□von Neumann最大最小定理
課題 2 解答
2.6 ʹର͢Δ Lagrange ؔΛ
L (a, u, v) = f (u) + L
S(a, u, v) = p · u + v · ( − K (a) u + p)
ͱ͓͘ɽ v ∈ U Lagrange Ͱ͋Δɽ L ͷશඍʹରͯ͠ɼ
L
′(a, u, v) [b, u, ˆ v] ˆ
= − {
v ·
( ∂K (a)
∂a
1u ∂K (a)
∂a
2u )}
b
+ p · u ˆ − v · K (a) ˆ u (= 0 ⇐ K
T(a) v = p ) + ˆ v · ( − K (a) u + p) (= 0 ⇐ K (a) u = p )
= g · b ∀ (b, u, ˆ v) ˆ ∈ Ξ × U × U (2.6)
͕Γཱͭɽ͜͜Ͱɼ g ೖ๏ʹΑΔࣜ (2.4) ͱҰக͢Δɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
͞ΒʹɼͦΕΛ͏Ұ a Ͱภඍ͢Εɼ
H =
∂
2f ˜
∂a
1∂a
1∂
2f ˜
∂a
1∂a
2∂
2f ˜
∂a
2∂a
1∂
2f ˜
∂a
2∂a
2
= l e
Y
2 (p
1+ p
2)
2a
310
0 2p
22a
32
(2.5)
ͱͳΔɽ a
1, a
2> 0 ͷͱ͖ɼ H ਖ਼ఆͱͳΔɽ
21 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
Ұํɼ j ∈ { 1, 2 } ʹରͯ͠
L
S(a,u)(a, u, v) [b
i, υ ˆ
j] = v · {− (K
′(a) [b
i]) u − K (a) ( ˆ υ
j) } = 0
∀ (b
i, υ ˆ
j) ∈ T
S(a, u) ΑΓɼ࣍ΛಘΔɽ
υ ˆ
j= − K
−1(a) (K
′(a) [b
i]) =
− u
1a
10
− u
1a
1− u
2− u
1a
2
( b
i1b
i2)
(2.8)
ࣜ (2.8) Λࣜ (2.7) ʹೖ͠ɼࣗݾਵؔΛ༻͍Εɼ
h (a, u, v) [b
1, b
2]
= L
(a,u)(a,u)(a, u, v) [(b
1, υ ˆ
1) , (b
2, υ ˆ
2)]
= b
1· (Hb
2) (2.9)
ͱͳΔɽ͜͜Ͱɼ H ೖ๏ͰಘΒΕͨࣜ (2.5) ͱҰக͢Δɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
Hesse ߦྻ࣍ͷΑ͏ʹಘΒΕΔɽڐ༰ू߹ͱڐ༰ํू߹͋Δ͍໘Λ
S = { (a, u) ∈ Ξ × U | h (a, u) = 0
U′} ,
T
S(a, u) = { (b, υ) ˆ ∈ Ξ × U | h
au(a, u) [b, υ] = ˆ 0
Rn} . ͱ͓͘ɽ L ͷઃܭม (a, u) ʹର͢Δ 2 ֊ภඍɼ
L
(a,u)(a,u)(a, u, v) [(b
1, υ ˆ
1) , (b
2, υ ˆ
2)]
= ( L
0a(a, u, v) [b
1] + L
0u(a, u, v) [ ˆ υ
1])
a[b
2] + (L
0a(a, u, v) [b
1] + L
0u(a, u, v) [ ˆ υ
1])
u[ ˆ υ
2]
= ( b
2ˆ υ
2)
· (
H
LS( b
1ˆ υ
1))
∀ (b
1, υ ˆ
1) , (b
2, υ ˆ
2) ∈ T
S(a, u) (2.7) ͱͳΔɽ͜͜Ͱɼ࣍ͷΑ͏Ͱ͋Δɽ
H
LS=
( L
SaaL
SauL
SuaL
Suu)
= −
0
R2×2( v
TK
a1v
TK
a2) ( K
aT1v K
aT2v )
0
R2×2
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ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
2.8 ( ੍͖ͭʹର͢Δޯ๏ )
ࢼߦ x
k∈ S ʹ͓͍ͯ f
0(x
k), f
i1(x
k) = 0, · · · , f
i|IA|(x
k) = 0, g
0(x
k), g
i1(x
k), · · · , g
i|IA|(x
k) Λطͱ͢Δɽ·ͨɼ A ∈ R
d×dΛਖ਼ఆ࣮ରশߦྻɼ c
aΛਖ਼ͷఆͱ͢Δɽ͜ͷͱ͖ɼ
q (y
g) = min
y∈X
{
q (y) = 1
2 y · (c
aAy) + g
0(x
k) · y + f
0(x
k)
� �
� �
f
i(x
k) + g
i(x
k) · y ≤ 0 for i ∈ I
A(x
k) }
Λຬͨ͢ x
k+1= x
k+ y
gΛٻΊΑɽ
2.8 ͷ Lagrange ؔΛ࣍ͷΑ͏ʹ͓͘ɽ
L
Q(y, λ
k+1) = q (y) + ∑
i∈IA(xk)
λ
i k+1(f
i(x
k) + g
i(x
k) · y)
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
■ ੍͖ͭʹ͓͚Δޯ๏ͱ Newton ๏ [1, 3.7 અ , 3.8 અ ]
͜ΕҎ߱ɼ࠷దઃܭʹ͓͚Δઃܭม ϕ Λ x ͱ͔͘͜ͱʹ͢Δɽ
2.7 ( ੍͖ͭ࠷దԽ )
X = R
dͱ͢Δɽ f
0, · · · , f
m∈ C
2(X ; R ) ʹରͯ͠ɼ min
x∈X{ f
0(x) | f
1(x) ≤ 0, · · · , f
m(x) ≤ 0 } Λຬͨ͢ x ΛٻΊΑɽ
ෆ੍͕ࣜຬͨ͞ΕΔڐ༰ू߹ͱ༗ޮͳ੍ʹର͢Δఴ͑ࣈͷू߹Λ S = { x ∈ X | f
1(x) ≤ 0, · · · , f
m(x) ≤ 0 } ,
I
A(x) = { i ∈ { 1, · · · , m } | f
i(x) ≥ 0 } = {
i
1, · · · , i
|IA(x)|} ͱ͓͘ɽ
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ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
2.8 ͷ࠷খ y
gʹ͓͚Δ KKT ݅ɼ L
Qy(y, λ
k+1) = c
aAy
g+ g
0(x
k) + ∑
i∈IA(xk)
λ
i k+1g
i(x
k) = 0
X′, (2.10) L
Qλk+1(y, λ
k+1) = f
i(x
k) + g
i(x
k) · y
g≤ 0 for i ∈ I
A(x
k) , (2.11) λ
i k+1(f
i(x
k) + g
i(x
k) · y
g) = 0 for i ∈ I
A(x
k) , (2.12)
λ
i k+1≥ 0 for i ∈ I
A(x
k) (2.13)
ͱͳΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
X
X
�x
kR
g
2g
0q
0f
2+g
2· y
g=0 f
1+g
1· y
g=0
g
1y
gਤ 2.5: ੍͖ͭʹର͢Δޯ๏
27 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
(2) 状態決定問題を解いて,評価関数を計算する.
(4) 勾配法で設計変数の変動を求める.
(6) 設計変数を更新して ( k +1),(2) をおこなう.
(7) 終了条件 Yes
No (3) 随伴問題を解いて,評価関数の勾配を計算する.
(5) Lagrange 乗数を求める.
(1) 初期設定 ( k =0)
(8) 終了
( k +1 → k )
ਤ 2.6: ੍͖ͭ࠷దԽʹର͢Δޯ๏ͷΞϧΰϦζϜ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
͜͜Ͱɼ y
g0, y
gi1, · · · , y
gi|IA|
Λ i ∈ I
A(x
k) ͝ͱʹޯ๏Λద༻ͨ͠ͱ͖ͷ ղͱ͢Δɽ͢ͳΘͪɼ
y
gi= − (c
aA)
−1g
ifor i ∈ I
A(x
k) .
·ͨɼ λ
k+1∈ R
|IA|Λະͷ Lagrange ͱ͢Δɽ͜ͷͱ͖ɼ y
g= y
g(λ
k+1) = y
g0+ ∑
i∈IA(xk)
λ
i k+1y
giࣜ (2.10) Λຬͨ͢ɽ͞Βʹɼࣜ (2.11)
g
i1· y
gi1· · · g
i1· y
gi|IA|.. . . .. .. . g
i|IA|
· y
gi1· · · g
i|IA|
· y
gi|IA|
λ
i1k+1.. . λ
i|IA|k+1
= −
f
i1+ g
i1· y
g0.. .
f
i|IA|+ g
i|IA|· y
g0
ͱͳΔɽ͜ͷ࿈ཱҰ࣍ํఔࣜΑΓɼ λ
k+1͕ܾఆ͞ΕΔɽ
29 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
(2) 状態決定問題を解いて,評価関数を計算する.
(8) 終了条件 Yes
No (4) 随伴問題を解いて,勾配と Hesse 行列を計算する.
(1) 初期設定 (k=0)
(9) 終了
(k+1→k) (5) Newton 法で設計変数の変動を求める.
(7) 設計変数を更新して (k+1),(2) をおこなう.
(6) Lagrange 乗数を求める.
勾配法で設計変数の変動を求める.
随伴問題を解いて,勾配を計算する.
Lagrange 乗数を求める.
