). & %% %& )'. % % =%) & )'. # %

+ )'. =%) *;4 ) '' # % K 7*;48 & %& +

+ .

'

'. '

'

'.=%

'

.

=%

'

'

*;*

% .* ' ' % >% & # %% + %& %% + &% = % # & + & 6 2/4 # & & + % % /) %% % + % & %= - : 6 /* ! , !/(9B 2

*)

Page 274: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%% % + > % = % 6 1 $ $.* 2 %% + , *4 L & % >

5.0 - - 4 ' D'

$ 9'9; %% % + = %& # % & % % $ + > %& =% + & 1 = % & % %

)

)

B

)

*;(

# % 2 ) %% & % & % % # & +

# 5> B ! * . <

- - 4 ' D'

Page 275: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

A

# % % & % # %

# + & + +

# % & # % & L + ;

# % % # % 1

)!'

) */B

# N %&& - + # L L & & %% %% + & $ 2/9/) # L + & ) % $ 9'9; % + # =% # & & D3 %& & N & & $ + + 4 1 %- % & & ;BBB + % Y# $ & % > % - 'BB

% L %& , **

5. *) )- 4

6 % + %= - % '(.B # %+ =%) & % &=%) % & K 1 H3: 7 F ' !%(8 # % 7 = 8 & + , *( =% % %& H & % 6< %

) ))) ) */'

*)

Page 276: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% #

) ))) ) */.

$9/ > >% K + % = # = 7 %=8 K 7# %& %+ %= K 8 %& 1 & $ % : 1 %% % % %& & % %= - %

2

1

0

–1

–2

Rea

l pre

ssur

e

0 30 60 90 120 150 180Polar angle, θ

ka = 100

Shell quadraticthrough thickness

2

1

0

–1

–2

Imag

inar

y pr

essu

re

0 30 60 90 120 150 180Polar angle, θ

ka = 100

Shell quadraticthrough thickness

# 55 7 * .8

*) )- 4

Page 277: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& + # & $/B # & & 7 8 % K 6 + %% & 6 2/* C < 1

) ))

& ';) ) */;

& % + & % & ! ! ,/(9B # % %% 0 12 2%% + ! , %%

5.8 1' 4

# %= - % + K 7*..8 & L # & = # & $/B & & &K &- H 12999) % &K + 94 1

5

4

3

2

1

00 2 4 6 8

z/a

r/a

Incident mode number = 1Reduced frequency ka == 11Spiral mode number mφ = 8

Conventional FEMWave envelope FEM

Plane wavelength

# 5? * E < ! *

% % + - + 6 % % + - +

*)

Page 278: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% " & $&V 19*9( %= # + & + & + $ % + & + # & > & 6/' H/.

5.< ' -'/

5 6)B); = % + %> & % % & $ 9'9; % %& 6 + L / % % % + & + ( # 1 %& %% & %& , *'B % % %% + %&

& !% $)/ $ + # %% & N % & %& & % & & %& % & + & H.( H;B " & % & #% 1)9

1.5

1.0

0.5

0

–0.5

–1.0

–1.50 0.5 1.0 1.5 2.0 2.5 3.0

Dimensionless time T (= tD/c)

Dim

ensi

onle

ss a

cous

tic p

ress

ure

P(A)

P(C)P(B)

# 5.@ 0 *?/

' -'/

Page 279: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

5.= '; ' )

6 & & % % > K , % $1L< %%& 6 %& %% # D & % & %& D :%< K # 2 % " $ < K 1 &=% %

.

. (

.#

'. ## B *//

# %% % 1 K 7*//8& % %&

.

. (

B

.

