The Inverse Problem of Determination of the Heat Source in the 1D Heat Equation
Jiichiro URABE* Yorimasa OSHIME** Hideki TAKUWA*** and Shota SAKURAI****
(Received January 20, 2011)
First of all, we think the uniform stick that the heat source exists in inside. The heat equation with the heat source is considered in this paper. As assumption, the special conditions are imposed to the heat source. We consider the inverse problem that decides the heat source from the observational data of temperature of the uniform stick at one point. Then, we find the unknown function of the heat source from the observational data of the stick at one point excluded a certain points of limited piece. In the theory of Yamamoto-kim (2008), though the uniqueness of determination of the heat source has been proven, the reconstruction of the heat source is not considered. The reconstruction method of the heat source is considered in this paper. Result, we find the heat source by imposing the special conditions to the heat source.
Key wordsɿ inverse problem, heat source Ωʔϫʔυ ɿٯɼݯ
Ұ࣍ݩํఔࣜʹ͓͚Δݯܾఆٯ
Ӝ ෦ ࣏ Ұ ɾ ԡ པ ণɾ ଟ ٱ ӳ थɾ ᓎ Ҫ ᠳ ଠ
1. ॹݴ
͋ΔΛղ͘ͱ͖ʹɼॳظͳͲͷʮݪҼʯɼํఔ
ࣜͳͲͷʮϞσϧʯ͔Βɼʮ݁ՌʯͰ͋ΔղΛٻΊΔॱ
͕ҰൠతͰ͋ΔɽͦΕʹର͠ɼݱࡏͷֶɼཧֶɼҩ
ֶͳͲͷ༷ʑͳͰʮԠʯʮ݁ՌʯͳͲͷग़ྗ͔
ΒɼʮݪҼʯʮೖྗʯΛਪఆ͢Δٯͱ͍͏͕
͘औΓѻΘΕΔΑ͏ʹͳ͖͍ͬͯͯΔɽ
ٯͷ۩ମతͳԠ༻ྫͱͯ͠ɼͨͱ͑ɼҩֶ
