Taylor Expansion

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  • 7/30/2019 Taylor Expansion

    1/6

    8 T h i r d o r d e r e x p a n s i o n s

    8 . 1 G e n e r a l

    A s s o m e t h i n g n e w w e w i l l i n t r o d u c e t h i r d o r d e r t e r m s i n t h e b o u n d a r y e l e -

    m e n t m o d e l . S o f r o m h e r e l e t t h e p e r t u r b a t i o n e x p a n s i o n s o f a n d b e o f

    t h e f o r m

    = "

    1

    + "

    2

    2

    + "

    3

    3

    + O "

    4

    8 . 1

    = "

    1

    + "

    2

    2

    + "

    3

    3

    + O "

    4

    8 . 2

    T h e s e r e d e n i t i o n s o f t h e e x p a n s i o n s o f a n d d o n o t c o n t r a d i c t t h e f o r m e r

    d e n i t i o n s 2 . 4 4 a n d 2 . 4 4 . T h u s t h e r e s u l t s o b t a i n e d i n t h e p r e v i o u s p a r t s

    o f t h i s w o r k a r e s t i l l v a l i d b u t t h e y m a y b e i m p r o v e d b y t h e i n t r o d u c t i o n o f

    t h i r d o r d e r t e r m s .

    I t i s e a s i l y s h o w n t h a t t h e t h i r d o r d e r p o t e n t i a l

    3

    m u s t s a t i s f y t h e L a p l a c e -

    e q u a t i o n a n d t h u s t h e b o u n d a r y i n t e g r a l e q u a t i o n 2 . 4 9 i s v a l i d f o r t h e t h i r d

    o r d e r p o t e n t i a l . A n a l y t i c a l l y t h i s i s w r i t t e n a s

    r

    2

    3

    = 0 8 . 3

    +

    Z

    ,

    0

    3

    @ G

    @ n

    0

    , G

    @

    3

    @ n

    0

    d s =

    3

    x 8 . 4

    I n d i s c r e t e f o r m t h e b o u n d a r y i n t e g r a l e q u a t i o n s o b t a i n e d f o r

    3

    w i l l h a v e

    t h e s a m e c o e c i e n t s a s t h e e q u a t i o n s f o r

    1

    a n d

    2

    a s d e s c r i b e d i n s e c t i o n

    4 . 5 . T h i s m e a n s t h a t t h e c a l c u l a t i o n t i m e p e r t i m e s t e p w i l l b e i n c r e a s e d b y

    r o u g h l y 5 0 b y i n t r o d u c i n g t h i r d o r d e r t e r m s . F o r v e r y w e a k l y n o n l i n e a r

    w a v e s i t m a y n o t b e w o r t h t h e e x t r a c a l c u l a t i o n t i m e t o o b t a i n t h e t h i r d

    o r d e r p o t e n t i a l b u t f o r w a v e s o f i n t e r m e d i a t e n o n l i n e a r i t y t h e t h i r d o r d e r

    t e r m s m a y m a k e t h i s m o d e l f e a s i b l e a n d t h i s m o d e l w i l l s t i l l b e a l o t f a s t e r

    t h a n a f u l l n o n l i n e a r B E M .

    8 . 2 F r e e s u r f a c e a n d o p e n b o u n d a r y c o n d i t i o n s

    8 . 2 . 1 G e n e r a l

    T h e m o s t d e m a n d i n g t a s k b y i n t r o d u c i n g t h i r d o r d e r t e r m s i n t h e B E M i s

    t h e e v a l u a t i o n o f n e w b o u n d a r y c o n d i t i o n s b a s e d o n t h e d y n a m i c 3 . 3 1 a n d

    k i n e m a t i c 3 . 3 2 f r e e s u r f a c e b o u n d a r y c o n d i t i o n s m o d i e d b y d i s s i p a t i v e

    t e r m s f o r a s p o n g e l a y e r f o r i n s t a n c e g i v e n b y 3 . 4 2 .