( */9

1 "& % F ' !% '( K 7'(';8 #> + & %& # > % & % % & F' !% 4 # & B %% .( !3 7 K7'(';8 F '8 #> + & 1 > + &- % % % D # & % D3 6 K F ' !% '( D3> % & 0 12 $)) D K & D & 7 =8 # D L % K % , *'' & & 2)4

6F % D &1 # & > & + *(

:, *5! % %

# % % %& F % 1 L

*)

Page 280: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1.0

0.5

00 1 2 3 4 5 6 7 8 9 10

Wave period T (s)

Wav

e tra

nsm

issi

on c

oeffi

cien

t CT

Eigenfunction method

Present method (two-dimensional model)

0.1 0.5 1.0 2.0 3.0 4.0 5.0 6.0 6.0 7.0 8.0Wavelength λ/B

Incidentwave

Infiniteelements Special three-

dimensionalfinite elements Three-dimensional

finite elementsBed

8 m

Freesurface

20m

3m

10 mFloatingbreakwater

Unit: m

Floatingbreakwater

Incidentwave

1.41.2

1.0

0.80.6

0.40.6 0.8

1.0

1.0

0.8

0.6

0.4

0.2

1.2

1.41.6

1.8

2.0

2.2λ = 34.9 m

η1 = 1 m

# 5.. + ! ! 4" ! A?E

'; ' )

Page 281: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% %& !% 9

:, 1 %

# K !% 4 >% # % % + , '3/ # + !% 4 & %% %& K & > % K & L " K 3 F K % &

(

' ;

.

.

)

(

;

; B */)

# K & & & + + & &)*

:, %

% L % =% & % =% % & + % =% & & #K & 1 & 1 >% % % # = L L % & > L %& + K # +> L %& & *( > %& +>%

"A

'

.

(' B */4

" "A

.

.

(.

.& */*

*)

Page 282: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

.&

.&/

.&& .

(*/(

.&/

.('&

.'/

.

'/

.(

'/

.'&

.

'&

.(

'/

'& *9B

.&&

.('&

.'&

.

'&

.

(

'& . *9'

# > & & +>%& & %+ % %% % & +> %& %%& # % % > % C1< % +> C< 1 +> & K %%% & & % , !1 2)( , *'. > & & !1 2 6 & & % & &

Incidentwave

–1.5

–1.00.0

1.00.5 0 0.5 0.0 0.5

0.0–0.5

–0.50.0

–0.51.0

0.0

–1.0

0.0

0.5

0.0

0.00.5

0.00.5

0.5

–1.0

–1.0

–1.0 –0.5–0.5

0.0

0.01.5

1.0

1.52.0 2.0

2.0

1.0

1.0

1.01.0

–1.5

–1.5

–0.5

–0.5

–1.0

0.5

2.5

Real ηD/(H2/4a)(2)

Imaginary ηD/(H2/4a)(2)

# 5.0 - ! * "* 2?>

'; ' )

Page 283: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& % & : 24B 6 + + # > & + % 7 =%8 # +> %& + +> % > K 7*9B8 7*9'8 # & % % & = & % N> % % % & &/

!'

' :& . !& = '(;.. H$ 0 7 @ ?1 '(4/; !! - < # 7 ?1 '(*;

/ @ : 7 , !& '(4*9 H: H 6 % > &

# 6 '4.3*) '()9) "! 0 12 5 !% & &

%& D 2 # , ( %% ;)B34* '3'9 '()(

4 6 ! # % % % %

+ # 28 9B(3.* '(4'* 5@ 6 , # #A # 2 !

=> ! 0 F ' %% ;3'4 ')3'* & '((*

( ,& F ' . H> ?1 '(9;

'B @! $1L : %% %& + , , ' 5 H 2 ! %% .9'3*B

'(49'' "! 0 12 $ + D

%& 2 1 2 #2 "2 2 #2 '(49

%& 0 F 9* @ 2 % >F$ '(4)

'. ! # $ "! 0 12 & A

% 2 2 "2 2 65 '/'39) '()('; $&V 1 , & # & H -

+ 2< K A K

2 2 2 2 2 6,7'*8 ;//;3). '((4'/ $&V 1 , & # & H -

+ 2< K A % 2 2 2 2 2 6,7.'8 ;**;3(BB '((4

'9 "! 0 12 $ # + D A > > !% / <% "! 0 12 5 :

