卡馬薩-霍爾姆方程 (Camassa Holm equation)是流體力學中的一個非線性偏微分方程
u
t
+
2
κ
u
x
−
u
x
x
t
+
3
u
u
x
=
2
u
x
u
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x
+
u
u
x
x
x
.
{\displaystyle u_{t}+2\kappa u_{x}-u_{xxt}+3uu_{x}=2u_{x}u_{xx}+uu_{xxx}.\,}
1993年卡馬薩和霍爾姆以此偏微分方程模擬淺水波[ 1] ,
其中κ是大於0的參數。
卡馬薩-霍爾姆方程3D動畫
卡馬薩-霍爾姆方程有行波解[ 2] :
u
2
:=
(
3
/
2
)
∗
c
∗
(
c
−
2
∗
κ
)
(
c
o
s
h
(
(
1
/
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)
∗
(
(
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−
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0
+
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∗
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)
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2
∗
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+
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)
)
{\displaystyle u2:=(3/2)*{\frac {c*(c-2*\kappa )}{(cosh((1/2)*{\sqrt {((c-2*\kappa )/c)}}*(-x-x0+c*t))^{2}*(\kappa +c))}}}
參數:c = 1, x0 = 1, kappa = .3 代人得:
u
(
x
,
t
)
=
.463
c
o
s
h
(
−
.316
∗
x
−
.316
+
.316
∗
t
)
2
{\displaystyle u(x,t)={\frac {.463}{cosh(-.316*x-.316+.316*t)^{2}}}}
Maple 軟件包TWSolution可提供多種行波解[ 3] 。
sech 展開
g
[
2
]
:=
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=
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/
2
)
∗
k
a
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p
a
+
C
5
∗
s
e
c
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(
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1
+
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1
/
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)
∗
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t
(
3
)
∗
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/
4
)
∗
k
a
p
p
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(
3
)
∗
t
)
2
{\displaystyle g[2]:={u(x,t)=-(1/2)*kappa+_{C}5*sech(_{C}1+(1/2)*sqrt(3)*x-(1/4)*kappa*sqrt(3)*t)^{2}}}
g
[
3
]
:=
u
(
x
,
t
)
=
−
(
1
/
2
)
∗
k
a
p
p
a
+
C
5
∗
s
e
c
h
(
C
1
−
(
1
/
2
)
∗
s
q
r
t
(
3
)
∗
x
+
(
1
/
4
)
∗
k
a
p
p
a
∗
s
q
r
t
(
3
)
∗
t
)
2
{\displaystyle g[3]:={u(x,t)=-(1/2)*kappa+_{C}5*sech(_{C}1-(1/2)*sqrt(3)*x+(1/4)*kappa*sqrt(3)*t)^{2}}}
g
[
4
]
:=
u
(
x
,
t
)
=
C
4
+
(
−
(
3
/
2
)
∗
C
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−
(
3
/
4
)
∗
k
a
p
p
a
)
∗
s
e
c
h
(
C
1
+
(
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/
2
∗
I
)
∗
s
q
r
t
(
3
)
∗
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−
(
1
/
4
∗
I
)
∗
k
a
p
p
a
∗
s
q
r
t
(
3
)
∗
t
)
2
{\displaystyle g[4]:={u(x,t)=_{C}4+(-(3/2)*_{C}4-(3/4)*kappa)*sech(_{C}1+(1/2*I)*sqrt(3)*x-(1/4*I)*kappa*sqrt(3)*t)^{2}}}
g
[
5
]
:=
u
(
x
,
t
)
=
C
4
+
(
−
(
3
/
2
)
∗
C
4
−
(
3
/
4
)
∗
k
a
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p
a
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∗
s
e
c
h
(
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1
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/
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∗
I
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(
3
)
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x
+
(
1
/
4
∗
I
)
∗
k
a
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p
a
∗
s
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t
(
3
)
∗
t
)
2
{\displaystyle g[5]:={u(x,t)=_{C}4+(-(3/2)*_{C}4-(3/4)*kappa)*sech(_{C}1-(1/2*I)*sqrt(3)*x+(1/4*I)*kappa*sqrt(3)*t)^{2}}}
g
[
6
]
:=
u
(
x
,
t
)
=
−
(
C
3
−
4
∗
C
3
∗
C
2
2
+
2
∗
k
a
p
p
a
∗
C
2
)
/
(
C
2
∗
(
3
+
4
∗
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2
2
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)
+
24
∗
C
2
∗
(
2
∗
C
3
+
k
a
p
p
a
∗
C
2
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∗
s
e
c
h
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1
+
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x
+
C
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∗
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)
2
/
(
16
∗
C
2
4
−
9
)
{\displaystyle g[6]:={u(x,t)=-(_{C}3-4*_{C}3*_{C}2^{2}+2*kappa*_{C}2)/(_{C}2*(3+4*_{C}2^{2}))+24*_{C}2*(2*_{C}3+kappa*_{C}2)*sech(_{C}1+_{C}2*x+_{C}3*t)^{2}/(16*_{C}2^{4}-9)}}
Camassa Holm equation traveling wave sech plot5
Camassa Holm equation traveling wave sech plot4
Camassa Holm equation traveling wave sech plot6
exp 展開
g
[