(3) 制約関数の Hesse 行列
Yes
No
ਤ 2.7: ੍͖ͭ࠷దԽʹର͢Δ Newton ๏ͷΞϧΰϦζϜ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
2.9 ( ੍͖ͭʹର͢Δ Newton ๏ )
ࢼߦ x
k∈ X ʹ͓͍ͯɼ λ
k∈ R
|IA| KKT ݅Λຬͨ͢ͱ͢Δɽ·ͨɼ H
L(x
k) = H
0(x
k) + ∑
i∈IA(xk)
λ
ikH
i(x
k) ͱ͓͘ɽ͜ͷͱ͖ɼ
q (y
g) = min
y∈X
{
q (y) = 1
2 y · (H
L(x
k) y) + g
0(x
k) · y + f
0(x
k)
� �
� �
f
i(x
k) + g
i(x
k) · y ≤ 0 for i ∈ I
A(x
k) }
Λຬͨ͢ x
k+1= x
k+ y
gΛٻΊΑɽ
ޯ๏ͷ A Λ H
Lʹ͓͖͔͑Ε Newton ๏ʹͳΔɽ
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ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
0 1
a2
a1
a(0)=(1/2,1/2)T
0 1
bg0(0)
a(1)
a=(2/3,1/3)T a(2)
λ1(1)bg1(0)
λ1(2)bg1(1)
bg0(1)
a(5)
0 1 2 3 4 5
0.90 0.95 1.00
Cost function
f0/f0 init
1+f1
Step number k
(a) ࢼߦͷਪҠ (b) ධՁؔͷཤྺ
ਤ 2.9: ޯ๏ʹΑΔղ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
■ ྫ
0 0
1 15
a
1 01
a
2f
0(a
1,1–a
1) f
0(a
1,a
2)
˜
˜
10 5
ਤ 2.8: ମੵ੍͖ͭฏۉίϯϓϥΠΞϯε࠷খԽͷྫ
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ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ؔղੳͷجૅ
§ 3 ؔղੳͷجૅ
■ ۭؔؒ [1, 4.3 અ ]
• W
k,p( Ω; R
d)
: k ֊ඍ·Ͱ p Մੵͳؔ Ω → R
dͷू߹
(Sobolev ۭؒ : උͳϊϧϜۭؒ (Banach ۭؒ ) ͷੑ࣭Λͭ )
• W
0,2( Ω; R
d)
= L
2( Ω; R
d)
• W
k,2( Ω; R
d)
= H
k( Ω; R
d)
: H
1( Ω; R
d)
ͷ߹ɼͨͱ͑ɼੵ
(u, v)
H1(Ω;Rd)=
∫
Ω
{ u · v + (
∇ u
T)
· (
∇ v
T)}
dx ʹରͯ͠උͳੵۭؒ (Hilbert ۭؒ ) ͷੑ࣭Λͭɽ
• W
0,∞( Ω; R
d)
= L
∞( Ω; R
d)
: ༗ք͔ͭՄੵͳؔͷू߹
• W
1,∞( Ω; R
d)
: Lipschitz ࿈ଓͳؔͷू߹
• C
0,σ(Ω; R ) : σ ∈ (0, 1] ʹରͯ͠ɼ H¨older ࿈ଓͳؔͷू߹
(σ = 1 ͷͱ͖ɼ Lipschitz ࿈ଓʹରԠ͢Δ )
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
࠷దઃܭͷղ๏
0 1
a2
a1
a(0)=(0.5,0.5)T
0 1
a(1)
bg0(0)
λ1(1)bg1(0)
λ1(2)bg1(1)
bg0(1)
a=(2/3,1/3)T a(2)
a(3)
0 1 2 3
0.90 0.95 1.00
Cost function f0/f0 init
1+f1
Step number k
(a) ࢼߦͷਪҠ (b) ධՁؔͷཤྺ
ਤ 2.10: Newton ๏ʹΑΔղ
35 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ؔղੳͷجૅ
■ ۭؔؒͷแؚؔ
ఆཧ 3.1 (Sobolev ͷຒଂఆཧ )
k ∈ { 1, 2, · · · } , p ∈ [1, ∞ ) ʹରͯ͠ɼ k + 1 − d/p ≥ k − d/q ͳΒ
W
k+1,p(Ω; R ) ⊂ W
k,q(Ω; R )
͕Γཱͭɽ͞Βʹɼ 0 < σ = k − d/p < 1 ͳΒɼ W
k,p(Ω; R ) ⊂ C
0,σ(Ω; R )
ͱͳΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ؔղੳͷجૅ
x f
x f
(a) σ = 0.5 (b) σ = 1 (Lipschitz ࿈ଓ ) ਤ 3.1: H¨ older ࿈ଓͳؔ
37 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ؔղੳͷجૅ
■ ରۭؒ [1, 4.4 અ ]
Banach ۭؒ X ʹରͯ͠ɼ
f (v) =
∫
Ω
uv dx = ⟨ u, v ⟩ ∀ v ∈ X
Λຬͨ͢Α͏ͳ༗քઢܗ൚ؔ f ( · ) = ⟨ u, · ⟩ ͷू߹ (u ͷू߹ ) Λ X
′ͱ͔͍
ͯɼ X ͷରۭؒͱ͍͏ɽ·ͨɼ ⟨· , ·⟩ : X
′× X → R Λ ⟨· , ·⟩
X′×Xͱ͔͍ͯɼ
ରੵͱ͍͏ɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ؔղੳͷجૅ
ఆཧ 3.2 (H¨ older ͷෆࣜ )
d ∈ N ʹରͯ͠ɼ Ω Λ R
d্ͷՄଌू߹ͱ͠ɼ p, q ∈ (1, ∞ ) 1
p + 1 q = 1
Λຬͨ͢ͱ͢Δɽ͜ͷͱ͖ɼ f ∈ L
p(Ω; R ) ͱ g ∈ L
q(Ω; R ) ʹରͯ͠
∥ f g ∥
L1(Ω;R)≤ ∥ f ∥
Lp(Ω;R)∥ g ∥
Lq(Ω;R)͕Γཱͭɽ
39 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ؔղੳͷجૅ
ࣜ (3.1) ɼ
f (x + y
1) = f (x) + f
′(x) [y
1] + o ( ∥ y
1∥
X) ͱ͔͚Δɽ͜͜Ͱɼ o ( ∥ y
1∥
X)
∥y1
lim
∥X→0o ( ∥ y
1∥
X)
∥ y
1∥
X= 0
YͷΑ͏ʹఆٛ͞ΕΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ؔղੳͷجૅ
ఆٛ 3.3 (k ֊ͷ Fr´ echet ඍ )
X ͱ Y Λ R ্ͷ Banach ۭؒͱ͢Δɽ x ∈ X ͷۙ B ⊂ X ্Ͱ f : B → Y
͕ఆٛ͞Ε͍ͯΔͱ͢ΔɽҙͷมಈϕΫτϧ y
1∈ X ʹରͯ͠ɼ
∥y1
lim
∥X→0∥ f (x + y
1) − f (x) − f
′(x) [y
1] ∥
Y∥ y
1∥
X= 0 (3.1)
Λຬͨ͢༗քઢܗ࡞༻ૉ f
′(x) [ · ] ∈ L (X; Y ) ͕ଘࡏ͢Δͱ͖ɼ f
′(x) [y
1] Λ f
ͷ x ʹ͓͚Δ Fr´echet ඍͱ͍͏ɽ͞Βʹɼҙͷ y
2∈ X ʹରͯ͠ɼ
∥y2∥
lim
X→0X∥ f
′(x + y
2) [y
1] − f
′(x) [y
1] − f
′′(x) [y
1, y
2] ∥
Y∥ y
2∥
X= 0
Λຬͨ͢ f
′′(x) [y
1, · ] ∈ L (X; L (X ; Y )) ͕ଘࡏ͢Δͱ͖ɼ f
′′(x) [y
1, y
2] Λ f ͷ x ʹ͓͚Δ 2 ֊ͷ Fr´echet ඍͱ͍͏ɽ L (X ; L (X; Y )) Λ L
2(X × X; Y ) ͱ
͔͘ɽ k ∈ { 3, 4, . . . } ֊ͷ Fr´echet ඍ f
(k)ಉ༷ʹఆٛ͞ΕΔɽ
41 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ภඍํఔࣜͷڥք
U = {
u ∈ H
1(
Ω; R
d) �� u = 0
Rdon Γ
D} , U (u
D) = {
u ∈ H
1(
Ω; R
d) �� u = u
Don Γ
D} , a(u, v) =
∫
Ω
S (u) · E (v) dx, l (v) =
∫
Ω
b · v dx +
∫
ΓN
p
N· v dγ.
4.2 ( ઢܗੑͷऑܗࣜ )
b ∈ L
2( Ω; R
d)
, p
N∈ L
2(
Γ
N; R
d)
, C ∈ L
∞(
Ω; R
d×d×d×d)
, u
D∈ H
1( Ω; R
d) ͷͱ͖ɼ
a (u, v) = l (v) ∀ v ∈ U Λຬͨ͢ u ∈ U (u
D) ΛٻΊΑɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ภඍํఔࣜͷڥք
§ 4 ภඍํఔࣜͷڥք
■ ઢܗੑ [1, 5.4 અ ]
Ω ⊂ R
dͷڥք ∂Ω Lipchitz ࿈ଓͱ͢ΔɽͻͣΈͱԠྗΛ࣍ͷΑ͏ʹ͔͘ɽ
E (u) = 1 2
{ ∇ u
T+ (
∇ u
T)
T}
, S (u) = CE (u)
Γ
DΓ
pp
Nb u
DΩ
ਤ 4.1: ઢܗੑ
4.1 ( ઢܗੑ )
ମੵྗ b : Ω → R
d, ڥքྗ p
N: Γ
N→ R
d, طมҐ u
D: Ω → R
dʹରͯ͠ɼ
− ∇
TS (u) = b
Tin Ω, S (u) ν = p
Non Γ
N, u = u
Don Γ
DΛຬͨ͢มҐ u : Ω → R
dΛٻΊΑɽ
43 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ภඍํఔࣜͷڥք
■ ղͷਖ਼ଇੑ [1, 5.3 અ ]
4.1 ʹ͓͍ͯɼ֯ͱ Dirichlet ڥքͱ Neumann ڥքͷڥք Γ ¯
N∩ Γ ¯
Dͷ
ۙΛ B ͱ͔͘͜ͱʹ͢Δɽ b ∈ L
2(
Ω; R
d)
ͳΒɼ u ∈ H
2(
Ω \ B; ¯ R )
ΛಘΔɽ
α
Γ
1Γ
2x
0∈ Θ
B(x
0,r
0) θ Ω
ਤ 4.2: ֯Λͭ 2 ࣍ݩྖҬ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ภඍํఔࣜͷڥք
■ ପԁܕภඍํఔࣜͷऑղͷҰҙଘࡏ [1, 5.2 અ ] ఆཧ 4.3 (Lax-Milgram ͷఆཧ )
U Λ࣮ Hilbert ۭؒͱ͢Δɽ a ڧѹత͔ͭ༗քͱ͢Δɽ·ͨɼ l ∈ U
′ͱ͢Δɽ
͜ͷͱ͖ɼ 4.2 ͷղ u ∈ U Ұҙʹଘࡏ͢Δɽ
ྫ 4.4 ( ઢܗੑͷղͷҰҙଘࡏ )
4.2 ʹ͓͍ͯɼ | Γ
D| > 0 ͷͱ͖ɼղ u ∈ U (u
D) Ұҙʹଘࡏ͢Δ͜ͱΛ
ࣔͤɽ
( ղ ) ࣍ͷ͓͖͔͑ʹΑΓɼ Lax-Milgram ͷఆཧͷԾఆ͕Γཱͭ͜ͱ͕͔֬ΊΒΕΔɽ a ( ˜ u, v) = l (v) − a (u
D, v) ˆ l (v)
□
45 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ภඍํఔࣜͷڥք
ఆཧ 4.6 ( ֯ۙʹ͓͚Δղͷਖ਼ଇੑ )
ݫີղ u x
0ͷۙͰ
1
Γ
1ͱ Γ
2͕ಉҰछڥքͳΒɼ α < π ͷͱ͖ɼ
2
Γ
1ͱ Γ
2͕ࠞ߹ڥքͳΒɼ α < π/2 ͷͱ͖ɼ W
1,∞(
B (x
0, r
0) ∩ Ω; R
2)
ʹೖΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ภඍํఔࣜͷڥք
B(x0,r0) Ω
ΓN
ΓD
B(x0,r0) Ω
(a) ಉҰछڥքͰ։͖͕֯ α > π (b) ࠞ߹ڥքͰ։͖͕֯ α > π/2 ਤ 4.3: ಛҟੑ͕ݱΕΔ֯Λͭ 2 ࣍ݩྖҬ
ఆཧ 4.5 ( ֯ۙʹ͓͚Δղͷਖ਼ଇੑ [1, ఆཧ 5.3.2])
ݫີղ u x
0ͷۙͰ u ∈ H
s(
B (x
0, r
0) ∩ Ω; R
2)
ʹೖΔɽͨͩ͠ɼ
1
Γ
1ͱ Γ
2͕ಉҰछڥքͳΒɼ α ∈ [π, 2π) ͷͱ͖ s ∈ (3/2, 2]
2
Γ
1ͱ Γ
2͕ࠞ߹ڥքͳΒɼ α ∈ [π/2, π) ͷͱ͖ s ∈ (3/2, 2] ɼ͓Αͼ α ∈ [π, 2π) ͷͱ͖ s ∈ (5/4, 3/2] ͱͳΔɽ
47 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
■ ઢܗۭؒͱڐ༰ू߹ [1, 8.1 અ ]
ઃܭมΛ θ ∈ D ⊂ X ͱ͓͘ɽͨͩ͠ɼઢܗۭؒ X ͱڐ༰ू߹ D Λ X = H
1(D; R ) ,
D = X ∩ W
1,∞(D; R ) ͱ͓͘ɽີΛ
ϕ (θ) = 1
2 tanh θ + 1 2
ͱ͓͘ɽ͞Βʹɼঢ়ଶม ( ঢ়ଶܾఆͷղ ) u ͷઢܗۭؒͱڐ༰ू߹Λ U = {
u ∈ H
1(
D; R
d) �� u = 0
Rdon Γ
D} , U (u
D) = {
u ∈ H
1(
D; R
d) �� u = u
Don Γ
D} , S = U ∩ W
1,2qR(
D; R
d)
, S (u
D) = U (u
D) ∩ W
1,2qR(
D; R
d) ͱ͓͘ɽͨͩ͠ɼ q
R> d ͱ͢Δɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
§ 5 ઢܗੑମͷີܕҐ૬࠷దԽ [1, ୈ 8 ষ ]
φ(θ) D
ΓD
Γp
pN
b uD
1
00 φ
�
C�
φα
�
C�
0 2 4 6
−2
−6 −4 1.0
0.5
θ φ
(a) ઢܗੑମ (b) ີ ϕ ͱ߶ੑ ϕ
α∥ C ∥ (c) ີ (tanh θ + 1) /2 ਤ 5.1: SIMP (solid isotropic material with penalization) Ϟσϧͱઃܭม θ : D → R
49 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
■ ධՁؔ
ฏۉίϯϓϥΠΞϯεͱྖҬͷେ͖͞ʹର͢Δ੍ؔΛ࣍ͷΑ͏ʹ͓͘ɽ
f
0(θ, u) =
∫
D
b (θ) · u dx +
∫
ΓN
p
N· u dγ −
∫
ΓD
u
D· (ϕ
α(θ) S (u) ν) dγ, f
1(θ) =
∫
D
ϕ (θ) dx − c
1.