H @ '(4*') " @ 6 %%

% "2

2 2 2 283 '9434/ '(()

*)

Page 284: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

'4 @ $1 " % %& "2

2 2 2 283 '9434/ '((*'* $ "! 0 12 L +

+ 2 2 2 2 2 22 '.4'3(B '(44

'( 5@ 6 6 % %% + # 79 9(93)B' '(*'

.B 5@ 6 % + 2 2 2

2 , 5 9B43.) '(*;.' !1 $ " : L

%% % + + 2 2 2 2 2 68;;939/ '(((

.. @ 1 $&V 1 # % + $ %% "2 2 2 2 2 25; .*(3;'/ '(()

.; @ 1 $&V 1 # % + 2 2 2

2 2 6, 4.439* '((4./ " : $ % + 3

% %% % 8? "

, C== %% .BBB.9 " : $ % + 3

" " %

" %% .BBB.) 6 $ #1 5 & >1 K "#

+ 2 B=!1: '(4(.4 6 $ H 2& #1 $

% K = "# + 2 >?&8 '(*B.* @6 $ $ 6 %% + L>

%& % L %& "2 2 2

2 2 296 '43/* '((*.( H $ - 6 '((.;B #: H " D - 6 &>

'((*;' $ $ ! # L %

= L & % 2 2 2 2 , 6 9((3)'4 '(*/

;. $ K 6 - 5 & 2 "2 52 ).(39. '(44

;; "! 0 12 $ # % +

& % 2 2 2 2 2 227'8 ;99349 '(44;/ "! 0 12 $ \ 3 & &

7+ & 8 !% 9 ,

'(4*;9 @! $1L !% & 3L 2 8 2 "2

" F @ 'B3'/ '(4.

;) ! !! " L & 0 + 8=? '(4/

;4 ! !! " > & % 2 8?2 #2 . <@ + %% 94;3(/ '(4/

;* @5 : $ &A & D# 7* / # ' #2 + 8 2 .!B:!1? '(4)

!'

Page 285: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

;( 5@ 6 , = 2 %& % ,> %% "2 2 2 2 23 .943)4 '(()

/B $ $ '((./' 5@ 6 + %&A

2 2 2 2 2 %% '(((

/. H + %& 2 "2 : /;3)..BBB

/; "! 0 12 ! $ 6 & + 2 2 2

2 2 2; ;(;3/B/ '(*;// "! 0 12 $ #! ! !

& + %& + # - 69''93/* ?1 '(*'

/9 $ ! #! ! 6 %% + = %& !% '4 " # 5 : $ @ ! '(*/

/) "! 0 12 $ $ ! #! ! %% + = %& 2 2 2 2 2 32 '..(39' '(*9

/4 5@ 6 $ @ !1 : 5 '.* 2 2 2

2 2 537'8 .B43( '(('/* 5@ 6 H@ @ ! %% %

2 # 27,7'8 (43''* '((/

/( : ! 5 , @ ! 6 & + % 2 # 2727/8 /*;39B* '((/

9B : ! 5 , " & + % 2 2 #2 2 ;77/8 .B.*3/B '((9

9' $ 6 > + & % %% =% 2 2 #2 2 ;8798 .4(*3*') '((/

9. $ 5: & % +

"2 2 2 2 2 28: ''43/' '((*9; $ 5: 6 % + "2 2 2

2 2 296 /(34) '((*

9/ $ 6 % % =% "2 2 2 5 443*B '(*4

99 H : 12 ; :% 2 K = & % >+ > + "2 2 2 2

2 257 .;(34; '(()9) : 12 H ! + >

2 K %& ' 7; ''3/. '((*

94 : 12 H # - - + 2 K = "2 2 2 2 2283 '.93/9 '((*

9* @@ = 2 %& + + # '((9

9( @@ $&V 1 6 % %%= &

+ = 2 %& "2 2 2 22 296 '.'3;( '((*

)B 5@ 6 # % %& 2 # 2;37'8 ./93)' '(()