    6 8

  • 7/30/2019 Taylor Expansion

    2/6

    T a y l o r e x p a n d i n g t h e k i n e m a t i c b o u n d a r y c o n d i t i o n f r o m z = 0 w e g e t

    @

    @ t

    ,

    @

    @ z

    +

    @

    @ x

    @

    @ x

    + x

    +

    @

    @ z

    @

    @ t

    ,

    @

    @ z

    +

    @

    @ x

    @

    @ x

    + x

    +

    2

    1

    2

    @

    2

    @ z

    2

    @

    @ t

    ,

    @

    @ z

    +

    @

    @ x

    @

    @ x

    + x

    +

    3

    1

    6

    @

    3

    @ z

    3

    @

    @ t

    ,

    @

    @ z

    +

    @

    @ x

    @

    @ x

    + x

    = O

    4

    a t z = 0 8 . 5

    +

    @

    @ t

    ,

    @

    @ z

    +

    @

    @ x

    @

    @ x

    + x

    ,

    @

    2

    @ z

    2

    +

    @

    2

    @ x @ z

    @

    @ x

    ,

    1

    2

    2

    @

    3

    @ z

    3

    +

    1

    2

    2

    @

    3

    @ x @ z

    2

    @

    @ x

    +

    3

    1

    6

    @

    3

    @ z

    3

    @

    @ z

    ,

    @

    @ t

    ,

    @

    @ x

    @

    @ x

    = O

    4

    a t z = 0 8 . 6

    S i m i l a r l y f r o m t h e d y n a m i c b o u n d a r y c o n d i t i o n w e g e t

    @

    @ t

    + g +

    1

    2

    r

    2

    + x

    +

    @

    @ z

    @

    @ t

    + g +

    1

    2

    r

    2

    + x

    +

    2

    1

    2

    @

    2

    @ z

    2

    @

    @ t

    + g +

    1

    2

    r

    2

    + x

    +

    3

    1

    6

    @

    3

    @ z

    3

    @

    @ t

    + g +

    1

    2

    r

    2

    + x

    = O

    4

    a t z = 0 8 . 7

    +

    @

    @ t

    + g +

    1

    2

    r

    2

    + x

    +

    @

    2

    @ t @ z

    +

    1

    2

    @

    @ z

    ,

    r

    2

    + x

    @

    @ z

    +

    1

    2

    2

    @

    3

    @ t @ z

    2

    +

    1

    4

    2

    @

    2

    @ z

    2

    ,

    r

    2

    +

    1

    2

    x

    2

    @

    2

    @ z

    2

    +

    3

    1

    6

    @

    3

    @ z

    3

    @

    @ t

    + g +

    1

    2

    r

    2

    + x

    = O

    4

    a t z = 0 8 . 8

    6 9

  • 7/30/2019 Taylor Expansion

    3/6

    P e r t u r b a t i o n e x p a n d i n g a n d i n 8 . 6 a n d k e e p i n g o n l y t e r m s o f t h i r d

    o r d e r i n " w e g e t

    @

    3

    @ t

    ,

    @

    3

    @ z

    + x

    3

    = ,

    @

    1

    @ x

    @

    2

    @ x

    ,

    @

    2

    @ x

    @

    1

    @ x

    +

    1

    @

    2

    2

    @ z

    2

    +

    2

    @

    2

    1

    @ z

    2

    ,

    1

    @

    2

    1

    @ x @ z

    @

    1

    @ x

    +

    1

    2

    2

    1

    @

    3

    1

    @ z

    3

    8 . 9

    +

    @

    3

    @ t

    ,

    @

    3

    @ n

    0

    + x

    3

    = ,

    @

    1

    @ x

    @

    2

    @ x

    ,

    @

    2

    @ x

    @

    1

    @ x

    ,

    1

    @

    2

    2

    @ x

    2

    ,

    2

    @

    2

    1

    @ x

    2

    ,

    1

    @

    1

    @ x

    @

    @ x

    @

    1

    @ n

    0

    ,

    1

    2

    2

    1

    @

    2

    @ x

    2

    @

    1

    @ n

    0

    8 . 1 0

    S i m i l a r l y p e r t u r b a t i o n e x p a n d i n g 8 . 8 a n d k e e p i n g o n l y t e r m s o f t h i r d o r d e r