5.2 ( ฏۉίϯϓϥΠΞϯε࠷খԽ )
f
0ͱ f
1ʹରͯ͠ɼ
(θ,u−uD
min
)∈D×S(uD){ f
0(θ, u) | f
1(θ) ≤ 0, 5.1 } Λຬͨ͢ θ ΛٻΊΑɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
■ ঢ়ଶܾఆ ( ੍ࣜ )[1, 8.8 અ ]
5.1 (θ ܕઢܗੑ )
α > 1 Λఆͱ͢Δɽ θ ∈ D , b (θ), p
Nʹରͯ͠ɼ
− ∇
T(ϕ
α(θ) S (u)) = b
T(θ) in D, ϕ
α(θ) S (u) ν = p
Non Γ
N,
u = u
Don Γ
DΛຬͨ͢ u ∈ S (u
D) ΛٻΊΑɽ
51 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
L
0ͷ Fr´echet ඍʹରͯ͠ɼ͕࣍Γཱͭɽ
L
0′(θ, u, v
0) [ϑ, u, ˆ v ˆ
0]
= L
0θ(θ, u, v
0) [ϑ]
+ L
0u(θ, u, v
0) [ ˆ u] (= 0 ⇐ L
0(θ, v
0, u) = 0 ˆ ∀ u ˆ ∈ U ) + L
0v0(θ, u, v
0) [ˆ v
0] (= 0 ⇐ L
0(θ, u, v ˆ
0) = 0 ∀ v ˆ
0∈ U )
=
∫
D
{ b
′· (u + v
0) − αϕ
α−1ϕ
′S (u) · E (v
0) } ϑ dx
= ⟨ g
0, ϑ ⟩ ∀ (ϑ, u, ˆ v ˆ
0) ∈ X × U × U Ұํɼ f
1(θ) ʹؔͯ͠ɼ͕࣍Γཱͭɽ
f
1′(θ) [ϑ] =
∫
D
ϕ
′ϑ dx = ⟨ g
1, ϑ ⟩ ∀ ϑ ∈ X
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
■ ධՁؔͷ θ ඍ [1, 8.8 અ ]
f
0(θ, u) ͷ Lagrange ؔΛ
L
0(θ, u, v
0) = f
0(θ, u) + L
S(θ, u, v
0)
ͱ͓͘ɽͨͩ͠ɼ L
S 5.1 ͷ Lagrange ؔͰ࣍ͷΑ͏ʹ͓͘ɽ L
S(θ, u, v
0)
=
∫
D
{− ϕ
α(θ) S (u) · E (v
0) + b (θ) · u } dx +
∫
ΓN
p
N· u dγ +
∫
ΓD
{ (u − u
D) · (ϕ
α(θ) S (v
0) ν) + v
0· (ϕ
α(θ) S (u) ν) } dγ
53 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
ࣜ (5.1) ӈลͷ֤߲ɼ
L
0θθ(θ, u, v
0) [ϑ
1, ϑ
2] =
∫
D
− (ϕ
α(θ))
′′S (u) · E (v
0) ϑ
1ϑ
2dx, (5.2) L
0θu(θ, u, v
0) [ϑ
1, υ ˆ
2] =
∫
D
− (ϕ
α(θ))
′S ( ˆ υ
2) · E (v
0) ϑ
1dx, (5.3) L
0θu(θ, u, v
0) [ϑ
2, υ ˆ
1] =
∫
D
− (ϕ
α(θ))
′S ( ˆ υ
1) · E (v
0) ϑ
2dx, (5.4)
L
0uu(θ, u, v
0) [ ˆ υ
1, υ ˆ
2] = 0 (5.5)
ͱͳΔɽͨͩ͠ɼ u − u
D, v
0− u
D, υ ˆ
1͓Αͼ υ ˆ
2 Γ
D্Ͱ 0
RdͱͳΔ͜ͱΛ
༻͍ͨɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
■ ධՁؔͷ θ Hesse ܗࣜ
b θ ͷؔͰͳ͍ͱԾఆ͢Δɽ (θ, u) ΛઃܭมͱΈͳ͠ɼͦͷڐ༰ू߹
ͱڐ༰ํू߹Λ
S = { (θ, u) ∈ D × S | L
S(θ, u, v) = 0 for all v ∈ U } ,
T
S(θ, u) = { (ϑ, υ) ˆ ∈ X × U | L
Sθu(θ, u, v) [ϑ, υ] = 0 ˆ for all v ∈ U } ͱ͓͘ɽ͜ͷͱ͖ɼ L
0ͷઃܭม (θ, u) ʹର͢Δ 2 ֊ Fr´echet ภඍ
L
0(θ,u)(θ,u)(θ, u, v
0) [(ϑ
1, υ ˆ
1) , (ϑ
2, υ ˆ
2)]
= L
0θθ(θ, u, v
0) [ϑ
1, ϑ
2] + L
0θu(θ, u, v
0) [ϑ
1, υ ˆ
2] + L
0θu(θ, u, v
0) [ϑ
2, υ ˆ
1] + L
0uu(θ, u, v
0) [ ˆ υ
1, υ ˆ
2]
∀ (ϑ
1, υ ˆ
1) , (ϑ
2, υ ˆ
2) ∈ T
S(θ, u) (5.1) ͱͳΔɽ
55 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
f
0ͷ 2 ֊ θ ඍɼࣜ (5.8) ͱࣜ (5.2) Λࣜ (5.1) ʹೖ͢Δ͜ͱʹΑΓɼ
h
0(θ, u, v
0) [ϑ
1, ϑ
2] =
∫
D
{
2 (ϕ
α(θ))
′2ϕ
α(θ) − (ϕ
α(θ))
′′}
S (u) · E (v
0) ϑ
1ϑ
2dx
=
∫
D
β (α, θ) S (u) · E (v
0) ϑ
1ϑ
2dx ͱͳΔɽͨͩ͠ɼ β (α, θ)
β (α, θ) = α (α + 1) ( 1
2 tanh θ + 1 2
)
α−2( sech
2θ
2 )
2− α ( 1
2 tanh θ + 1 2
)
α−1( − sech
2θ tanh θ )
ͱͳΔɽਤ 5.2 (a) ΑΓɼ β (α, θ) > 0 ͕֬ೝ͞ΕΔɽ͞ΒʹɼࣗݾਵؔΛ༻
͍Εɼ S (u) · E (v
0) > 0 ͱͳΓɼ h
0(θ, u, v
0) [ · , · ] X ্ͷڧѹత͔ͭ༗ք ͳ͋Δ 1 ࣍ܗࣜͱͳΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
Ұํɼ j ∈ { 1, 2 } ʹରͯ͠ɼ L
Sθu(θ, u, v) [ϑ
j, υ ˆ
j]
=
∫
D
{ − (ϕ
α(θ))
′ϑ
jS (υ) − ϕ
α(θ) S ( ˆ υ
j) }
· E (v) dx
= 0 ∀ (ϑ
j, υ ˆ
j) ∈ T
S(θ, u) (5.6)
ͱͳΔɽͨͩ͠ɼ v
0ͱ υ ˆ
jͷ Dirichlet ڥք͕݅ΘΕͨɽࣜ (5.6) ΑΓɼ
S ( ˆ υ
j) = − (ϕ
α(θ))
′ϕ
α(θ) ϑ
jS (u) in D (5.7)
ΛಘΔɽͦ͜Ͱɼࣜ (5.7) ͷ υ ˆ
jΛࣜ (5.4) ͷ υ ˆ
1ͱࣜ (5.3) ͷ υ ˆ
2ʹೖ͢Ε
ɼ࣍ΛಘΔɽ
L
0θu(θ, u, v
0) [ϑ
1, υ ˆ
2] = L
0θu(θ, u, v
0) [ϑ
2, υ ˆ
1]
=
∫
D
(ϕ
α(θ))
′2ϕ
α(θ) S (u) · E (v
0) ϑ
1ϑ
2dx (5.8)
57 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
■ H 1 ޯ๏ͱ H 1 Newton ๏ [1, 8.6 અ ]
5.3 (θ ܕ H 1 ޯ๏ )
X ্ͷ༗ք͔ͭڧѹతͳ 1 ࣍ܗࣜ a
X: X × X → R ͱ g
i(θ
k) ∈ X
′͕༩͑Β Εͨͱ͖ɼ
a
X(ϑ
gi, ψ) = − ⟨ g
i(θ
k) , ψ ⟩ ∀ ψ ∈ X Λຬͨ͢ ϑ
gi∈ X ΛٻΊΑɽ
ྫ͑ɼ
a
X(ϑ, ψ) =
∫
D
( ∇ ϑ · ∇ ψ + c
Dϑψ) dx ͱ͓͘ɽΞϧΰϦζϜɼਤ 2.6 ͕ΘΕΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
Ұํɼ f
1(θ) ͷ 2 ֊ θ ඍɼ h
1(θ) [ϑ
1, ϑ
2] =
∫
D
ϕ
′′(θ) ϑ
1ϑ
2dx =
∫
D
− sech
2θ tanh θϑ
1ϑ
2dx ͱͳΔɽਤ 5.2 (b) ΑΓɼ h
1(θ) [ · , · ] ڧѹతʹͳΒͳ͍ɽ
2
1
0 1 2 3
θ
−1
−3 −2
α=3 β
α=2
−0.2
−0.4 0
θ
1 2 3
−1
−3 −2
φ
��0.4 0.2
(a) β (α, θ) (b) ϕ
′′(θ)
ਤ 5.2: ධՁؔͷ 2 ֊ θ ඍʹ͓͚Δؔ
59 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
ఆཧ 5.5 (θ ܕ H 1 ޯ๏ [1, ఆཧ 8.4.2, ఆཧ 8.5.5])
θ ∈ D ʹରͯ͠ɼ 5.1 ͷղ u ͕ S (u
D) ʹೖΔͱ͖ɼ i ∈ { 0, 1 } ʹରͯ͠ɼ g
i∈ L
qR(D; R ) ͱͳΔɽ͞Βʹɼ 5.4 ͷऑղ ϑ
giҰҙʹଘࡏ͠ɼͦͷղ ϑ
gi D \ B ¯ ্Ͱɼ W
1,∞ڃͱͳΔɽ·ͨɼ ϑ
gi f ˜
i(θ) ͷ߱ԼํΛ͍ͯ
͍Δɽ
( ূ໌ ) H¨older ͷෆࣜͳͲʹΑΓɼ g
i∈ L
qR(D; R ) ⊂ X
′ΛಘΔɽ͞Βʹɼ Lax-Milgram ͷఆཧΑΓɼ ϑ
giҰҙʹଘࡏ͠ɼ ϑ
gi D \ B ¯ ্Ͱ W
2,qRڃΛಘ Δɽ͞Βʹɼ Sobolev ͷຒଂఆཧΑΓɼ
2 − d q
R= 1 + σ > 1 (σ ∈ (0, 1)) ⇒ W
2,qR(
D \ B, ¯ R )
⊂ W
1,∞(
D \ B, ¯ R )
͕Γཱͭɽ·ͨɼ͕࣍Γཱͭɽ
f ˜
i(θ + ¯ ϵϑ
gi) − f ˜
i(θ) = ¯ ϵ ⟨ g
i, ϑ
gi⟩ + o ( | ¯ ϵ | )
= − ¯ ϵa
X(ϑ
gi, ϑ
gi) + o ( | ¯ ϵ | ) ≤ − ϵα ¯
X∥ ϑ
gi∥
2X+ o ( | ¯ ϵ | )
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
5.4 (H 1 ੵΛ༻͍ͨ θ ܕ H 1 ޯ๏ )
θ ∈ D ʹରͯ͠ g
i∈ X
′͕༩͑ΒΕͨͱ͖ɼ࣍Λຬͨ͢ ϑ
gi∈ X ΛٻΊΑɽ
− ∆ϑ
gi+ c
Dϑ
gi= − g
iin D,
∂
νϑ
gi= 0 on ∂D.