)' 5@ 6 H@ @ ! : ! # > >% & ' , K 2 2 #2 2 2,57'8 /(3); '((*

*)

Page 286: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

). 5@ 6 H@ @ ! : ! # > >% & . ,

2 2 #2 2 2,57'8 )/34. '((*); 5@ 6 %% % > % & %&

2 2 2 2 2 62 '.;939/ '((*

)/ @: !% @ $ + %% % =% 2 2 2 2 2 65798 **(3(B* '((*

)9 :: #% 1 6 %> + =

%&A # % & % 2 2 2 2 2 5; ');9394 '(()

)) "! 0 12 $ ,3 6 > 2 2 2 2 2 25 '3') '(4*

)4 6 # # ? L % L # "2 >&?B "& '(*;

)* 65 & , !% ') " # 5 : $ @ ! %% /)93** '(*/

)( @ !1 $ @ H L L + 2 2 2 2 , 23;/;3)4 '(('

4B : : 0 # & & >% + " 2 2 "2 " 5 & & 6 ?1 %% ;;'3;4 '(*4

!'

Page 287: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

-' - " #'

& %'

?. ('

% % % % !$ + " & > % # % % %& & %&<& %AOO&O% O # % & L

D %&A

' !%& D %&. %& D; %& D / D9 > %&

% + %& & D+ & # %% & % % !% .B F ' &1 % % & &1 !% .B F ' ,"5#56'. + % F ';

% %!$D & !$ !% ; % 1% %& %& D % =% % % & % % > % & %& % % % % & =% % % 6 % & & % & % &

5 , % !

Page 288: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# !% .B F ' 7'8 % %% 7.8 7;8 % 1 2 % !% .B F ' % !$D 31 7 318 K %& =% >% K>% % !% ; > + K % % % & %& %& D >

K # %%% % 7!% ; / 98 L > % (. & % %

& %& + (; =% % !$ % &D 1 % & 1% %% L % K (/ % & % %% % 7 (98 %& = !$D %& & D

?0 -

# % % % % %% %%% % + % 1 !% .B F ' % !$D % % $ & % % % % !% / 9 & % %# % & !% .BF '

; $

" + & %%% 7 %> & !% .B F '8 & !% .B F ' # , + %%% ' ' . . + & & /, $ & $ & & &

-

Page 289: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& % & D & >& %% 6 % - & %%% D # >%

; &

% !% .B F ' & %& & !$D & K & 7 % %+ 8 % & %%

; <$

& % % D , =% %& D% > % & 5 & & > K % ;' !% ; !% 9 # % L %& #& (' % D & 1 % &

% , % D % %&< & %

; " $

6 % & & %& 7 8

;2 > %

> & & , %

! D & &- D & + !%& D & ) !%& %&

% D D5 & - D5 & !%& %&

% DF D

-' - " #'

Page 290: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

!

" !

" #

$

" !

" !

" #

$

$

" #

" !

" ! $ %&'()*+, -.)/-0

1

1 2 *3- &( 45/ 6* 7&.(4-

1

080 $ 2 *3 2&+ -& .) 6* -0

"

"

080#

" 9 !

"

"

"

"

$

$

1

" !

"

"

! "

-

Page 291: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

= % & & % # & , (' " % & & 2 & 2

? "

, (. D !$D 6 % % % &% % !$ & >% %& D % % &

; - !

# % !$ & % 1 % 6 > D & =% K & % ' & , L % (;/ !%; % !$

! "

" #0###

00#

! " ! 9

! " ! 9

" 9

" 8!! 9 !!