    w e g e t

    @

    3

    @ t

    + g

    3

    + x

    3

    = ,

    @

    1

    @ x

    @

    2

    @ x

    ,

    @

    1

    @ z

    @

    2

    @ z

    ,

    1

    @

    2

    2

    @ t @ z

    ,

    2

    @

    2

    1

    @ t @ z

    ,

    1

    2

    1

    @

    @ z

    ,

    r

    1

    2

    , x

    1

    @

    2

    @ z

    , x

    2

    @

    1

    @ z

    ,

    1

    2

    2

    1

    @

    3

    1

    @ t @ z

    2

    ,

    1

    2

    x

    2

    1

    @

    2

    1

    @ z

    2

    8 . 1 1

    +

    @

    3

    @ t

    + g

    3

    + x

    3

    = ,

    @

    1

    @ x

    @

    2

    @ x

    ,

    @

    1

    @ n

    0

    @

    2

    @ n

    0

    ,

    1

    @

    @ t

    @

    2

    @ n

    0

    ,

    2

    @

    @ t

    @

    1

    @ n

    0

    ,

    1

    @

    1

    @ x

    @

    @ x

    @

    1

    @ n

    0

    +

    1

    @

    1

    @ n

    0

    @

    2

    1

    @ x

    2

    , x

    1

    @

    2

    @ n

    0

    , x

    2

    @

    1

    @ n

    0

    +

    1

    2

    2

    1

    @

    @ t

    @

    2

    1

    @ x

    2

    +

    1

    2

    x

    2

    1

    @

    2

    1

    @ x

    2

    8 . 1 2

    T h e e q u a t i o n s 8 . 9 a n d 8 . 1 1 s h o w t h e t e r m s a s t h e y w i l l l o o k d i r e c t l y a f t e r

    t h e e x p a n s i o n w h i l e t h e e q u a t i o n s 8 . 1 0 a n d 8 . 1 2 a r e r e w r i t t e n t o f o r m s

    r e a d y f o r i m p l e m e n t a t i o n i n a c o m p u t e r p r o g r a m .

    8 . 2 . 2 U p d a t i n g - A p p l y i n g a n i m p l i c i t A d a m s m e t h o d

    A s w e h a v e s e e n i n t h e p r e v i o u s s e c t i o n 8 . 2 . 1 t h e t h i r d o r d e r e x p r e s s i o n s

    f o r t h e d y n a m i c a n d k i n e m a t i c f r e e s u r f a c e b o u n d a r y c o n d i t i o n s a r e q u i t e

    7 0

  • 7/30/2019 Taylor Expansion

    4/6

    c o m p l i c a t e d a n d t h u s t o a v o i d c o m p l i c a t i n g t h i n g s e v e n m o r e w e w i l l n o t

    T a y l o r e x p a n d t h e s e e q u a t i o n s i n t i m e . I n s t e a d w e w i l l u s e a n e x p l i c i t A d a m s -

    B a s h f o r t h m e t h o d f o r t h e u p d a t i n g o f

    k

    a n d t h e n u s e t h e k i n e m a t i c b o u n d -

    a r y c o n d i t i o n f o r n d i n g n e w v a l u e s o f

    @

    k

    @ t

    a s d e s c r i b e d i n s e c t i o n 4 . 3 . 3 .