φ
α(θ) D
−
g
ic
Dਤ 5.3: H
1ۭؒͷੵΛ༻͍ͨ H
1ޯ๏
61 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
■ ྫ
¡D0 ¡p0
pN
0 200 400 600
評価関数
f0/f0 init
1+f1/c1
1.0
0 0.2 0.4 0.6 0.8 1.2
H1勾配法 H1 Newton 法
ステップ数 k
(a) ॳظີͱڥք݅ (b) ධՁؔͷཤྺ
(c) H
1ޯ๏ʹΑΔ࠷దີ (d) H
1Newton ๏ʹΑΔ࠷దີ
ਤ 5.4: 2 ࣍ݩઢܗੑମͷີܕҐ૬࠷దԽʹର͢Δྫ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷີܕҐ૬࠷దԽ
5.6 (θ ܕ H 1 Newton ๏ )
ࢼߦ θ
k∈ X ʹ͓͍ͯɼ λ
k∈ R
|IA| KKT ݅Λຬͨ͢ͱ͢Δɽ·ͨɼ h
L(θ
k) [ϑ
1, ϑ
2] = h
0(θ
k) [ϑ
1, ϑ
2] + ∑
i∈IA(θk)
λ
ikh
i(θ
k) [ϑ
1, ϑ
2] ∀ ϑ
1, ϑ
2∈ X ͱ͓͘ɽ a
X: X × X → R Λ X ্ͷ༗ք͔ͭڧѹతͳ 1 ࣍ܗࣜͱ͢Δͱ͖ɼ
c
hh
L(θ
k) [ϑ
gi, ψ] + c
aa
X(ϑ
gi, ψ) = − ⟨ g
i(θ
k) , ψ ⟩ ∀ ψ ∈ X Λຬͨ͢ φ
gi∈ X ΛٻΊΑɽ
ਤ 2.7 ͷΞϧΰϦζϜ͕ΘΕΔɽ
63 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
■ ঢ়ଶܾఆ ( ੍ࣜ )[1, 9.11 અ ]
6.1 ( ઢܗੑ )
ϕ ∈ D , b (ϕ), p
N(ϕ), u
D(ϕ) ͓Αͼ C (ϕ) ʹରͯ͠ɼ
− ∇
TS (ϕ, u) = b
T(ϕ) in Ω (ϕ) , S (ϕ, u) ν = p
N(ϕ) on Γ
p(ϕ) , S (ϕ, u) ν = 0
Rdon Γ
N(ϕ) \ Γ ¯
p(ϕ) , u = u
D(ϕ) on Γ
D(ϕ)
Λຬͨ͢ u ∈ S (u
D) ΛٻΊΑɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
§ 6 ઢܗੑମͷܗঢ়࠷దԽ [1, ୈ 9 ষ ]
■ ઢܗۭؒͱڐ༰ू߹ [1, 9.1 અ ]
ઃܭมΛ ϕ ∈ D ⊂ X ͱ͓͘ɽͨͩ͠ɼઢܗۭؒ X ͱڐ༰ू߹ D Λ X = {
ϕ ∈ H
1(
R
d; R
d) �� ϕ = 0
Rdon Ω ¯
C0} , D = {
ϕ ∈ X ∩ W
1,∞(
R
d; R
d) �� શ୯ࣹͷ݅ } .
ͱ͓͘ɽͨͩ͠ɼ Ω ¯
C0⊂ Ω ¯
0ઃܭ্ͷݻఆྖҬ͋Δ͍ڥքͱ͢Δɽ ঢ়ଶม ( ঢ়ଶܾఆͷղ ) u ͷઢܗۭؒͱڐ༰ू߹Λ
U = {
u ∈ H
1(
R
d; R
d) �� u = 0
Rdon Γ
D(ϕ) } , U (u
D) = {
u ∈ H
1(
R
d; R
d) �� u = u
Don Γ
D(ϕ) } , S = U ∩ W
1,∞(
R
d; R
d) , S (u
D) = U (u
D) ∩ W
1,∞(
R
d; R
d) ͱ͓͘ɽ
65 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
■ ධՁؔͷܗঢ়ඍ [1, 9.11 અ ]
f
0(ϕ, u) ͷ Lagrange ؔΛ
L
0(ϕ, u, v
0) = f
0(ϕ, u) + L
S(ϕ, u, v
0)
ͱ͓͘ɽͨͩ͠ɼ L
S 6.1 ͷ Lagrange ؔͰ࣍ͷΑ͏ʹ͓͘ɽ
L
S(ϕ, u, v) =
∫
Ω(ϕ)
( − S (u) · E (v) + b · v) dx +
∫
Γp(ϕ)
p
N· v dγ +
∫
ΓD(ϕ)
{ (u − u
D) · (S (v) ν) + v · (S (u) ν) } dγ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
■ ධՁؔ [1, 9.11 અ ]
ฏۉίϯϓϥΠΞϯεͱྖҬͷେ͖͞ʹର͢Δ੍ؔΛ࣍ͷΑ͏ʹ͓͘ɽ
f
0(ϕ, u) =
∫
Ω(ϕ)
b · u dx +
∫
ΓN(ϕ)
p
N· u dγ −
∫
ΓD(ϕ)
u
D· (S (u) ν) dγ,
f
1(ϕ) =
∫
Ω(ϕ)
dx − c
1.
6.2 ( ฏۉίϯϓϥΠΞϯε࠷খԽ )
f
0ͱ f
1ʹରͯ͠ɼ
(ϕ,u−
min
uD)∈D×S{ f
0(ϕ, u) | f
1(ϕ) ≤ 0, 6.1 } Λຬͨ͢ Ω (ϕ) ΛٻΊΑɽ
67 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
͕Γཱͭɽͨͩ͠ɼ G
Ω0= 2S (u) (
∇ u
T)
T, g
Ω0= − S (u) · E (u) + 2b · u, g
p0= 2κ (p
N· u) ν,
g
∂p0= 2 (p
N· u) τ Ͱ͋Δɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
b (ϕ), p
N(ϕ), u
D(ϕ) ͓Αͼ C (ϕ) ࣭ݻఆͰ͋ΔͱԾఆ͢Δɽ͜ͷͱ͖ɼ L
0′(ϕ, u, v
0) [φ, u, ˆ v ˆ
0]
= L
0ϕ′(ϕ, u, v
0) [φ]
+ L
0u(ϕ, u, v
0) [ ˆ u] (= 0 ⇐ L
0(ϕ, v
0, u) = 0 ˆ ∀ u ˆ ∈ U ) + L
0v0(ϕ, u, v
0) [ˆ v
0] (= 0 ⇐ L
0(ϕ, u, v ˆ
0) = 0 ∀ v ˆ
0∈ U )
= ⟨ g
0, φ ⟩ ( ⇐ [1, ໋ 9.3.4 ͱ໋ 9.3.7] )
=
∫
Ω(ϕ)
( G
Ω0· ∇ φ
T+ g
Ω0∇ · φ ) dx
+
∫
Γp(ϕ)
g
p0· φ dγ +
∫
∂Γp(ϕ)∪Θ(ϕ)
g
∂p0· φ dς
∀ (φ, u, ˆ v ˆ
0) ∈ Ξ × U × U
69 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
Ұํɼ f
1(ϕ) ͷܗঢ়ඍɼ f
1′(ϕ) [φ] = ⟨ g
1, φ ⟩ =
∫
Ω(ϕ)
∇ · φ dx ͱͳΔɽ͋Δ͍ɼ
f
1′(ϕ) [φ] = ⟨ g ¯
1, φ ⟩ =
∫
∂Ω(ϕ)
ν · φ dγ ͱͳΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
͋Δ͍ɼ b, p
N, u
D͓Αͼ C ۭؒݻఆͷؔͰ͋ΔͱԾఆͯ͠ɼ u ͱ v
0 q
R> d ʹରͯ͠ W
2,2qR(
R
d; R
d)
ͱԾఆͱ͖ɼ L
0ϕ∗(ϕ, u, v
0) [φ]
= ⟨ g ¯
0, φ ⟩ ( ⇐ [1, ໋ 9.3.9 ͱ໋ 9.3.12] )
=
∫
∂Ω(ϕ)
g ¯
∂Ω0· φ dγ +
∫
Γp(ϕ)
g ¯
p0· φ dγ +
∫
∂Γp(ϕ)∪Θ(ϕ)
g ¯
∂p0· φ dς
+
∫
ΓD(ϕ)
g ¯
D0· φ dγ
ͷΑ͏ʹ͔͔ΕΔɽ͜͜Ͱɼ
¯
g
∂Ω0= ( − S (u) · E (u) + 2b · u) ν,
¯
g
p0= 2 (∂
ν+ κ) (p
N· u) ν, g ¯
∂p0= 2 (p
N· u) τ ,
¯
g
D0= 2 { ∂
ν(u − u
D) · (S (u) ν) } ν .