! " !:

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00;#0

! " #0###

" #0###

!< .- 4+*. .(3 /)3/< $ /030 */+&2&. 0

$

# ?. - " !

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Page 292: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

Inputs

Preliminaryroutines

Datacheck

Step 1Intermediatemomentum

Step 2Density/pressure

Step 3Momentumcorrection

Energycoupling

Boundaryconditions

Steadystate

Output

End

Make changes

Failed

Passed

Energy/temperaturecalculation

Yes

No

Timeloop

Yes

No

# ?0 2! " .-4!

"

Page 293: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

; - !

L & % %& %& % > C %% < 7 ;;/ !% ;8 % % % 1 %& > C

%< % % 6 K % C+=< >%&

% K & =% D %&# % & &> %

% & % % & %& & % >%+ += % % , (; & % %& D 6 /;; !% / L %

& &2 %/ 78 = 78 %% % & , (;

; $ !

# !$ &2 & %& >%D N %% 1 + & 7 )9!% )8 L + & % % 6 %& %1 % & K % &% K >% D %& + % % 7 K

7)')8 !% )8 % , (/ % =% & , 7, (/788

.' /' . ; / 9

' . ' ; ' / ' 9('

& 7, (/7&88

.' 9' .. ; ./

.' . ' ; .' /(.

-' - " #'

Page 294: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

=

1 1* 1' *4/- 45/ 1+.4.1* &1* 4.>/ -4/7- *4 (&)/-0

1 1* 1' *4/- .(4/+(* *() /?4/+(* 4.>/ -4/7-0

1

"@###

!

#

1

!AA!AAA!AAAA

1

B

=

1

A A $ &1* *++*,-

080;!

1

1 ->&&45.(3 45/ C*+.*% /-

1

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A " #0##9##

" #0##9##

" #0##9##

" =:=!

A " =:=!

A " 89A

" !

! "

A " A 9 A !

" 9 !

" 9 =!!

$

# ? -

"

Page 295: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

A " A :

" :

" :

" 8 :

$

" !

" !0#)#D

" 8 :=! $ -7//) &2 -&'()

$

1

1 &&7 2&+ 1* 1' *4.&( &2 &1* 4.>/ -4/7-

1

" !

! " !

" $ 1&((/14.C.4,

"

! " =!:=!! $ '! C/ &1.4,

A! " =!:=!! $ ' C/ &1.4,

" =:=!

A " =:=!

" =:=!

A " =:=!

A! " 8! 9 !

A " 8 9

A " 8 9

A " A! A A

" !

A " A 9

1

" ! $ -5*7/ 2'(14.&( )/+.C*4.C/-

"

" !0#:8 9 $ / />/(4 /(345 *4 (&)/ !

" :A

" :A

! " ! $ /?4/+(* 4.>/ -4/7

! " ! $ .(4/+(* 4.>/ -4/7

1

"

" E

" !0#:8 9

" :A

" :A

"

! " !

# ?

-' - " #'

Page 296: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

# K =% & K 7)'48 !% ) , (9 % = % & %

% 7 /9' !% /8& " %%= % &

1

"

" D

" !0#:8 9

" :A

" :A

"

! " !

$

" !

" $ ; -*2/4, 2*14&+

$

080#

" !0#)9#D

" !

"

$

# ?

54

43

3

2

2

1

1

(a) (b)

# ?8 0* #$ #$ *

"

Page 297: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

/9' !% / # % %%= %

; 1& $ !

F % !$ & !% ;# % !$ 7, (.8 , & % O% + # % O% + & & %& & % & % =% K & + % & -4/7 %>%

& < 7 !% )8 # L K % K # L &2> & %%% 5 # , 5 & % & & % =% O% &

K 7;9;8 7 K 7;9/88 # & -4/7 %% % L ' . & =% . K 2 ' & B9 'B , %& D% >% . 2 =% , >% %& D %& %, %& D %& >%

' & & B9 ' . % K -4/7 - N = & # % &

% % =% 6 % & > %% %& % = .); !% . =

; &

6 =% & & & 6 .-.)/. F D

-' - " #'

Page 298: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

=

1

1 45.- -'%+&'4.(/ 1* 1' *4/- 45/ 7+/--'+/ -6.415 *4 /*15 (&)/

1 >*?.>'> C* '/ ! *() >.(.>'> C* '/ #

1

!