அͷͨΊͷ̢̧̞ɼൃػߏɼ͢ͳΘͪݯʹ͓͚Δμ
* Department of Factory of Culture and Information Science, Doshisha University.
Telephone:+81-774-65-7610, E-mail:[email protected]
** Department of Science and Engineering, Doshisha University.
Telephone:+81-774-65-6494, E-mail:[email protected]
*** Department of Science and Engineering, Doshisha University.
Telephone:+81-774-65-6431, E-mail:[email protected]
ΠφϛΫεͷܾఆɼُ྾ͷ୳ɼը૾෮ݩͳͲ༷ʑͷ
͕͋͛ΒΕΔ1)ɽ͔͠͠ɼٯҰൠతʹॱͱ
ҧ͍ɼղ͘͜ͱࠔͰ͋ΔͱݴΘΕ͍ͯΔɽ
ͦ͜ͰຊݚڀͰɼ
• Ұ༷ͳͷԹΛଌఆ͠ɼݟΔ͜ͱͷͰ͖ͳ͍ঢ়ଶ ͷෆ໌ͳݯΛਪఆ͢Δ
͜ΕΛѻ͏͜ͱΛతͱ͍ͯ͠Δɽ
ͦ͜Ͱɼݯͷ݅Λ
Q(x, t) =μ(t)f(x), 0< x < π, t >0 ͱ͓͘ɽͨͩ͠ɼ
μ(t) =e−σt
Ͱ͋Δͱͯ͠ɼ৽ͨʹݯͷ݅Λઃఆͨ͠ɽͷ۠ؒ
ͷҰͰͷ؍ଌσʔλ͔ΒݯΛܾఆ͢ΔٯΛߟ
ͨ݁͠ՌɼݯΛܾఆ͢Δ͜ͱ͕Ͱ͖ͨɽ
2. ݁Ռ
෦ʹݯ͕ଘࡏ͢Δ͕͞πͷҰ༷ͳΛߟ͑Δɽ
ͷ෦ͷॴΛxɼ࣌ࠁΛtɼॴx࣌ࠁtʹ͓͚Δ
ͷԹΛu(x, t)ͱ͢Δɽݯͷ͋ΔಋํఔࣜΛߟ
͑ɼͦͷͱ͖ͷॳظ݅ɼڥք݅ͱʹ0ͱ͢Δɽ nx=kπ(n= 1, ..., N, k= 1, ..., N)ͱͳΔ༗ݶݸͷx Λআ͍ͨͷ۠ؒͷҰΛx0ͱ͠ɼͦͷͰͷ؍ଌ σʔλu(x0, t)͔ΒɼະͷݯΛܾఆ͢ΔٯΛߟ
͑Δɽͦͷ݁Ռɼݯͷܗʹ݅Λ༩͑ͯΔ͜ͱͰɼ
ݯͷະͰ͋ͬͨ෦ΛٻΊΔ͜ͱ͕Ͱ͖ͨɽ
3. ݯܾఆٯͷֶతهड़
ຊདྷॱͱͯ͠ͷܗɼաڈͷԹͱɼؔͷܗ͕
Θ͔͍ͬͯΔݯ͔ΒɼະདྷͷԹΛٻΊΔͱ͍͏
Ͱ͋ΔɽͦΕʹର͠ࠓճѻ͏ɼ෦ͷҰͰͷ Թͷ؍ଌσʔλu(x0, t)͔ΒະͷݯQ(x, t)Λਪఆ
͠Α͏ͱ͢ΔͰ͋Δɽ
σΟϦΫϨڥք݅ͷԼͰɼݯͷ͋Δํఔࣜɼ ut(x, t) =uxx(x, t) +Q(x, t), 0< x < π, t >0 (1) Λߟ͑ɼͦͷͱ͖ॳظ݅ɼ
u(x,0) = 0, 0< x < π, (2) ڥք݅ɼ
u(0, t) =u(π, t) = 0, t >0 (3)
ͱ͢Δɽ
͜ͷͱ͖ݯͷ݅Λ
Q(x, t) =μ(t)f(x), 0< x < π, t >0 (4) ͱ͍͏࣌ؒͷؔͱۭؒͷؔͷੵͷܗͰ৽ͨʹߟ͑Δ
͜ͱʹ͢Δɽf(x)͕ܾఆ͍ͨؔ͠ͱ͢ΔɽͦͷͨΊ μ(t)͋Β͔͡ΊΘ͔͍ͬͯΔͱ͍͏ઃఆͰ͋Δɽ͜ͷ ͱ͖۠ؒͷҰx0 ∈(0, π) Ͱͷ؍ଌσʔλ͔Βɼ