71 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
ࣜ (6.1) ͷӈลୈ 2 ߲ɼ L
0ϕ′u(ϕ, u, v
0) [φ
1, υ ˆ
2]
=
∫
Ω(ϕ)
[{ S ( ˆ υ
2) (
∇ v
T0)
T+ S (v
0) (
∇ υ ˆ
2T)
T}
· ∇ φ
T1− (S( ˆ υ
2) · E (v
0)) ∇ · φ
1]
dx (6.2)
ͱͳΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
■ ධՁؔͷܗঢ় Hesse ܗࣜ [1, 9.11 અ ]
b = 0
RdΛԾఆ͢Δɽઃܭม (ϕ, u) Λ (ϕ, u) ͷڐ༰ू߹ͱڐ༰ํू߹Λ S = { (ϕ, u) ∈ D × S | L
S(ϕ, u, v) = 0 for all v ∈ U } ,
T
S(ϕ, u) = { (φ, υ) ˆ ∈ X × U | L
Sϕu(ϕ, u, v) [φ, υ] = 0 ˆ for all v ∈ U } ͱ͓͘ɽ͜ͷͱ͖ɼ L
0ͷ (ϕ, u) ʹର͢Δ 2 ֊ Fr´echet ภඍɼ
L
0(ϕ′,u)(ϕ′,u)(ϕ, u, v
0) [(φ
1, υ ˆ
1) , (φ
2, υ ˆ
2)]
= (L
0ϕ′(ϕ, u, v
0) [φ
1] + L
0u(ϕ, u, v
0) [ ˆ υ
1])
ϕ[φ
2] + (L
0ϕ′(ϕ, u, v
0) [φ
1] + L
0u(ϕ, u, v
0) [ ˆ υ
1])
u[ ˆ υ
2]
= L
0ϕ′ϕ′(ϕ, u, v
0) [φ
1, φ
2] + L
0ϕ′u(ϕ, u, v
0) [φ
1, υ ˆ
2] + L
0ϕ′u(ϕ, u, v
0) [φ
2, υ ˆ
1] + L
0uu(ϕ, u, v
0) [ ˆ υ
1, υ ˆ
2]
∀ (φ
1, υ ˆ
1) , (φ
2, υ ˆ
2) ∈ T
S(ϕ, u) (6.1) ͱͳΔɽࣜ (6.1) ͷӈลୈ 1 ߲ͷܭࢉলུ͢Δɽ
73 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
ҙͷ v ∈ U ʹରͯࣜ͠ (6.3) ͕Γཱͭ͜ͱ͔Βɼ S ( ˆ υ
j) (
∇ v
T)
T= {(
∇ φ
Tj)
TS (u) + C (
∇ φ
Tj∇ u
T)
s− ∇ · φ
jS (u) } (
∇ v
T)
T(6.4)
͕ಘΒΕΔɽ·ͨɼࣜ (6.3) L
Sϕ′u(ϕ, u, v) [φ
j, υ ˆ
j]
=
∫
Ω(ϕ)
[ ∇ v
TS (u) ∇ φ
Tj+ S (v) {(
∇ u
T)
T((
∇ φ
Tj)
T− ∇ · φ
j) − (
∇ υ ˆ
jT)
T}]
· I dx
= 0 ͱ͔͚Δɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
Ұํɼ j ∈ { 1, 2 } ʹରͯ͠ɼ L
Sϕ′u(ϕ, u, v) [φ
j, υ ˆ
j]
=
∫
Ω(ϕ)
{ S (u) · (
∇ φ
Tj∇ v
T)
s+ S (v) · (
∇ φ
Tj∇ u
T)
s− (S (u) · E (v)) ∇ · φ
j− S ( ˆ υ
j) · E (v) } dx
=
∫
Ω(ϕ)
[{( ∇ φ
Tj)
TS (u) + C (
∇ φ
Tj∇ u
T)
s− S (u) ∇ · φ
j− S ( ˆ υ
j) } (
∇ v
T)
T]
· I dx
= 0 ∀ (φ
j, υ ˆ
j) ∈ T
S(ϕ, u) (6.3)
ͱͳΔɽͨͩ͠ɼ v ͱ υ ˆ
jͷ Dirichlet ڥք͕݅ΘΕͨɽ
75 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
Ҏ্ͷ݁ՌʹՃ͑ͯɼࣗݾਵؔͱ
h
0(ϕ, u, v
0) [φ
1, φ
2] = h
0(ϕ, u, v
0) [φ
2, φ
1]
͕Γཱͭ͜ͱΛ༻͍Εɼ f
0ͷܗঢ় Hesse ܗࣜ࣍ͷΑ͏ʹಘΒΕΔɽ h
0(ϕ, u, u) [φ
1, φ
2]
=
∫
Ω(ϕ)
[ S (u) · E (u) {(
∇ φ
T2)
T· ∇ φ
T1+ ( ∇ · φ
2) ( ∇ · φ
1) } + (
∇ u
TS (u) )
· {
∇ φ
T1(
∇ φ
T2)
T+ ∇ φ
T2(
∇ φ
T1)
T}
− 2 (S (u) E (u)) · {
∇ φ
T2( ∇ · φ
1) + ∇ φ
T1( ∇ · φ
2) }]
dx
∀ φ
1, φ
2∈ X
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
ͦ͜Ͱɼ S (v) (
∇ υ ˆ
Tj)
T= ∇ v
TS (u) ∇ φ
Tj+ S (v) (
∇ u
T)
T{(
∇ φ
Tj)
T− ∇ · φ
j}
(6.5) ΛಘΔɽࣜ (6.2) ʹࣜ (6.4) ͱࣜ (6.5) Λೖ͢Εɼࣜ (6.1) ͷӈลୈ 2 ߲͕
ܭࢉ͞ΕΔɽಉ༷ʹɼࣜ (6.1) ͷӈลୈ 3 ߲ɼӈลୈ 2 ߲ͷ݁Ռʹ͓͍ͯ φ
1ͱ φ
2Λ͍Ε͔͑ͨͷͱͳΔɽࣜ (6.1) ͷӈลୈ 4 ߲ 0 ͱͳΔɽ
77 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
■ H 1 ޯ๏ͱ H 1 Newton ๏ [1, 9.8 અ ]
6.3 ( ྖҬมಈܕ H 1 ޯ๏ )
X ্ͷ༗ք͔ͭڧѹతͳ 1 ࣍ܗࣜ a
X: X × X → R ͱ g
i∈ X
′͕༩͑ΒΕͨ
ͱ͖ɼ
a
X(φ
gi, ψ) = − ⟨ g
i, ψ ⟩ ∀ ψ ∈ X Λຬͨ͢ φ
gi∈ X ΛٻΊΑɽ
ྫ͑ɼ
a
X(φ, ψ) =
∫
Ω(ϕ)
{( ∇ φ
T)
· (
∇ ψ
T)
+ c
Ωφ · ψ } dx ͱ͓͘ɽΞϧΰϦζϜɼਤ 2.6 ͕ΘΕΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
Ұํɼ f
1(ϕ) ͷܗঢ় Hesse ܗࣜ࣍ͷΑ͏ʹͳΔɽ h
1(ϕ) [φ
1, φ
2]
=
∫
Ω(ϕ)
{ − (
∇ φ
T2)
T· ∇ φ
T1+ ( ∇ · φ
2) ( ∇ · φ
1) }
dx ∀ φ
1, φ
2∈ X
79 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
6.4 ( ྖҬมಈܕ H 1 Newton ๏ )
ࢼߦ ϕ
k∈ X ʹ͓͍ͯɼ λ
k∈ R
|IA| KKT ݅Λຬͨ͢ͱ͢Δɽ·ͨɼ h
L(ϕ
k) [φ
1, φ
2] = h
0(ϕ
k) [φ
1, φ
2] + ∑
i∈IA(xk)
λ
ikh
i(ϕ
k) [φ
1, φ
2]
∀ φ
1, φ
2∈ X
ͱ͓͘ɽ a
X: X × X → R Λ X ্ͷ༗ք͔ͭڧѹతͳ 1 ࣍ܗࣜͱ͢Δɽ͜ͷ ͱ͖ɼ
c
hh
L(ϕ
k) [φ
gi, ψ] + c
aa
X(φ
gi, ψ) = − ⟨ g
i(ϕ
k) , ψ ⟩ ∀ ψ ∈ X Λຬͨ͢ φ
gi∈ X ΛٻΊΑɽ
ਤ 2.7 ͷΞϧΰϦζϜ͕ΘΕΔɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
ΓD(φ)
Γp(φ) pN(φ)
uD(φ)b(φ)
Ω(φ)
ΓD(φ)
Γp(φ)=Γηi(φ) (φ)
−gpi−gηi
−g∂pi−g∂ηi
−gΩi
cΩ
−GΩi
(Á+') (Á)
x '(x)
ঢ়ଶܾఆ H
1ޯ๏ ܗঢ়ߋ৽
(b, p, u
D) → u g
i→ φ
giΩ (ϕ) → Ω (ϕ + ϵφ
gi) ਵ
(ζ
iu, η
iu) �→ v
iਤ 6.1: H
1ޯ๏ʹΑΔܗঢ়ߋ৽
81 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
0 20 40 60 80 100 120 0.4
0.6 0.8
Cost function
1.0
f
0/f
0 init1+f
1/c
1H
1grad. meth.
H
1Newton meth.