= !! !

1

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!! " 0#)##! ;

" 0#)## ;

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! " ! 9 ! ; 9 ! ;

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" 9 ; 9 ! ;

$

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" ! ;

! " ! 9

" ;

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" 9

"

Page 299: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

% & ' .% & & ; % & / D % & 7 % & %&< & %8 & & 6 % %& , ()

;, 5!

# K & >% !$ # % % # + & L , >& % # % - # & & # % K & !% .B F '

;3 ?

%& D % K % 1 # %& D K & & %& D % K & % & % & %& D K 7;)'8 K 7/)8 >%& D %&

;: -$ ! %

6 % D %& D % = %& 6%%% D

$

" !

00#0! "

$

" !

" =:

$

# ?< ! "

-' - " #'

Page 300: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

> % & % , D !% 9

;; 1

# 7L & % % %8 K 1 >%& & > K 7 8 % % # %& & # % = & # += K %% , (4

=

A

1

1 -,>>/4+.1 %&'()*+, 1&().4.&(- 2&+1/)0 &(/ 1&>7&(/(4 &2 C/ &1.4,

1 2&+1/) 4& G/+&

1

A

=

1

" !

080 $ -,>>/4+, 2 *3

"

"

" !

"

" ;= 9 =

= " ;

= "

$

$

# ?= - **

"

Page 301: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1

=

1

1 7'+7&-/ H 1* 1' *4.&(- &2 +/-.)'* -0

1

1

!

! !!

=

! " #0###)##

" #0###)##

" #0###)##

" #0###)##

" !

! " =! ; ! $ )/(-.4, &+ 7+/--'+/

" = ; $ '! C/ &1.4, &+ >*-- 2 '?

" = ; $ ' C/ &1.4, &+ >*-- 2 '?

" = ; $ /(/+3, &+ 4/>7/+*4'+/

! " !

"

"

"

!00 !

! " !

! "

00

"

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00

"

"

00

"

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# ?> - "

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Page 302: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

?8 -

% + % % + # % K %>% % % &! 7H8 % %% 9 # H > > 2

;

# K A

.

.' .

..

.

'(;

# K + % + & K

?< &/ : "3

6 %& = 6 %& % K & % % & C < & )

6 &- & % C < !% 9 K & 4

# % %& %%% K *'.

# K & K & %+ # & % %&# & D K K

K =% !% 9 , 3 ';# % !$D & +

, + % % C < 1 N %

!'

' F HN , # ! '((*

. 5 R #$ , ! '((9

; "! 0 12 5: # , 2 8 9 6 : .BBB

/ "! 0 12 " &2 !$

= % 2 2 2 2 2 6: *493*B .BBB

!'

Page 303: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

9 H ! R ! J B*B;/ $ %

) # - &>L + D % 3 >%% . 5, /';3.) '(()

4 5 " J ! , % %& 2 2 2 2 2 68 9B;3.* '(((

* 6 2 "2 2

2 2 2 3: .493*/ '(*'( 6 5 : , % 2 2 2 2 , 26 'B'(3;) '((.

'B # - F H 6 & %% >

+ % % %% 2 2 . 58.*)9344 '((.

'' 5 : 5 # ,

. ! '(()'. 6 % + % + %& .

7 %% .BBB8

'; "! 0 12 $F 5 ! % & >% O& %& D 2 2 2 2 ,35 '3.; '(()

-' - " #'

Page 304: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

%;')) ' %)'9" 2

# 31 K >

! A

B 6'

! A

B 6.