    W e h a v e c h o s e n a n e x p l i c i t A d a m s - B a s h f o r t h m e t h o d o f h i g h e r o r d e r t h a n

    b e f o r e k

    a

    = 3 a c c o r d i n g t o 4 . 2 5 w i t h t h e c o e c i e n t s A

    0

    = 5 5 = 2 4

    A

    1

    = , 5 9 = 2 4 A

    2

    = 3 7 = 2 4 a n d A

    3

    = , 9 = 2 4 . S o s t i l l l e t t i n g i n d i c e s m ; j "

    r e f e r t o t i m e t = t

    m

    a n d s p a c e x = x

    j

    t h e n e w u p d a t i n g o f w i l l b e

    k m + 1 j

    =

    k m j

    + t

    5 5

    2 4

    @

    k

    @ t

    m j

    ,

    5 9

    2 4

    @

    k

    @ t

    m , 1 j

    +

    3 7

    2 4

    @

    k

    @ t

    m , 2 j

    ,

    9

    2 4

    @

    k

    @ t

    m , 3 j

    ; k 2 f 1 ; 2 ; 3 g 8 . 1 3

    A f t e r s o m e c o n s t r u c t i v e c o n v e r s a t i o n s w i t h J e s p e r S k o u r u p w e c h o s e t o

    u p d a t e o n t h e f r e e s u r f a c e b y a n i m p l i c i t A d a m s m e t h o d . T h i s p r o c e -

    d u r e i s o f t e n a t t r i b u t e d t o A d a m s - M o u l t o n a n d t h i s w i l l a l s o b e d o n e h e r e

    e v e n t h o u g h t h e f o r m u l a i s d u e t o A d a m s . S i m i l a r l y t o t h e e x p l i c i t A d a m s -

    B a s h f o r t h m e t h o d s a n i m p l i c i t A d a m s - M o u l t o n m e t h o d i s o f t h e f o r m

    y

    m + 1

    = y

    m

    + t B

    0

    f

    m + 1

    + + B

    k

    a

    f

    m + 1 , k

    a

    8 . 1 4

    C h o o s i n g k

    a

    = 3 w e h a v e t h e c o e c i e n t s B

    0

    = 9 = 2 4 B

    1

    = 1 9 = 2 4 B

    2

    =

    , 5 = 2 4 a n d B

    3

    = 1 = 2 4 . T h e m e t h o d i s o f t e n u s e d a s t h e c o r r e c t o r s t e p i n a

    p r e d i c t o r - c o r r e c t o r m e t h o d b u t w e u s e t h e m e t h o d f o r p r e d i c t i o n o f

    k

    o n l y .

    T h e d y n a m i c f r e e s u r f a c e b o u n d a r y c o n d i t i o n w i t h F

    k

    a s r i g h t h a n d s i d e

    c a n f o r k 2 f 1 ; 2 ; 3 g b e w r i t t e n a s

    @

    k

    @ t

    m + 1 j

    + g

    k m + 1 j

    + x

    k m + 1 j

    = F

    k m + 1 j

    8 . 1 5

    I n s e r t i n g

    @

    k

    @ t

    m + 1 j

    i n t h e e q u a t i o n f o r t h e i m p l i c i t A d a m s - M o u l t o n m e t h o d

    w e g e t

    k m + 1 j

    =

    1

    1 + t B

    0

    x

    "

    k m j

    + t

    B

    0

    ,

    , g

    k m + 1 j

    + F

    k m + 1 j

    + B

    1

    @

    k

    @ t

    m j

    + B

    2

    @

    k

    @ t

    m , 1 j

    + B

    3

    @

    k

    @ t

    m , 2 j

    8 . 1 6

    7 1

  • 7/30/2019 Taylor Expansion

    5/6

    W h e n

    k m + 1 j

    a n d

    k m + 1 j

    a r e k n o w n t h e d y n a m i c s u r f a c e b o u n d a r y

    c o n d i t i o n s w i l l p r o v i d e

    @

    k

    @ t

    m + 1 j

    t o b e u s e d i n t h e f o l l o w i n g t i m e s t e p s .