ݯʹදΕΔؔf(x)Λܾఆ͢ΔٯΛߟ͢Δɽ͜
͜Ͱͷ؍ଌσʔλҰʹݶఆ͞Ε͓ͯΓɼใྔগ ͳ͍͕ԹܭͳͲΛઃஔ͢Δ͜ͱͰ࣮ݱͰ͖Δɽ
ٯͰɼॱͷखॱͷٯΛ୧Δ͜ͱͰະͷؔ
f(x)ΛٻΊΔ͜ͱ͕Ͱ͖ͦ͏Ͱ͋ΔɽͦΕΛ͔֬Ί ΔͨΊʹ۩ମతͳܗͱͯ͠ɼ
μ(t) =e−σt
ͱͯ͠ɼٻΊ͍ͨٯͷղͷܗΛɼ
f(x) = N n=1
bnsinnx (5)
ͱ͢Δɽͨͩ͠bn(n= 1, ..., N)ະͰ͋Δɽ͜ͷ
ྻ{bn}Nn=1ΛٻΊ͍ͨɽ
4. ओఆཧ
෦ʹݯͷଘࡏ͢ΔҰ༷ͳͷಋํఔࣜΛߟ͑
Δɽu(x, t)Λॴxɼ࣌ࠁtʹ͓͚ΔͷԹͱ͢Δͱɼ
ut(x, t) =uxx(x, t) +Q(x, t), 0< x < π, t >0 (6) ͱͳΓɼͦͷͱ͖ͷॳظ݅ɼ
u(x,0) = 0, 0< x < π (7) Ͱ͋Γɼڥք݅ɼ
u(0, t) =u(π, t) = 0, t >0 (8) ͱ͢Δɽͦͷͱ͖ɼԾఆͱͯ͠ݯͷ݅Λ
Q(x, t) =μ(t)f(x), 0< x < π, t >0 (9)
ͱ͓͘ɽͨͩ͠μ(t)ɼ
μ(t) =e−σt (10)
ͱΘ͔͍ͬͯΔͷͱ͢Δɽsinnx = 0(n = 1, ..., N)ɼ
͢ͳΘͪnx=kπ(n= 1, ..., N, k= 1, ..., N)ͱͳΔ༗ݶ ݸͷxΛআ͍ͨ۠ؒͷҰx0Ͱͷ؍ଌσʔλu(x0, t)
͔ΒɼݯͷٻΊ͍ͨ෦Ͱ͋Δf(x)Λܾఆ͢Δٯ
Λߟ͑Δɽ ٻΊ͍ͨؔΛ
f(x) = N n=1
bnsinnx (11)
ͱઃఆ͢Δɽͨͩ͠bn(n= 1, ..., N)ະͰ͋Δɽ
͜ͷͱ͖ࠓճͷٯ࣍ͷ༷ͳఆཧͱͳΔɽ
ఆཧ[ݯܾఆٯ]
u(x, t)͕ࣜ(6)ʖ (8)ɼQ(x, t)͕ࣜ(9)Ͱ༩͑ΒΕɼμ(t) Λࣜ(10)ͷͷͱ͢Δɽ·ͨf(x)Λࣜ(11)ͱ͢Δɽ
͜ ͷ ͱ ͖ ɼ͋ Δ ༗ ݶ ݸ ͷ Λ আ ͍ ͨ x0 ʹ ର ͠ ͯ u(x0, t)(t > 0)Λ༩͑ΕɼҰҙతʹྻ{bn}Nn=1 ͕ ߏͰ͖Δɽ
ͭ·ΓɼະͷݯQ(x, t) =μ(t)f(x)͕ߏͰ͖Δɽ
5. ຊݚڀͱઌߦ݁Ռͷൺֱɾٴͼվળ
5.1 ઌߦ݁Ռ
ઌߦ݁Ռͱͯ͠ɼࢁຊɾۚ[2]ɼp.60ͷఆཧΛҎԼͰ
հ͢Δɽ
ݯͷ͋Δํఔࣜɼ
ut(x, t) =uxx(x, t) +Q(x, t), 0< x < π, t >0 (12) Λߟ͑ɼͦͷͱ͖ॳظ݅ɼ
u(x,0) = 0, 0< x < π (13) Ͱ͋Γɼڥք݅ɼ
u(0, t) =u(π, t) = 0, t >0 (14)
ͱ͢Δɽ
ݯͱͯ͠ɼ
Q(x, t) =μ(t)f(x), 0< x < π, t >0 (15) ͷܗΛߟ͑Δɽ͜ͷͱ͖ɼf(x)Λ۠ؒͷҰx0∈(0, π) Ͱͷ؍ଌσʔλ͔Βܾఆ͢ΔٯΛߟ͍ͯ͠Δɽ
͜͜Ͱɼ
μ∈C1[0,∞), (16)
f ∈C5[0, π], (17)
djf
dxj(0) = djf