! A

B 6;

5 K L

B 6/

& K 7K 6'8 & K K

'

'

B 69

& K 7K 6;8 & L

B 6)

Page 305: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 & K & K K

'

'

'

64

K 76'8 7698 7648 %& D %& > K % # % >% %& D %& 1 # > K & %& D %&

1-- : 1

Page 306: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

,'

)9 2

F ' &1 C H1 < = %& % % !% '; F '

& %%% %%= % 1 & : % % % H1 %% D = D %%

H1 A

% D= %%= P

%& > % & %&P

%% %% % & %% & D=P & & % !% .

# % > &% %&

B $'

L 7 8 N 7 & %8 & K 7$'8P =%

B B

( $.

@# " % '(((

Page 307: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

6 B % 7 8 ' ' . ! % %1 K 7$'8 7$.8 + &

!'

'

!'

,

-

,

-

B

!'

'

B( B $;

& 7D=8

.$/

-% $9

& B # % 1 K 7$;8 + 1

& A

' = K 7$'8 7$.8 7 8 K 7$;8P K 7$'8 7$.8 % %& & K 7$;8

. # K 7$'8 7$.8 + K 7$;8 & D= A

B

,

- B $)

; # & 7 D 8 1 > %% & % &

/ # . & L K K 7$;8 K 7$'8 7$.8& % & & H1 7H8

9 D= & 7$)8 : % > K 7$;8 1

!'

$4

% 6 % % & + D= -%A

,

- $*

1-- :

Page 308: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

K 7$*8 K 7$48 K 7$;8 % %%= + %%= K 7$'8 K 7$.8 & & 7 !% '; F '8

%%= K 7$'8 7$.8 & H 5 K 7$;8 % %%= P

B

- $(

- 7%

8 K 7$(8 7$;8 =% % % >

!'

B

'

,

-

-

,

-

-

,

-

,

-

BB B

-

'

'

(

B B B

' . ' . ! $'B# H %%= K 7$;8 %% K 7$'B8 A

' # % & & P

1 & % 7% >

=% % % % % 8 # 1 N - %

. L % P K 7$'B8% > + %%=

; %% B # % K 7$'8 K 7$'B8 L = % -% & = % + & & % %%

/ K 7$'B8 7 8 H1 %%= K 7$'8 7$.8 % % % 2 %%= & % & H

1-- :

Page 309: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

9 % % & '' '

'

% % 2 % =%> & .

) # H + %%=> % %

'

B $''

# %% & > %%=

# H & & % H1 %%= %% 3L %& 3L %&

% # 1 %& A

.

.

. B '

' . ' B = &

.

'

.

, $' $. & %& 'B'B ''B & H1 % = !% .

2.5

2.0

1.5

1.0

0.5

0

–0.5

–1.0

–1.5

–2.0

–2.5–1.0 –0.6 –0.2 0 0.2 0.6 1.0

Exactp = 2p = 3p = 4p = 5

x

u

# .

1-- :

Page 310: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

2.5

2.0

1.5

1.0

0.5

0

–0.5

–1.0

–1.5

–2.0

–2.5–1.0 –0.6 –0.2 0 0.2 0.6 1.0

Exactp = 2p = 3p = 4p = 5

x

u

# 0 3

1-- :

Page 311: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

#;/ 4 '

# >& & + > D %& 6 )* !% ) # =% K & > + , !' , K 7'./8 K

B !'

& >& & K &2 1 &

#

!.

=% % > &% % = 7 !% ;8 5 & K / 7, !'788 & % %% H <

/

'

/

/

'

;

/

/ 1

!;

' / 1 7 8 # %& %%= K #3H1 7 !% .8 & 5 & 7, !'788

'';

/

/ ' .

'.;

/

/ . ;

';;

/

/ ; ' !/

'' '. '; ' . ; % , > & 5

0 /

0

/ 0

0 /

0

)./

1

0

!9

Page 312: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& # & K & / , !'7&8

0'

)./

; ' 0.

)./

' . !)

0' 0. %%% # & K 7!;8 7!98 & >&

% K 7!;8 & 7 /8

/

/

!#

.'