Iteration number k
ਤ 6.3: 2 ࣍ݩઢܗੑମʹର͢Δ݁Ռ : ධՁؔͷཤྺ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ઢܗੑମͷྖҬมಈܕܗঢ়࠷దԽ
■ ྫ
ΓD0
Γp0
ΓD0
pN
(a) ॳظܗঢ় (b) H
1ޯ๏ (c) H
1Newton ๏ ਤ 6.2: 2 ࣍ݩઢܗੑମʹର͢Δ݁Ռ : ܗঢ়ൺֱ
83 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ઃܭม
• L = { 1, 2, · · · , |L|} : ϦϯΫʹ͚ΒΕͨ൪߸ͷू߹
• Ω
0l⊂ R
d: ϦϯΫ l ∈ L ͷ࣌ࠁ t = 0 ͷͱ͖ͷॳظྖҬ
• Ω
0 def= { Ω
0l}
l∈L, ∂Ω
0 def= { ∂Ω
0l}
l∈L• X = {
ϕ ∈ H
1(
R
d; R
d) �� ϕ = 0
Rdon Ω ¯
C0}
• D = {
ϕ ∈ X ∩ W
1,∞(
R
d; R
d) �� શ୯ࣹͷ݅ }
• ϕ
l∈ D ʹରͯ͠ɼ Ω
l(ϕ
l) = { (i + ϕ
l) (x) | x ∈ Ω
0l}
• ϕ
def= { ϕ
l}
i∈L∈ D
|L|, Ω (ϕ)
def= { Ω
l(ϕ
l) }
l∈Lܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
§ 7 ϦϯΫػߏͷܗঢ়࠷దԽ [3]
Ω
03Ω
01b
1Ω
02Ω
04x
J1x
J2x
J3p
N3Γ
p03Ω
2(φ
2)
Ω
1(φ
1)
ਤ 7.1: t = 0 ʹ͓͚ΔϦϯΫ݁߹͞Εͨ߶ମͷྖҬมಈ
85 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
• u
l(q
l, x) = x
Gl(t) − x
Gl(0) + θ
l(t) e
3× (x − x
Gl(0)) : q
l͔Β Ω
l(ϕ
l) ্ ͷҙͷ x ͷมҐ
• Ω ˜
l(ϕ
l, q
l) = { x + u
l(q
l, x) | x ∈ Ω
l(ϕ
l) } : ߶ମӡಈ͢ΔྖҬ
• Γ ˜
pl(q
l) = {
x + u
l(q
l, x) � � x ∈ ∂Ω
0l∩ Γ
p0} : ߶ମӡಈ͢Δඇಉ࣍
Neumann ڥք
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ঢ়ଶม
• x
Gl: (0, t
T) → R
d: Ω
l(ϕ) ͷॏ৺ͷҐஔ
• θ
l: (0, t
T) → R : x
GlपΓͷճస
• q
l(t) = (
(x
Gl(t) − x
Gl(0))
T, θ
l(t) )
T: (0, t
T) → R
dF: Ω
l(ϕ) ͷ߶ମӡಈ (d
F= 3)
• q = (
q
1T, · · · , q
|L|T)
T: (0, t
T) → R
dF|L|: શମܥͷ߶ମӡಈ
Q = {
q ∈ H
1(
(0, t
T) ; R
dF|L|) ��
� �
( q ˙ (0) q (0)
)
= ( 0
0 ) }
, Q
0=
{
q ∈ H
1(
(0, t
T) ; R
dF|L|) ��
� �
( q ˙ (0) q (0) )
= ( q
1q
0) } , Q
T(q) =
{
r ∈ H
1(
(0, t
T) ; R
dF|L|) ��
� �
( r ˙ (t
T) r (t
T)
)
=
( q ˙ (t
T) q (t
T)
) }
87 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ҰൠԽ࣭ྔͱҰൠԽ֎ྗ
ϦϯΫػߏͷҰൠԽ࣭ྔ
M (ϕ) = diag (
m
1(ϕ
1) , m
1(ϕ
1) , j
G1(ϕ
1) , . . . , m
|L|(
ϕ
|L|)
, m
|L|( ϕ
|L|)
, j
G|L|( ϕ
|L|))
ͨͩ͠ɼ
m
l(ϕ
l) =
∫
Ωl(ϕl)
ρ
ldx, j
Gl(ϕ
l) =
∫
Ωl(ϕl)
ρ
l∥ x − x
Gl(0) ∥
2Rddx
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ӡಈ੍
• J = { 1, 2, · · · , |J |} : ϦϯΫ݁߹੍ʹ͚ΒΕͨ൪߸ͷू߹
• i ∈ J ʹରͯ͠ɼ u
l(q
l, x
Jil) − u
m(q
m, x
Jim) = 0
R2: ϦϯΫ݁߹੍
• T = { 1, 2, · · · , |T |} : ฒਐӡಈ੍ʹ͚ΒΕͨ൪߸ͷू߹
• i ∈ T ʹରͯ͠ɼ u
Til(q
l, x
Gl) = (x
Glj(t) − x
Glj(0)) · e
Ti= 0 : ฒਐӡಈ
੍
• R = { 1, 2, · · · , |R|} : ճసӡಈ੍ʹ͚ΒΕͨ൪߸ͷू߹
• i ∈ R ʹରͯ͠ɼ θ
l(t) = 0 : ճసӡಈ੍
• ψ (q) = 0
R|C|( C
def= ( { 1, 2 } × J ) ∪ T ∪ R ) : ͯ͢ͷӡಈ੍
89 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ঢ়ଶܾఆ
7.1 ( ϦϯΫӡಈ )
ϕ ∈ D
|L|༩͑ΒΕͨͱ͢Δɽ·ͨɼ q
0, q
1∈ R
dF|L|͕༩͑ΒΕͨͱͯ͠ɼ ( ψ
′(q
0) [q
1]
ψ (q
0) )
= ( 0
0 )
Λຬͨ͢ͱ͢Δɽ͞Βʹɼ rank ψ
qT(q
0) = |C| ͱ͢Δɽ͜ͷͱ͖ɼ ( M (ϕ) (
ψ
qT(q) )
Tψ
qT(q) 0
) ( q ¨
− µ )
=
( s
− ψ
′′(q) [ ˙ q, q] ˙ )
in (0, t
T) , ( q ˙ (0)
q (0) )
= ( q
1q
0)
Λຬͨ͢ (
q
T, µ
T)
T: (0, t
T) → R
dF|L|+|C|ΛٻΊΑɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
ϦϯΫ l ∈ L ʹ࡞༻͢Δମੵྗ b
l∈ L
2(
(0, t
T) ; L
∞(
R
d; R
d))
ͱඇྵͷڥք
ྗ p
Nl∈ L
2(
(0, t
T) ; L
∞(
Γ
p0l; R
d))
ʹର͢ΔҰൠԽ֎ྗ
s
l= (
s
TFl, s
Ml)
T∈ R
dFͨͩ͠ɼ
s
Fl=
∫
Ωl(ϕl)
b
l(t) dx +
∫
Γp0l
p
Nl(t) dγ,
s
Mle
3=
∫
Ωl(ϕl)
b
l(t) × (x − x
Gl(t)) dx +
∫
Γp0l
p
Nl(t) × (x − x
Gl(t)) dγ
શମܥͷҰൠԽྗ
s = (
s
T1, . . . , s
T|L|)
T91 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
µ
J2(q)
µ
J1(q) x
G1(q)
x
J2(q)
x
J1(q) x
G3(q) µ
R4e
3Ω
03µ
T3e
2(a) ϦϯΫ݁߹ྗ (b) ฒਐ੍ྗͱճస੍Ϟʔϝϯτ ਤ 7.2: ӡಈ੍ʹର͢Δ੍ྗ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
7.1 ʹ͓͍ͯɼ µ ɼӡಈ੍ʹର͢Δ Lagrange Ͱɼӡಈ੍Λຬ
ͨͨ͢Ίʹ࡞༻੍ͨ͠ྗΛද͢ɽͦ͜Ͱɼ µ ͷཁૉΛ
µ = (
µ
TJ1, . . . , µ
TJ|J |, µ
TT1, . . . , µ
TT|T |, µ
TR1, . . . , µ
TR|R|)
T∈ E ͱ͔͘͜ͱʹ͢Δɽ͜͜Ͱɼ࣍ͷΑ͏ʹ͓͘ɽ
E = L
2(
(0, t
T) ; R
|C|)
■ ੍ྗͱ੍Ϟʔϝϯτ
• ϦϯΫ݁߹ྗ : x
Ji∈ Ω
l(ϕ) ʹ͓͍ͯ µ
Ji: (0, t
T) → R
2ɼ x
Ji∈ Ω
m(ϕ) ʹ
͓͍ͯ − µ
Ji(0, t
T) → R
2( ਤ 7.2 (a))
• ฒਐӡಈ੍ʹର͢Δ੍ྗ : x
Gl∈ Ω
l(ϕ) ʹ͓͍ͯ µ
Tie
j( ਤ 7.2 (b))
• ճసӡಈ੍ʹର͢Δ੍Ϟʔϝϯτ : µ
Rie
3on x
Gl∈ Ω
l(ϕ) ( ਤ 7.2 (b))
93 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
7.2 ( ϦϯΫӡಈͷऑܗࣜ )
7.1 ͷԾఆ͕Γཱͭͱ͖ɼ
L
Sr,η(q, µ, r, η) [ˆ r, η] = 0 ˆ ∀ (ˆ r, η) ˆ ∈ Q
T(0) × E Λຬͨ͢ (q, µ) ∈ Q
0× E ΛٻΊΑɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
7.1 ͷ Lagrange ؔɼ (q, µ, r, η) ∈ Q
0× E × Q
T(q) × E ʹରͯ͠
L
S(ϕ, q, µ, r, η)
=
∫
tT0
( − q ¨
TM (ϕ) ˙ r + µ
Tψ
qT(q) ˙ r + ¨ q
T(
ψ
qT(q) )
Tη + ψ
′′(q) [ ˙ q, q] ˙ · η + η
Tψ
qT(q) ˙ q + ¨ r
T(
ψ
qT(q) )
Tµ + ψ
′′(q) [ ˙ r, r] ˙ · µ + s · r ˙ ) dt + 1
2 q ˙
T(t
T) M (ϕ) ˙ q (t
T) (7.1)
ͱ͓͘ɽ·ͨɼ࣍ͷΑ͏ʹ͔͘ɽ L
Sr,η(ϕ, q, µ, r, η) [ˆ r, η] ˆ
=
∫
tT0
( − q ¨
TM (ϕ) ˙ˆ r + µ
Tψ
qT(q) ˙ˆ r + ¨ q
T(
ψ
qT(q) )
Tˆ
η + ψ
′′(q) [ ˙ q, q] ˙ · η ˆ + ˆ η
Tψ
qT(q) ˙ q + ¨ ˆ r
T(
ψ
qT(q) )
Tµ + ψ
′′(q) [
˙ˆ r, r ˙ˆ ]
· µ + s · r ˙ˆ ) dt
∀ (ˆ r, η) ˆ ∈ Q
T(0)
95 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ܗঢ়ඍ
f ˜
0′(ϕ) [φ] = ∑
l∈L
∫
Ωl(ϕl)
g
M0l∇ · φ
ldx = ∑
l∈L
⟨ g
0l, φ
l⟩ = ⟨ g
0, φ ⟩
͋Δ͍ɼ
f ˜
0′(ϕ) [φ] = ∑
l∈L
∫
∂Ωl(ϕl)
g
M0lν · φ
ldγ = ∑
l∈L
⟨ g ¯
0l, φ
l⟩ = ⟨ g ¯
0, φ ⟩
ͨͩ͠ɼ
g
M0l= −
∫
tT 0ρ
lu
l( ¨ q
l) · u
l( ˙ r
0l) dt
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ܗঢ়࠷దԽ
f
0(ϕ, q, µ) = −
∫
tT 0s · q ˙ dt, f
1(ϕ) = c
1− ∑
i∈L
∫
Ωl(ϕl)
dx
7.3 ( ମੵ੍͖ͭ֎ྗࣄ࠷େԽ )
࣍Λຬͨ͢ Ω (ϕ) ΛٻΊΑɽ
(ϕ,q,µ)∈D
min
|L|×Q0×E{ f
0(ϕ, q, µ) | f
1(ϕ) ≤ 0, 7.2 }
97 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
0 100 200
0.5 1.0 1.5 2.0
(1{f
1/c
1)/2 f
0/f
0 initIteration number of reshaping
C ost f u n ct ion
50 150
ਤ 7.4: ܗঢ়मਖ਼ʹର͢ΔධՁؔͷཤྺ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
■ ྫ
֎ྗ p
N3= ( − 0.2, 0)
TN/mm ɼॳظ࢟ θ
1(0) = 60
◦ɼ θ
2(0) = 150
◦ɼॳظ
֯ 0.2618rad/s ɼऴ࣌ࠁ θ
1(t
T) = 73
◦( ॳظܗঢ়ͷͱ͖ )
ॳظܗঢ় ࠷దܗঢ়
ਤ 7.3: ܗঢ়ൺֱ
99 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ
§ 8 ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ [4]
ϒϨʔΩ໐͖ɼϩʔλͱύουؒͷຎࡲʹΑΔࣗྭৼಈݱͰ͋Δɽಛʹɼ
ෳૉݻ༗ͷ࣮෦͕ਖ਼ͱͳΔݻ༗ৼಈͱߟ͑ΒΕ͖ͯͨɽ
ਤ 8.1: ं྆ͷϒϨʔΩ෦
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϦϯΫػߏͷܗঢ়࠷దԽ
ਤ 7.5: όολͷʢʁʣ
101 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ
8.1 ( ݻ༗ৼಈ )
ϕ ∈ D ͕༩͑ΒΕͨͱ͖ɼ k ∈ { 1, 2, · · · } ʹରͯ͠ɼ࣍Λຬͨ͢
(s
k, u ˆ
k) = (s
k, u ˆ
R, u ˆ
P) ∈ C × S ΛٻΊΑɽ s
2kρ
Ru ˆ
R− ( ∇ · S ( ˆ u
R))
T= 0
Rdin Ω
R0, s
2ρ
Pu ˆ
P− ( ∇ · S ( ˆ u
P))
T= 0
Rdin Ω
P(ϕ) , S ( ˆ u
R) ν
R= 0
Rdon (
∂Ω
R0\ Γ ¯
R0) , S ( ˆ u
P) ν
P= 0
Rdon (
∂Ω
P(ϕ) \ Γ ¯
P0) ,
S ( ˆ u
R) ν
R= Re [α { ( ˆ u
R− u ˆ
P) · ν
R} ν
R] on Γ
R0, S ( ˆ u
R) τ
R= Re [µα { ( ˆ u
R− u ˆ
P) · ν
R} τ
R] on Γ
R0, S ( ˆ u
P) ν
P= α { ( ˆ u
P− u ˆ
R) · ν
P} ν
Pon Γ
P0, S ( ˆ u
P) τ
P= − µα { ( ˆ u
P− u ˆ
R) · ν
P} τ
Pon Γ
P0ˆ
u
R= ˆ u
Pon (Γ
R0∪ Γ
P0) , u ˆ = 0
Rdon Γ
D0.