dxj(π) = 0, j= 0,1, ...,4 (18) ͱ͍ͯ͠Δɽ
μ(t)Θ͔͍ͬͯΔͱͯ͠ɼf(x)ΛٻΊΔΛߟ
͑Δɽ
͜ͷͱ͖ɼ͜ͷٯͰ࣍ͷ͜ͱ͕Θ͔Δɽ
ఆཧ(ࢁຊɾۚ[2]ɼp.60)
u(x, t)͕ࣜ(12)-(14)ɼQ(x, t)͕ࣜ(15)Ͱ༩͑ΒΕͯ
͍Δɽ·ͨμ(t)ࣜ(16)ɼf(x)ࣜ(17)(18)ͷ͕݅
༩͑ΒΕ͍ͯΔɽͦͯ͠μ(0)= 0ΛԾఆ͢Δɽ
͜ͷͱ͖؍ଌx0ɼx0
π ͕ແཧͰ͋ΔͱԾఆ͢Δɽ
͜ͷx0ʹରԠ͢Δu(x0, t)Λ༩͑Εɼf(x)ΛҰҙత ʹٻΊΔ͜ͱ͕Ͱ͖Δɽ
5.2 ઌߦ݁Ռͱຊݚڀͱͷൺֱɾվળ
ઌߦ݁ՌͱຊݚڀͷతΛͦΕͧΕ͋͛ͯΈΔɽ
(ઌߦ݁Ռ)
• ݯܾఆٯͷֶతهड़
• ݯܾఆͷҰҙੑͷূ໌
• f(x)ࣜ(17)(18)ͷԾఆͷԼ
(ຊݚڀ)
• ݯܾఆٯͷֶతهड़
• ݯܾఆͷ۩ମతͳ࠶ߏ
• f(x)ࣜ(17)(18)ͷԾఆʹͯ·Βͳ͍
ઌߦ݁Ռʹ͓͍ͯɼݯܾఆٯͷֶతهड़
ͳ͞Ε͍ͯΔ͕ɼͦ͜ͰҰҙੑͷূ໌Λ͢Δ͜ͱ͕
తͰ͋Δɽैͬͯ۩ମతͳݯͷ࠶ߏͷखॱʹ͍ͭͯ
ड़ΒΕ͍ͯͳ͍ɽͦΕʹର͠ຊݚڀͰɼ۩ମతͳ
ݯͷ࠶ߏߦͬͨɽ
ͦͯ͠ઌߦ݁ՌͰɼf(x)ࣜ(17)(18)ͷԾఆʹ
ͯ·Βͳ͚ΕͳΒͳ͔͕ͬͨɼຊݚڀͰf(x)
ࣜ(17)(18)ͷԾఆʹͯ·Βͳ͍ͷߟ͑Δ͜ͱ͕
Ͱ͖Δɽ ɹ
6. ݯܾఆٯͷղ๏
6.1 ॱͰͷղͱͦͷߏखଓ͖
͜ͷ߹ͷॱɼݯͷؔͷܗ͕Θ͔͍ͬͯͯɼ ղͰ͋ΔະདྷͷԹΛٻΊΔͱ͍͏Ͱ͋Δɽ
ॱͷղެࣜɼ u(x, t) =
∞ n=1
2 π{
t
0 e−n2(t−s){ π
0 μ(s)f(y) sinnydy}ds}sinnx ͱͳΔɽ
an= 2 π
π
0 f(y) sinnydy (19) ͱ͓͘ͱɼx=x0Λೖͯ͠u(x0, t)ͱ͢Δͱ
u(x0, t) = t
0 { ∞ n=1
e−n2(t−s)ansinnx0}μ(s)ds ͱͳΔɽ͜͜Ͱ
k(t) = ∞ n=1
e−n2tansinnx0 (20)
ͱ͓͘ͱɼ
u(x0, t) = t
0 k(t−s)μ(s)ds ͱͳΓɼมมʹΑΓɼ
u(x0, t) = t
0 μ(t−s)k(s)ds (21)
ΛಘΔɽ
ݫີʹ͜ͷ߹ͷॱu(x, t) ΛٻΊΔͰ
͋Δɽ͜͜Ͱu(x, t)ʹx=x0Λೖͯ͠u(x0, t)ͱ
͢Δखॱߟ͍͑ͯΔɽཧ͢Δͱɼࣜ(19)ʖ (21)ͷख ॱΛॱʹ౿Ή͜ͱͰu(x0, t)ΛٻΊΔ͜ͱ͕Ͱ͖Δɽ
۩ମతʹॱΛղ͍͍ͯ͘ɽࣜ(19)ΑΓf →anɼ an=bn (n= 1, ..., N)
ͱͳΔɽ࣍ʹࣜ(20)ΑΓɼan →k(t)ɼ
k(t) = N n=1
e−n2tbnsinnx0
ͱͳΔɽͦͯࣜ͠(21)ΑΓk(t)→u(x0, t)ɼ
u(x0, t) = N n=1
bnsinnx0
σ−n2 (e−n2t−e−σt) ͱͳΓɼ͜ΕͰu(x0, t)͕ٻ·ͬͨɽ
6.2 ٯͰͷݯ{bn}ͷߏखॱ6)