//#

'

;

/

/

/#

!4

!# & /

. //# = //#

# & K K K 7!/8 / , !'78 # & K 7!98 7!)8

1

1

2

2

3

3

I

I

3

2

1

21

(a) (b)

# . 0* " ' #$ ) #$ *

1-- :

Page 313: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

#'

& K + + L %& % + # % % & K & # % % %& !% * + % # % % - &

+ %& = & + & % & & + # %% + & 1 + % K % K # & % %&

' 2 % & & " 2

/ . & K % & # + 2

/ ; & & % %> + % & #

' /

Page 314: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

&

& % & & K & % + % "& & + % # " % & & % + & % &

/ 9

K & % % & - >K 6 = + > +

+

) + #

+

4 # & % & && % >1

/'

*

6 ' %

% > # > & K & & % % & & & %

+ & & & # % % & %% !% )

1-- :

Page 315: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

' '9) 3 -#

6 % & 3 D % !% ) %% = &D =% % % D% % # % % & % D % , ' $ & + 2 %

# 2 K & % & # & % &

# 3 & %% % % & % % # % & 7, '8 & C# %&< & % & C> < &

# 5 # % & % 6 , ' > %

Semi-inverse

Semi-inverse

Semi-inverse

Semi-inverse

Dire

ct

Direct

Turbulent

TurbulentLaminar Transition

Stagnation

stream

Turbulent wake

# . 2! 0* * * 4! "

Page 316: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

& L # > % &2 & % , . D % & 3 %

, # %& > % & )'. !% ) 7: $ 18

Unstructured gridsor multiblock Euler

inviscid method

Direct calculation

Lag-entrainmentboundary layerviscous method

Direct calculation

Cp,s

ρVN

VN δ*

(a)

Unstructured gridsor multiblock Euler

inviscid method

Direct calculation

Lag-entrainmentboundary layerviscous method

Direct calculationδ, θ, Cf, H

Cp,s

(b)

ρVNm + 1 = ρVN

m + K*θ

uv

duv

ds– θ

uv

du i

ds

m

dds

ρVN = (ρv uv δ*)

# 0 " ( ' #$ ) #$

1-- :

Page 317: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

, . N %P # P & 1 P 1 P 1 N P %+ % %P P % >% P % & P &% 1 & P % 1 P %% %% ! , & K A

B

'

.

'+.

'

K & & >

#

'

. '

#

.

%' '

#

. .+.

#

;

B'

#

.*

' B9U B9

#

U

#

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' B'+.

/

BB. .

B*

;

BB'

9

& K ' %+ % % +

'

B

'

'

)

N P % & P+ &P N P % P &% U U % K& K& & D &

1-- :

Page 318: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

" & K % % , . & % # % % % &

1-- :

Page 319: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics
Page 320: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

1' :

& " %

6&& $ .'* 35;

6 56 ;) ;* 92

6 'B. 'B; 257

61 @ )4 44 ::P '99 299

6= @ '.B 25; 26,

6 6# '.B 26,

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6 5@ ./; ./) .9( .)B .). .)/ .)9

37, 372 373 375

6 6 )4 ::P ')' 297

61 $ '.B 25;

61 @ .; 9,

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$- ,# '.B 26,

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./) ./4 ./* ./( .9. .9; .99 .)B .)'

.). .); .)/ .)) .)( 37, 372 373 375

$ 5 '.B './ 25;

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$ @ .)9 375

Page 321: ZIENKIEWICZ O. C. the Finite Element Method (5th Ed.) Vol 3 - Fluid Dynamics

! ? '/) 298

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44 *' :: :; ;,P (4 (* (( 256 258P '/*

')' '). 298 297P '4/ '4) '*9 '*) '*4

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! + H! '.B 25;

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! 6 ./; 37,

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')/ 29:

= 6 'B. 258

& !6 ';B 262

'B. 258

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