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ
P0 R0
¡P0, ¡R0
Coulomb friction
¡D0 ¡P0
¡R0
®, ¹ ºP
¿P ºP
¿R R0 P0
¡P0 P0 P(Á)=(i+Á)( P0)
x
¡D0
(i+Á)(x)
(a) σΟεΫͱύου (b) Coulomb ຎࡲ (c) ύουͷྖҬมಈ ਤ 8.2: ϒϨʔΩϞσϧ
■ ঢ়ଶܾఆ
ݻ༗ৼಈϞʔυ ( มҐ ) u ˆ ͷ Fourier มͷͨΊͷઢܗۭؒͱڐ༰ू߹
U = { ˆ
u ∈ H
1(
R
d; C
d) �� u ˆ = 0
Cdon Γ
D0} , S = U ∩ W
2,2qR(
R
d; C
d)
103 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ
■ ྫ
ද 8.1: ෳૉݻ༗ͷมԽ
ॳظܗঢ় ࠷దܗঢ়
k Re Im
1 -1.692E+01 8.022947E+03 2 -1.444E+01 9.438261E+03 3 8.613E+00 1.249724E+04 4 -2.944E+01 1.437360E+04 5 -5.783E+01 1.629984E+04 6 -5.356E+01 2.168113E+04 7 -5.195E+01 2.394771E+04 8 -6.593E+01 2.573753E+04 9 -6.325E+01 2.711726E+04 10 -6.896E+01 2.893466E+04
k Re Im
1 -1.647E+01 7.745197E+03 2 -1.765E+01 1.027973E+04 3 -1.163E+01 1.110440E+04 4 -3.048E+01 1.503565E+04 5 -4.185E+01 2.092213E+04 6 -5.070E+01 2.186379E+04 7 -6.588E+01 2.671747E+04 8 -7.522E+01 2.756015E+04 9 -7.540E+01 3.137934E+04 10 -7.658E+01 3.320161E+04
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ
■ ܗঢ়࠷దԽ
Ϟʔυ࣍ k ༩͑ΒΕΔͱԾఆ͢ΔɽධՁؔΛ࣍ͷΑ͏ʹఆٛ͢Δɽ f
0(ϕ, s
k) = 2Re [s
k] = s
k+ s
ck,
f
1(ϕ) = −
∫
ΩP(ϕ)
dx + c
1.
8.2 ( ମੵ੍͖ͭෳૉݻ༗࣮෦࠷খԽ )
࣍Λຬͨ͢ Ω
P(ϕ) ΛٻΊΑɽ
(ϕ,ϕ,sk
min
)∈D×C×S{ f
0(ϕ, s
k) | f
1(ϕ) ≤ 0, 8.1 }
105 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ
(a) ॳظܗঢ় (b) ࠷దܗঢ়
ਤ 8.4: 3 ࣍ݻ༗ৼಈϞʔυͷൺֱ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ϒϨʔΩ໐͖ݱʹର͢Δܗঢ়࠷దԽ
(a) ༗ݶཁૉϞσϧ
(a) ॳظܗঢ় (b) ࠷దܗঢ়
ਤ 8.3: ܗঢ়ൺֱ
107 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
M
0Á( µ )º
0º( µ ) M ( µ)
x
1x
2t
h
¡
D0¡
p0p
Nb
D
»
1»
2¹
0( »)
» x
1x
2x
3¹
¹
ਤ 9.2: Ϗʔυ͖ͷγΣϧϞσϧ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
§ 9 γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏ [5]
γΣϧߏʹઃ͚ΒΕͨখ͞ͳߴ͞ͷತԜϏʔυͱΑΕΔɽ
(a) ࣗಈंͷϗϫΠτϘσΟ (b) Ϗʔυߏ
ਤ 9.1: Ϗʔυ͖ͷγΣϧϞσϧ
109 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
ઃܭม θ ͷઢܗۭؒͱڐ༰ू߹
X (θ) = {
θ ∈ H
1(D; R ) � � θ = 0 on D ¯
C0} , D = X ∪ W
1,∞(D; R )
ঢ়ଶܾఆͷղ ( ঢ়ଶม ) u ˆ ͷઢܗۭؒͱڐ༰ू߹
U = { ˆ
u ∈ H
1(
M (θ) ; R
5) �� u ˆ = 0
R5on Γ
D(θ) } S = U ∩ W
2,2qR(
Ω (θ) ; R
5)
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
■ ঢ়ଶܾఆ
ॳظͷγΣϧʹର͢Δதཱ໘ͱྖҬ M
0= {
µ
0(ξ) ∈ R
3� � ξ ∈ D } , Ω
0= {
x + ξ
3ν
0(x) ∈ R
3� � x ∈ M
0, ξ
3∈ ( − t/2, t/2) }
ઃܭม θ : D → R ʹରͯ͠ɼϏʔυͷߴ͞Λ࣍ͷΑ͏ʹ͓͘ɽ ϕ (θ) = h
π tan
−1θ + h 2 มಈޙͷதཱ໘ͱྖҬ
M (θ) = {
(µ
0+ ϕ (θ) ν
0◦ µ
0) (ξ) � � ξ ∈ D } Ω (θ) = {
x + ξ
3ν (x) ∈ R
3� � x ∈ M (θ) , ξ
3∈ ( − t/2, t/2) } .
111 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
■ ܗঢ়࠷దԽ
f (θ, u) = ˆ
∫
M(θ)
( ¯ b · v
M+ ¯ p
N3z − m ¯ · r ) dx +
∫
Γp(θ)∩∂M(θ)
( ¯ p
N· v
M+ ¯ p
N3z − m ¯ · r) dγ
9.2 ( ฏۉίϯϓϥΠΞϯε࠷খԽ )
࣍Λຬͨ͢ θ ΛٻΊΑɽ
(θ,u)ˆ
min
∈D×S{ f (θ, u) ˆ | 9.1 }
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
9.1 (Mindlin-Reissner ͷ൘ཧʹΑΔઢܗੑ )
θ ∈ D ʹରͯ͠ɼ࣍Λຬͨ͢ u ˆ ∈ S ΛٻΊΑɽ
−∇
TMS ˆ
M( ˆ u) = ¯ b
T−∇
M· m ( ˆ u) = ¯ p
N3−∇
TMM ( ˆ u) + m ( ˆ u) = ¯ m
T
in M (θ) , S ˆ
M( ˆ u) ν
M= ¯ p
Nm ( ˆ u) · ν
M= ¯ p
N3M ( ˆ u) ν
M= ¯ m
T
on Γ
p(θ) ∩ ∂M (θ) , S ˆ
M( ˆ u) ν
M= 0
R2m ( ˆ u) · ν
M= 0 M ( ˆ u) ν
M= 0
R2
on (
Γ
N(θ) \ Γ ¯
p(θ) )
∩ ∂M (θ) , u ˆ = 0
R5on Γ
D(θ) .
113 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
0.0Mpa 4.0Mpa
(a) ࠷దܗঢ় (b) Mises Ԡྗ
ਤ 9.4: Ͷ͡ΓՙॏΛ͏͚Δย࣋ͪγΣϧͷ࠷దܗঢ়
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
γΣϧߏʹ͓͚ΔϏʔυͷઃܭ๏
■ ྫ
¡
Dp
Np
N0.0Mpa 7.0Mpa
(a) ڥք݅ (b) Mises Ԡྗ
ਤ 9.3: Ͷ͡ΓՙॏΛ͏͚Δย࣋ͪγΣϧͷॳظܗঢ়
115 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
■ ঢ়ଶܾఆ
ఆৗྲྀͷྲྀͱѹྗͷઢܗۭؒͱڐ༰ू߹
U = {
u ∈ H
1(
R
d; R
d) �� u = 0
Rdon ∂Ω (ϕ) } , U (u
D) = {
u ∈ H
1(
R
d; R
d) �� u = u
Don ∂Ω (ϕ) } , S = U ∩ W
1,∞(
R
d; R
d) , S (u
D) = U (u
D) ∩ W
1,∞(
R
d; R
d) , P =
{
q ∈ L
2(
R
d; R ) � � � �
∫
Ω(ϕ)
q dx = 0 }
, Q = P ∩ L
∞(
R
d; R )
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
§ 10 ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ [6]
அ໘ੵ͕֊ஈঢ়ʹมԽ͢Δ Poiseuille ྲྀΕʹ͓͍ͯɼఆৗྲྀ͔Βඇఆৗྲྀʹ ਪҠ͢Δྟք Reynolds Re
c 40 ͋ͨΓͰ͋Δͱใࠂ͞Ε͍ͯΔɽ
ਤ 10.1: ஈ͖ Poiseuille ྲྀΕ
117 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
͞Βʹɼ u ͱ p ͷ͔͘ཚΛ x ∈ Ω (ϕ) ͱ τ ∈ [0, ∞ ) ʹରͯ͠ɼ
u (τ, x) = u (0, x) + e
sτu ˆ (x) + e
scτu ˆ
c(x) = u (0, x) + 2Re [e
sτu ˆ (x)] , p (τ, x) = p (0, x) + 2Re [e
sτp ˆ (x)]
ͱԾఆ͢Δɽͨͩ͠ɼ s ∈ C ɼ ( · )
cෳૉڞΛද͢ɽ u ˆ ͱ p ˆ ʹର͢Δઢܗۭؒ
ͱڐ༰ू߹Λ࣍ͷΑ͏ʹ͓͘ɽ
U ˆ = { ˆ
u ∈ H
1(
R
d; C
d) �� u ˆ = 0
Rdon ∂Ω (ϕ) } , S ˆ = ˆ U ∩ W
1,∞(
R
d; C
d) , P ˆ =
{ ˆ q ∈ L
2(
R
d; C ) �
� �
�
∫
Ω(ϕ)
ˆ
q dx = 0 }
, Q ˆ = ˆ P ∩ L
∞(
R
d; C )
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
10.1 ( ఆৗ Navier-Stokes )
ϕ ∈ D ʹରͯ͠ b, u
D, µ ͓Αͼ ρ ͕༩͑ΒΕͨͱ͖ɼ ρ (u · ∇ ) u
T− ∇
T(
µ ∇ u
T)
+ ∇
Tp = b
Tin Ω (ϕ) ,
∇ · u = 0 in Ω (ϕ) , u = u
Don ∂Ω (ϕ) ,
∫
Ω(ϕ)
p dx = 0
Λຬͨ͢ (u, p) ∈ S (u
D) × Q ΛٻΊΑɽ
119 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
■ ܗঢ়࠷దԽ
ධՁؔΛ͔͘ཚݻ༗࣮෦ f
0(s
r) = s
r+ s
cr= 2Re [s
r]
ͱ͓͘ɽͨͩ͠ɼ r Re[s
i] ͕࠷େͱͳΔϞʔυ࣍ͱ͢Δɽ
10.3 ( ͔͘ཚݻ༗࣮෦ͷ࠷খԽ )
࣍Λຬͨ͢ Ω (ϕ) ΛٻΊΑɽ min
(ϕ,u,p,s˜ r,ˆur,ˆpr)∈D×S×Q×C×S׈ Qˆ
{ f
0(s
r) � � 10.1, 10.2 }
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
10.2 ( ͔͘ཚݻ༗ )
ϕ ∈ D ʹରͯ͠ (u, p) ͕༩͑ΒΕͨͱ͖ɼ i ∈ { 1, 2, · · · } ʹରͯ͠
ρs u ˆ
Ti+ ρ (u · ∇ ) ˆ u
Tr+ ρ ( ˆ u
i· ∇ ) u
T− ∇
T(
µ ∇ u ˆ
Ti)
+ ∇
Tp ˆ = 0
TRdin Ω (ϕ) ,
∇ · u ˆ
i= 0 in Ω (ϕ) , ˆ
u
i= 0
Rdon ∂Ω (ϕ) ,
∫
Ω(ϕ)
ˆ
p dx = 0,
∫
Ω(ϕ)
ρ u ˆ
i· u ˆ
cidx = 1
Λຬͨ͢ s
i∈ C ͱ ( ˆ u
i, p ˆ
i) ∈ S × ˆ Q ˆ ΛٻΊΑɽ
121 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
¡0.006
¡0.004
¡0.002 0 0.002 0.004 0.006 0.008
35 40 45 50 55
Real part of the eigenvalue
Reynolds number Re Initial domain
Optimized domain
ਤ 10.3: Reynolds ʹର͢Δݻ༗ͷ࣮෦࠷େͷਪҠ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ྲྀΕͷ҆ఆੑ্ͷͨΊͷܗঢ়࠷దԽ
■ ྫ
(a) ॳظܗঢ়
(b) ࠷దܗঢ়
ਤ 10.2: ஈ͖ Poiseuille ྲྀΕ ( ॳظྖҬʹ͓͍ͯ Re = 45)
123 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
■ ঢ়ଶܾఆ
ઃܭม ϕ ͷઢܗۭؒͱڐ༰ू߹
X = {
ϕ ∈ H
1(
D
0; R
d) �� ϕ = 0
Rdon ∂D
0∪ ∂F
0∪ ∂G
0∪ Γ
C0∪ Ω ¯
C0} , D = {
ϕ ∈ X ∩ W
1,∞(
R
d; R
d) �� શ୯ࣹͷ݅ } .