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:=
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−
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9
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∗
s
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(
3
)
∗
C
3
−
(
1
/
3
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a
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+
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5
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e
x
p
(
C
1
−
s
q
r
t
(
3
)
∗
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+
C
3
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)
{\displaystyle g[2]:={u(x,t)=-(1/9)*sqrt(3)*_{C}3-(1/3)*kappa+_{C}5*exp(_{C}1-sqrt(3)*x+_{C}3*t)}}
g
[
3
]
:=
u
(
x
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=
(
1
/
9
)
∗
s
q
r
t
(
3
)
∗
C
3
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(
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/
3
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(
C
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+
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(
3
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{\displaystyle g[3]:={u(x,t)=(1/9)*sqrt(3)*_{C}3-(1/3)*kappa+_{C}5*exp(_{C}1+sqrt(3)*x+_{C}3*t)}}
g
[
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s
q
r
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3
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−
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(
e
x
p
(
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/
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)
∗
s
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(
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)
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+
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)
)
3
{\displaystyle g[5]:={u(x,t)=-(1/3)*sqrt(3)*_{C}3-(1/3)*kappa+_{C}7*(exp(_{C}1-(1/3)*sqrt(3)*x+_{C}3*t))^{3}}}
Camassa Holm equation traveling wave exp plot2
Camassa Holm equation traveling wave exp plot3
Camassa Holm equation traveling wave exp plot5
csch 展開
g
[
2
]
:=
u
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−
(
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/
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)
∗
k
a
p
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a
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C
5
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c
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c
h
(
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(
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/
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r
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3
)
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/
4
)
∗
k
a
p
p
a
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s
q
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3
)
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2
{\displaystyle g[2]:={u(x,t)=-(1/2)*kappa+_{C}5*csch(_{C}1+(1/2)*sqrt(3)*x-(1/4)*kappa*sqrt(3)*t)^{2}}}
g
[
4
]
:=
u
(
x
,
t
)
=
C
4
+
(
(
3
/
2
)
∗
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4
+
(
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/
4
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k
a
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c
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(
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∗
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∗
k
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p
a
∗
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t
(
3
)
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2
{\displaystyle g[4]:={u(x,t)=_{C}4+((3/2)*_{C}4+(3/4)*kappa)*csch(_{C}1+(1/2*I)*sqrt(3)*x-(1/4*I)*kappa*sqrt(3)*t)^{2}}}
g
[
6
]
:=
u
(
x
,
t
)
=
−
(
C
3
−
4
∗
C
3
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C
2
2
+
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a
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/
(
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+
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)
)
−
24
∗
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2
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(