࣍ʹٯͰͷݯͷߏखॱʹ͍ͭͯड़Δɽॱ
ͰٻΊͨu(x0, t)Λ؍ଌσʔλͱߟ͑ͯɼ
f(x) = N n=1
bnsinnx
ͷະͷ෦Ͱ͋Δbn(n= 1, ..., N)ΛٻΊ͍ͯ͘ɽ u(x0, t) → k(t)ͱͯࣜ͠(21)ͷٯͷखॱΛߟ͑Δɽ u(x0, t)∈C1[0,∞)ͳΒɼ
k(t) =ut(x0, t) +σu(x0, t)
ͱͳΓɼ͜Εʹઌ΄ͲٻΊͨॱͷղΛೖ͢Δͱɼ
k(t) = N n=1
e−n2tbnsinnx0 (22)
ͱͳΔɽ
࣍ʹk(t)→anΛߟ͑Δɽdn=bnsinnx0ͱ͓͍ͯd1
͔ΒॱʹٻΊ͍ͯ͘ɽࣜ(22)Λมܗ͢Δͱɼ
d1=etk(t)−e−t N n=2
dne(−n2+2)t
ͱͳΔɽࣜ(20)ͷk(t)Λೖͯ͠t→ ∞ͱ͢Δͱୈೋ
߲ୈҰ߲ʹൺແࢹͰ͖ͯɼ d1= lim
t→∞etk(t) =a1sinx0
ͱͳͬͯɼa1 =b1ͱͳΔɽ͜͜Ͱsinx0= 0Ͱͳ͚Ε
ͳΒͳ͍͜ͱ͕Θ͔Δɽn= 2Ҏ߱ಉ༷ͷख๏Ͱղ
͘͜ͱ͕Ͱ͖ɼ
an=bn (n= 1, ..., N)
ͱͳΔɽͦͯ͠ઌ΄Ͳͱಉ༷ʹsinnx0 = 0Ͱͳ͚Ε
ͳΒͳ͍ɽΑͬͯ؍ଌͰ͋Δx0ɼsinnx= 0(n= 1, ..., N)ɼ͢ͳΘͪnx=kπ(n= 1, ..., N, k = 1, ..., N) ͱͳΔxΛআ͍ͨͰͳ͚ΕͳΒͳ͍͜ͱ͕Θ͔Δɽ
͜Ε͕؍ଌx0ͷ݅Ͱ͋Δɽ
࠷ޙʹan → f ͱͯࣜ͠(19)ͷٯΛߟ͑Δͱɼf(x)
ਖ਼ݭڃͰ͋ΔͷͰɼ f(x) =
∞ n=1
ansinnx
Ͱ͋Δɽઌ΄Ͳٻ·ͬͨanΛೖ͢Δͱɼ
f(x) = N n=1
bnsinnx
ͱͳΓٻΊ͍ͨܗͷղΛٻΊΔ͜ͱ͕Ͱ͖ͨɽΑͬͯ
μ(t) =e−σtͷͱ͖ݯΛ࠶ߏ͢Δ͜ͱ͕Ͱ͖ͨɽ
6.3 ༗ݶ࣌ؒͷ؍ଌσʔλͷ߹
ٯͷk(t)→anͷͱ͖ʹɼ؍ଌσʔλu(x0, t)ͷ t͕༗ݶͷ۠ؒʹؚ·ΕΔ߹Λߟ͑Δɽ
T ਖ਼ఆͱ͢Δͱɼࣜ(22)ΑΓ
k(T) = e−Td1+e−4Td2+· · ·+e−N2TdN
k(2T) = e−2Td1+e−8Td2+· · ·+e−2N2TdN
k(3T) = e−3Td1+e−12Td2+· · ·+e−3N2TdN ...
k(N T) = e−NTd1+e−4NTd2+· · ·+e−N3TdN
Ͱ͋Γɼ͜͜Ͱvn=e−n2T ͱ͓͘ͱ
⎛
⎜⎜
⎜⎜
⎜⎜
⎝ k(T) k(2T)
... k(N T)
⎞
⎟⎟
⎟⎟
⎟⎟
⎠
=
⎛
⎜⎜
⎜⎜
⎜⎜
⎝
v1 v2 . . . vN v12 v22 . . . v2N ... ... . .. ...
vN1 v2N . . . vNN
⎞
⎟⎟
⎟⎟
⎟⎟
⎠
⎛
⎜⎜
⎜⎜
⎜⎜
⎝ d1 d2
... dN
⎞
⎟⎟
⎟⎟
⎟⎟
⎠ ͱͳΔɽ
V =
⎛
⎜⎜
⎜⎜
⎜⎜
⎝
v1 v2 . . . vN
v21 v22 . . . vN2 ... ... . .. ...