੩ిϙςϯγϟϧͷઢܗۭؒͱڐ༰ू߹
U = {
u ∈ H
1(D
0; R ) � � u = 0 on ∂E (ϕ) ∪ ∂G (ϕ) } , U (u
D) = {
u ∈ H
1(D
0; R ) �
� u = u
Don ∂E (ϕ) ∪ ∂G (ϕ) } , S = U ∩ W
1,∞(D
0; R ) ,
S (u
D) = U (u
D) ∩ W
1,∞(D
0; R ) ,
ͱ͓͘ɽͨͩ͠ɼ u
D∈ H
1(D
0; R ) ∩ W
1,∞(D
0; R ) ∂E (ϕ) ্Ͱ u = α ɼ
∂G (ϕ) ্Ͱ u = 0 Λຬͨؔ͢ͱ͢Δɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
§ 11 ੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ [7]
੩ి༰ྔࣜηϯαࢦͷݕग़ͳͲʹΘΕΔɽ
E0
F0
G0 G0 G0
∂D0
Ω0
ਤ 11.1: ॳظ੩ి Ω
0= D
0\ ( E ¯
0∪ G ¯
0)
125 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
11.2 ( ݕग़ମ͕͋Δ੩ి )
ϕ ∈ D ͱਖ਼ఆ α ͕༩͑ΒΕͨͱ͖ɼ
− ∇ · e (u
F) = 0 in Ω (ϕ) \ F
0= D
0\ (E (ϕ) ∪ G (ϕ) ∪ F
0) ,
∂
νu
F= 0 on ∂D
0(ϕ) , u
F= α on ∂E (ϕ) , u
F= 0 on ∂G (ϕ) ∪ F ¯
0Λຬͨ͢ u
F∈ S (u
D) ΛٻΊΑɽ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
11.1 ( جຊ੩ి )
ϕ ∈ D ʹରͯ͠ɼਖ਼ఆ α ͕༩͑ΒΕͨͱ͖ɼ
− ∇ · e (u) = 0 in Ω (ϕ) = D
0\ (E (ϕ) ∪ G (ϕ)) ,
∂
νu = 0 on ∂D
0(ϕ) , u = α on ∂E (ϕ) , u = 0 on ∂G (ϕ)
Λຬͨ͢ , u ∈ S (u
D) ΛٻΊΑɽ
127 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
■ ྫ
E0
F0
G0 0
@D0
¡C0
(a) ઃఆ (b) ༗ݶཁૉϞσϧ
ਤ 11.2: ಥ͖ग़ͨిۃͷ͋Δ 2 ࣍ݩ੩ి
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
■ ܗঢ়࠷దԽ
f
0(ϕ, u, u
F) = − ∥ u − u
F∥
2H1(Ω(ϕ)\F0(ϕ);R)= −
∫
Ω(ϕ)\F0
{ (u − u
F)
2+ (e (u) − e (u
F)) · (e (u) − e (u
F)) } dx, f
1(ϕ) =
∫
E(ϕ)
dx − s
1 11.3 ( ମੵ੍͖ͭ੩ిؒͷޡࠩϊϧϜ࠷খԽ )
࣍Λຬͨ͢ Ω (ϕ) ΛٻΊΑɽ
(ϕ,u,uF)∈D×S
min
(uD)×S(uD){ f
0(ϕ, u, u
F) | f
1(ϕ) ≤ 0, 11.1, 11.2 }
129 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
0 2 4 6 8 10 12
0.6 0.7 0.8 0.9 1 1.1
Costfunctions
Number of Iteration
1+f
1/s
02+f
0/jf
0 initj
0 2 4 6 8 10 12
0 20 40 60 80
Sencing capacitance [pF/m] Increasing rate of capacitance
Number of Iteration
0 0.1 0.2 0.3 0.4
with finger without finger increasing rate
(a) ධՁؔ (b) ੑೳ
ਤ 11.4: ܗঢ়มಈʹର͢Δ܁ฦཤྺ
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
(a) ॳظ (b) ࠷దԽޙ ( ະऩଋ )
ਤ 11.3: ྖҬมಈલޙͷܗঢ়
131 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
(a) ॳظ (b) ࠷దԽޙ ( ऩଋ )
ਤ 11.6: ྖҬมಈલޙͷܗঢ় (E (ϕ) ⊂ D
0\ Ω ¯
C0)
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
F0
G0
@D0
E0
D0n C0 0
¹
(a) ઃఆ (b) ༗ݶཁૉϞσϧ
ਤ 11.5: ಥ͖ग़ͨిۃͷ͋Δ 2 ࣍ݩ੩ి (E (ϕ) ⊂ D
0\ Ω ¯
C0)
133 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
FreeFEM++Λ༻͍࣮ͨश
12 FreeFEM++ Λ༻͍࣮ͨश
1
H
1ޯ๏ / H
1Newton ๏
2 ࣍ݩઢܗੑମ ( ฏۉίϯϓϥΠΞϯε࠷খԽ , hook):
9.11.5_shape_elastic/2d-hook/domain_integral/grad/
9.11.5_shape_elastic/2d-hook/domain_integral/Newton/
2
༗ݶཁૉͷ࣍ : 1 ࣍ཁૉ / 2 ࣍ཁૉ
3 ࣍ݩઢܗੑମ ( ฏۉίϯϓϥΠΞϯε࠷খԽ , cantilever):
9.11.5_shape_elastic/3d-cantilever/boundary_integral/grad/
main.edp ϑΝΠϧΛςΩετΤσΟλͰ։͖ɼ
fespace Vh(Th,[P2,P2,P2]);//Finite element space Λ
fespace Vh(Th,[P1,P1,P1]);//Finite element space ʹมߋ͢Δɽ
3
ಛҟͷڍಈ : ڥքੵܕܗঢ়ඍ / ྖҬੵܕܗঢ়ඍ
2 ࣍ݩઢܗੑମ ( ฏۉίϯϓϥΠΞϯε࠷খԽ , L-shape):
9.11.5_shape_elastic/2d-L-shape/boundary_integral/grad/
9.11.5_shape_elastic/2d-L-shape/domain_integral/grad/
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
੩ి༰ྔࣜηϯαͷܗঢ়࠷దԽ
0 5 10 15 20
0.6 0.7 0.8 0.9 1 1.1
Costfunctions
Number of Iteration
1+f
1/s
02+f
0/jf
0 initj
0 5 10 15 20
0 20 40 60 80
0 0.1 0.2 0.3 0.4
Sencing capacitance [pF/m] Increasing rate of capacitance
Number of Iteration with finger without finger increasing rate
(a) ධՁؔ (b) ੑೳ
ਤ 11.7: ܗঢ়มಈʹର͢Δ܁ฦཤྺ (E (ϕ) ⊂ D
0\ Ω ¯
C0)
135 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ࢀߟจݙ
ࢀߟจݙ
[1] ൞্ ल . ܗঢ়࠷దԽ .
ग़൛ , ౦ژ , 10 2016.
[2] H. Azegami.
Second derivatives of cost functions and h1 newton method in shape optimization problems.
In Patrick van Meurs, Masato Kimura, and Hirofumi Notsu, editors, Mathematical Analysis of Continuum Mechanics and Industrial Applications II, Proceedings of the International Conference CoMFoS16, Mathematics for Industry 30, pages 61–72.
Springer Singapore, 12 2017.
[3] H. Azegami, L. Zhou, K. Umemura, and N. Kondo.
Shape optimization for a link mechanism.
Structural and Multidisciplinary Optimization, 48(1):115–125, 2 2013.
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
·ͱΊ
13 ·ͱΊ
1
࠷దઃܭɼঢ়ଶܾఆ੍͕ࣜͱͯ͠ՃΘͬͨෆ͖ࣜͭඇઢܗ
࠷దԽͷΫϥεͱΈͳ͢͜ͱ͕Ͱ͖Δɽͦͷղ๏ޯ๏ Newton
๏ʹج͍ͮͯߏ͞ΕΔɽ
2
࿈ଓମͷܗঢ়࠷దԽͷ֦ுؔղੳʹΑ࣮ͬͯݱ͞ΕΔɽ
3
ઃܭʹཱͭΑ͏ͳΛదʹߏͰ͖ΕɼͦΕΒΛղ͘͜ͱՄ
ೳͱͳ͍ͬͯΔɽ
137 / 140
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ࢀߟจݙ
ࢀߟจݙ (cnt.)
[7] Masayoshi Satake, Noboru Maeda, Shinji Fukui, and Hideyuki Azegami.
Shape optimization of electrostatic capacitive sensor.
In Proceedings of the 10th World Congress on Structural and Multidisciplinary Optimization (WCSMO-10) (USB), pages 1–10, 5 2013.
ܗঢ়࠷దԽཧͱઃܭͷԠ༻
ࢀߟจݙ
ࢀߟจݙ (cnt.)
[4] K. Shintani and H. Azegami.
Shape optimization for suppressing brake squeal.
Structural and Multidisciplinary Optimization, 50(6):1127–1135, 5 2014.
[5] K. Shintani and H. Azegami.
A design method of beads in shell structure using non-parametric shape optimization method.
In Proceedings of the the ASME 2014 International Design Engineering Technical Conferences & Computers and Information in Engineering Conference (IDETCCIE 2014) (eBook), pages 1–8, 8 2014.
[6] T. Nakazawa and H. Azegami.
Shape optimization of flow field improving hydrodynamic stability.
Japan Journal of Industrial and Applied Mathematics Japan Journal of Industrial and Applied Mathematics, 10 2015.
Accepted.
139 / 140