特里忒蔡卡方程 (Tritzeica equation)是一个最早由罗马尼亚数学家George Tritzeica在1907年在微分几何领域研究的非线性偏微分方程[ 1] 常见于微分几何学和物理学的非线性偏微分方程:[ 2]
罗马尼亚数学家George Tritzeica
u
x
y
=
e
x
p
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u
x
,
y
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−
e
x
p
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−
2
∗
u
x
,
y
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{\displaystyle u_{xy}=exp(u_{x,y})-exp(-2*u_{x,y})}
作变换
w
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=
e
x
p
(
u
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)
{\displaystyle w(x,y)=exp(u(x,y))}
得
w
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y
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x
∗
w
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−
w
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x
∗
w
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y
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w
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3
+
1
=
0
{\displaystyle w(x,y)_{y,x}*w(x,y)-w(x,y)_{x}*w(x,y)_{y}-w(x,y)^{3}+1=0}
求得行波解,再用反代换
u
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x
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=
l
n
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w
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)
{\displaystyle u(x,y)=ln(w(x,y))}
即得 原方程的行波解。
解析解
u
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∗
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3
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c
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2
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{\displaystyle u(x,y)=ln(-1/2-(1/2*I)*{\sqrt {(}}3)+(3/4+(3/4*I)*{\sqrt {(}}3))*csc(_{C}1+_{C}2*x+(3/4)*(1/2+(1/2*I)*{\sqrt {(}}3))*y/_{C}2)^{2})}
u
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,
y
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=
l
n
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−
1
/
2
−
(
1
/
2
∗
I
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∗
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3
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+
(
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/
4
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(
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/
4
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I
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∗
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3
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∗
s
e
c
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C
1
+
C
2
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x
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(
3
/
4
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∗
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2
+
(
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∗
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3
)
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∗
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/
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)
2
)
{\displaystyle u(x,y)=ln(-1/2-(1/2*I)*{\sqrt {(}}3)+(3/4+(3/4*I)*{\sqrt {(}}3))*sec(_{C}1+_{C}2*x+(3/4)*(1/2+(1/2*I)*{\sqrt {(}}3))*y/_{C}2)^{2})}
u
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=
l
n
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−
1
/
2
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(
1
/
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∗
I
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∗
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3
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+
(
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/
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−
(
3
/
4
∗
I
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∗
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3
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∗
c
s
c
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C
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+
C
2
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x
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/
4
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∗
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1
/
2
−
(
1
/
2
∗
I
∗
(
3
)
)
∗
y
/
C
2
)
2
)
{\displaystyle u(x,y)=ln(-1/2+(1/2*I)*{\sqrt {(}}3)+(3/4-(3/4*I)*{\sqrt {(}}3))*csc(_{C}1+_{C}2*x+(3/4)*(1/2-(1/2*I*{\sqrt {(}}3))*y/_{C}2)^{2})}
u
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x
,
y
)
=
l
n
(
1
/
4
−
(
1
/
4
∗
I
)
∗
(
3
)
+
(
−
3
/
4
+
(
3
/
4
∗
I
)
∗
(
3
)
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∗
c
o
t
h
(
C
1
+
C
2
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x
+
(
3
/
4
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∗
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−
1
/
2
+
(
1
/
2
∗
I
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∗
s
q
r
t
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3
)
)
∗
y
/
C
2
)
2
)
{\displaystyle u(x,y)=ln(1/4-(1/4*I)*{\sqrt {(}}3)+(-3/4+(3/4*I)*{\sqrt {(}}3))*coth(_{C}1+_{C}2*x+(3/4)*(-1/2+(1/2*I)*sqrt(3))*y/_{C}2)^{2})}
u
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x
,
y
)
=
l
n
(
1
/
4
−
(
1
/
4
∗
I
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∗
(
3
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+
(
−
3
/
4
+
(
3
/
4
∗
I
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∗
(
3
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∗
t
a
n
h
(
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/
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/
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+
(
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/
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∗
I
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∗
s
q
r
t
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3
)
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∗
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/
C
2
)
2
)
{\displaystyle u(x,y)=ln(1/4-(1/4*I)*{\sqrt {(}}3)+(-3/4+(3/4*I)*{\sqrt {(}}3))*tanh(_{C}1+_{C}2*x+(3/4)*(-1/2+(1/2*I)*sqrt(3))*y/_{C}2)^{2})}
u
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x
,
y
)
=
l
n
(
1
/
4
−
(
1
/
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∗
I
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∗
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3
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+
(
3
/
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−
(
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/
4
∗
I
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∗
(
3
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∗
c
o
t
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+
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/
4
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∗
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−
(
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/
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∗
I
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∗
(
3
)
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∗
y
/
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)
2
)
{\displaystyle u(x,y)=ln(1/4-(1/4*I)*{\sqrt {(}}3)+(3/4-(3/4*I)*{\sqrt {(}}3))*cot(_{C}1+_{C}2*x+(3/4)*(1/2-(1/2*I)*{\sqrt {(}}3))*y/_{C}2)^{2})}
u
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x
,
y
)
=
l
n
(
1
/
4
−
(
1
/
4
∗
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∗
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3
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+
(
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/
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(
3
/
4
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I
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∗
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3
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∗
t
a
n
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C
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+
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x
+
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3
/
4
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∗
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1
/
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−
(
1
/
2
∗
I
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∗
(
3
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)
∗
y
/
C
2
)
2
)
{\displaystyle u(x,y)=ln(1/4-(1/4*I)*{\sqrt {(}}3)+(3/4-(3/4*I)*{\sqrt {(}}3))*tan(_{C}1+_{C}2*x+(3/4)*(1/2-(1/2*I)*{\sqrt {(}}3))*y/_{C}2)^{2})}
w
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x
,
y
)
=
(
8
/
3
)
∗
C
4
2
−
(
1
/
3
)
∗
R
o
o
t
O
f
(
64
∗
C
4
6
+
27
−
24
∗
C
4
4
∗
Z
−
6
∗
C
4
2
∗
Z
2
+
Z
3
)
−
4
∗
C
4
2
∗
J
a
c
o
b
i
D
N
(
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+
(
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/
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x
+
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t
,
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/
2
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∗
R
o
o
t
O
f
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−
R
o
o
t
O
f
(
64
∗
C
4
6
+
27
−
24
∗
C
4
4
∗
Z
−
6
∗
C
4
2
∗
Z
2
+
Z
3
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+
Z
2
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/
C
4
)
2
{\displaystyle w(x,y)=(8/3)*_{C}4^{2}-(1/3)*RootOf(64*_{C}4^{6}+27-24*_{C}4^{4}*_{Z}-6*_{C}4^{2}*_{Z}^{2}+_{Z}^{3})-4*_{C}4^{2}*JacobiDN(_{C}2+(1/2)*_{C}4*x+_{C}4*t,(1/2)*RootOf(-RootOf(64*_{C}4^{6}+27-24*_{C}4^{4}*_{Z}-6*_{C}4^{2}*_{Z}^{2}+_{Z}^{3})+_{Z}^{2})/_{C}4)^{2}}
行波图
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
Tritzeica equation traveling wave plot
参考文献
^ G. Tzitz´eica, “Geometric infinitesimale-sur une nouvelle classes
de surfaces,”Comptes Rendus de l’Acad´emie des Sciences, vol. 144,pp. 1257–1259, 1907.
^ Andrei D. Polyanin,Valentin F. Zaitsev, HANDBOOK OF NONLINEAR PARTIAL DIFFERENTIAL EQUATIONS, SECOND EDITION p540-542 CRC PRESS
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