vN1 vN2 . . . vNN
⎞
⎟⎟
⎟⎟
⎟⎟
⎠
ͱ͓͘ͱɼϰΝϯσϧϞϯυͷߦྻࣜΑΓVͷߦྻࣜɼ
|V| =
1≤j≤N
vj
1≤j≤i≤N
(vj−vi)
=
1≤j≤N
e−j2T
1≤j≤i≤N
(e−j2T −e−i2T)
ͱͳΓ|V| = 0ΑΓɼV ٯߦྻ͕ଘࡏ͢ΔͷͰɼdnΛ ٻΊΔ͜ͱ͕Ͱ͖Δɽ
͜ͷΑ͏ʹtΛT,2T,3T, . . . , N Tͱִؒʹऔͬͯ
Δ͜ͱͰdnΛٻΊΔ͜ͱ͕Ͱ͖Δɽ
7. ݁ݴ
ຊݚڀͰɼٯΛղ͍ͯɼҰ༷ͳͷݯΛܾఆ
͢Δ͜ͱ͕తͰ͋ͬͨɽͦͷͨΊʹݯʹQ(x, t) =
μ(t)f(x)ͱ͍͏݅Λ༩͑ͨɽͦͯ͠μ(t)Θ͔͍ͬͯ
Δͷͱͯ͠ɼະͷؔf(x)ΛٻΊΔΛߟ͠
ͨɽ͞Βʹf(x)ʹ f(x) =
N n=1
bnsinnx
ͱ͍͏ղͷܗΛߟ͑ɼະͰ͋Δ{bn}ΛٻΊΔʹ ؼணͨ͠ɽ
ͦͷ݁Ռɼ͋Δ༗ݶݸͷΛআ͍ͨ۠ؒͷҰͰͷ Թͷ؍ଌσʔλ͔ΒɼݯͷٻΊ͍ͨؔͰ͋Δf(x) Λܾఆ͢Δ͜ͱ͕Ͱ͖ͨɽ
ࢁຊɾۚ[2]ɼp.60ͷઌߦ݁Ռʹ͓͍ͯɼݯܾఆͷ ٯͷҰҙੑূ໌͞Ε͍ͯΔ͕ɼݯܾఆͷ۩ମత ͳղ๏ʹ͍ͭͯ৮ΕΒΕ͍ͯͳ͍ɽ
ຊݚڀͰɼݯܾఆͷ۩ମతͳղ๏ʹ͍ͭͯߟ͠ɼ ಛघͳ݅ͷԼͰݯΛܾఆ͢Δ͜ͱ͕Ͱ͖ͨɽ
ຊݚڀ2009ಉࢤࣾཧֶݚڀॴݚڀॿۚͷ
ิॿΛड͚ͯߦΘΕ·ͨ͜͠ͱΛه͠ɼ֤ؔҐʹײँ
ޚྱਃ্͛͠·͢ɽ
ࢀɹߟɹจɹݙ
1) ٱอ࢘,ʠ ٯͷߟ͑ํͱΈ ʡɼཧՊֶɼ403 רɼ1߸(1998)ɼpp28-33.
2) ࢁຊণ߂ɼۚשɼʮํఔࣜͰֶͿٯʯ,ʢαΠΤ ϯεࣾɼ౦ژɼ2008ʣ
3) ऱ೭உ,ʮվగɹؔղੳೖʯ,ʢαΠΤϯεࣾɼ౦ ژɼ1975ʣ
4) అਖ਼ٛ,ʮٯͷֶʯ,ʢڞཱग़൛ɼ౦ژɼ2000ʣ 5) Victor Isakov, Inverse Source Problems, American
Mathematical Society, (1990)
6) Victor Isakov,Inverse Problems for Partial Differential Equations, Springer-Verlag, (2006)
7) ొࡔએ,ʮٯͷཧͱղ๏ʯ,ʢ౦ژେֶग़൛ձɼ౦ ژ1999ʣ
8) ୩ౡݡೋ,ʮϧϕʔάੵͱؔղੳʯ,ʢேॻళɼ౦ ژɼ2002ʣ
9) ࢁຊণ,ʮٯೖʯ,ʢؠॻళɼ౦ژɼ2002ʣ 10) ྛࠀߦ,ʮֶͷָ͠Έʯ,ʢຊධࣾɼ౦ژɼ2007ʣ