    A f t e r h a v i n g s o l v e d t h e b o u n d a r y i n t e g r a l e q u a t i o n s t h e k i n e m a t i c f r e e s u r -

    f a c e b o u n d a r y c o n d i t i o n s s u p p l y

    @

    k

    @ t

    m + 1 j

    a t ,

    f 0

    T h e m e t h o d d e s c r i b e d a b o v e h a s b e e n i m p l e m e n t e d a n d i s h e r e a f t e r u s e d

    i n t h e t h i r d o r d e r m o d e l a l s o f o r t h e r s t a n d s e c o n d o r d e r t e r m s . T h e

    m e t h o d s e e m s s t a b l e a n d r e l i a b l e w h e n t h e C o u r a n t n u m b e r i s b e l o w u n i t y

    s a y C r = 0 8 . S i n c e t h e m o d e l m a y t u r n o u t t o b e u n s t a b l e w h e n t h e C o u r a n t

    n u m b e r i s g r e a t e r t h a n u n i t y c a r e s h o u l d b e t a k e n t o e n s u r e t h a t t h i s d o e s

    n o t h a p p e n .

    I t s h o u l d b e n o t e d t h a t t h e A d a m s - B a s h f o r t h - M o u l t o n m e t h o d s a r e n o r -

    m a l l y u s e d i n p r e d i c t o r - c o r r e c t o r m e t h o d s a n d s i n c e o u r m e t h o d r e p r e s e n t s

    t h e p r e d i c t o r s t e p o n l y s t a b i l i t y c a n n o t b e g u a r a n t e e d . T o i m p r o v e s t a b i l i t y

    a c o r r e c t o r s t e p c a n b e i n c l u d e d i n t h e m o d e l b u t s i n c e t h i s r o u g h l y w o u l d

    d o u b l e t h e c a l c u l a t i o n t i m e a n d n o t i m p r o v e t h e a c c u r a c y b y m u c h w e h a v e

    n o t i m p l e m e n t e d a c o r r e c t o r s t e p .

    8 . 3 P i s t o n b o u n d a r y c o n d i t i o n

    A p i s t o n t y p e w a v e - m a k e r s e e s e c t i o n s 3 . 3 a n d 3 . 4 c a n i n m a t h e m a t i c a l

    t e r m s b e d e s c r i b e d b y a b o u n d a r y c o n d i t i o n o n t h e f o r m 3 . 1 3 a n d

    @

    @ z

    = 0

    i . e .

    @

    @ n

    0

    = ,

    @

    @ x

    T a y l o r e x p a n d i n g 3 . 1 3 f r o m x = 0 w e g e t

    ,

    @

    @ x

    +

    @

    @ x

    ,

    @

    @ x

    +

    1

    2

    2

    @

    2

    @ x

    2

    ,

    @

    @ x

    +

    1

    6

    3

    @

    3

    @ x

    3

    ,

    @

    @ x

    + O

    4

    = V

    n

    ; a t ,

    r 1 0

    8 . 1 7

    P e r t u r b a t i o n e x p a n d i n g a n d a n d k e e p i n g o n l y t e r m s o f t h i r d o r d e r w e

    g e t

    ,

    @

    3

    @ x

    ,

    1

    @

    2

    2

    @ x

    2

    ,

    2

    @

    2

    1

    @ x

    2

    ,

    1

    2

    2

    1

    @

    3

    1

    @ x

    3

    = V

    n 3

    8 . 1 8

    7 2

  • 7/30/2019 Taylor Expansion

    6/6

    U s i n g t h e L a p l a c e - e q u a t i o n

    @

    1

    @ n

    0

    = V

    n 1

    a n d

    @

    @ z

    = 0 w e g e t

    @

    3

    1

    @ x

    3

    =

    @

    @ x

    ,

    @

    2

    1

    @ z

    2

    = ,

    @

    2

    @ z

    2

    @

    1

    @ x

    =

    @

    2

    @ z

    2

    @

    1

    @ n

    0

    =

    @

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    T h u s 8 . 1 8 c a n b e r e d u c e d t o

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