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+
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a
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2
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∗
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s
c
h
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+
C
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∗
x
+
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t
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2
/
(
16
∗
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2
4
−
9
)
{\displaystyle g[6]:={u(x,t)=-(_{C}3-4*_{C}3*_{C}2^{2}+2*kappa*_{C}2)/(_{C}2*(4*_{C}2^{2}+3))-24*_{C}2*(2*_{C}3+kappa*_{C}2)*csch(_{C}1+_{C}2*x+_{C}3*t)^{2}/(16*_{C}2^{4}-9)}}
Camassa Holm equation traveling wave csch plot2
Camassa Holm equation traveling wave csch plot4
Camassa Holm equation traveling wave csch plot6
sec 展開
g
[
3
]
:=
u
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,
t
)
=
−
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/
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∗
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a
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e
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/
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a
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p
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3
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{\displaystyle g[3]:={u(x,t)=-(1/2)*kappa+_{C}5*sec(_{C}1-(1/2*I)*sqrt(3)*x+(1/4*I)*kappa*sqrt(3)*t)^{2}}}
g
[
5
]
:=
u
(
x
,
t
)
=
C
4
+
(
−
(
3
/
2
)
∗
C
4
−
(
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/
4
)
∗
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e
c
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/
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p
p
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q
r
t
(
3
)
∗
t
)
2
{\displaystyle g[5]:={u(x,t)=_{C}4+(-(3/2)*_{C}4-(3/4)*kappa)*sec(_{C}1-(1/2)*sqrt(3)*x+(1/4)*kappa*sqrt(3)*t)^{2}}}
g
[
6
]
:=
u
(
x
,
t
)
=
(
C
3
+
4
∗
C
3
∗
C
2
2
+
2
∗
k
a
p
p
a
∗
C
2
)
/
(
C
2
∗
(
4
∗
C
2
2
−
3
)
)
−
24
∗
C
2
∗
(
2
∗
C
3
+
k
a
p
p
a
∗
C
2
)
∗
s
e
c
(
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1
+
C
2
∗
x
+
C
3
∗
t
)
2
/
(
16
∗
C
2
4
−
9
)
{\displaystyle g[6]:={u(x,t)=(_{C}3+4*_{C}3*_{C}2^{2}+2*kappa*_{C}2)/(_{C}2*(4*_{C}2^{2}-3))-24*_{C}2*(2*_{C}3+kappa*_{C}2)*sec(_{C}1+_{C}2*x+_{C}3*t)^{2}/(16*_{C}2^{4}-9)}}
JacobiSN 展開
g
[
3
]
:=
u
(
x
,
t
)
=
(
1
/
9
∗
I
)
∗
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(
3
)
∗
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4
−
(
1
/
3
)
∗
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a
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p
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+
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6
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i
n
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C
2
−
I
∗
s
q
r
t
(
3
)
∗
x
+
C
4
∗
t
)
{\displaystyle g[3]:={u(x,t)=(1/9*I)*sqrt(3)*_{C}4-(1/3)*kappa+_{C}6*sin(_{C}2-I*sqrt(3)*x+_{C}4*t)}}
g
[
4
]
:=
u
(
x
,
t
)
=
−
(
2
/
9
∗
I
)
∗
s
q
r
t
(
3
)
∗
C
4
−
(
1
/
2
)
∗
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/
3
)
∗
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a
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+
C
7
∗
s
i
n
(
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2
+
(
1
/
2
∗
I
)
∗
s
q
r
t
(
3
)
∗
x
+
C
4
∗
t
)
2
{\displaystyle g[4]:={u(x,t)=-(2/9*I)*sqrt(3)*_{C}4-(1/2)*_{C}7-(1/3)*kappa+_{C}7*sin(_{C}2+(1/2*I)*sqrt(3)*x+_{C}4*t)^{2}}}
Camassa Holm equation traveling wave Jacobish plot4
{\displaystyle }
{\displaystyle }
{\displaystyle }
{\displaystyle }
{\displaystyle }
^ Camassa & Holm 1993
^ Beals, Sattinger & Szmigielski 1999
^ Inna Shingareva, Carlos Lizárraga-Celaya,Solving Nonlinear Partial Differential Equations with Maple Page 27-35
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Eckhardt, Jonathan; Teschl, Gerald , On the isospectral problem of the dispersionless Camassa-Holm equation, Adv. Math. 235 (1), 2013, 235 (1): 469–495, arXiv:1205.5831 , doi:10.1016/j.aim.2012.12.006
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