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Canonical form for elliptic PDE?
Help Deriving the Canonical Form of this Elliptic PDECanonical form for parabolic PDE?Canonical form for hyperbolic PDE?canonical form of parabolic-type PDE involving $exp(x)$ and $ln(x)$Reduction of a quadratic form to a canonical formGreens function for 2d laplace equation with neumann boundary conditionsCanonical form of an elliptic PDECanonical Form (Elliptic Equation)Solving the canonical form of an elliptic PDE [HEAT EQUATION]
$begingroup$
I'm having trouble reducing this elliptic equation to canonical form.
$$fracpartial^2 upartial x^2 + 2fracpartial^2 upartial x partial y + 5fracpartial^2 upartial y^2 + 3fracpartial upartial x + u = 0$$
I know it's elliptic because I checked: $B^2 - AC < 0$,
$$beginalign
A = 1,\
B = 1,\
C = 5,\
B^2 - AC = 1 - (1)(5) = -4 < 0 endalign$$ so it's elliptic.
I think the characteristics are to be found from the equation:
$$xi_x^2 + 2xi_x xi_y + 5xi_y^2 = 0$$
And then I tried to solve for $xi_x/xi_y$ as follows:
$$fracxi_xxi_y = -1 ± fracsqrt(1 - (1)(5)2 =-frac12 ± i$$
$$fracxi_xxi_y = -frac12 ± i =-fracdydx,$$
Trying to solve, I obtained:
$$xi = phi_+x + y$$ where $$phi_+x = -frac12 + i$$
and
$$eta = phi_–x + y$$ where $$phi_–x = -frac12 + i$$
But I'm really not sure where to go from here, or if I'm even on the right track. I'm finding reductions to canonical form really difficult, and now that imaginary numbers are in the mix I'm completely stuck. I appreciate any help. Thanks in advance!
pde
$endgroup$
add a comment |
$begingroup$
I'm having trouble reducing this elliptic equation to canonical form.
$$fracpartial^2 upartial x^2 + 2fracpartial^2 upartial x partial y + 5fracpartial^2 upartial y^2 + 3fracpartial upartial x + u = 0$$
I know it's elliptic because I checked: $B^2 - AC < 0$,
$$beginalign
A = 1,\
B = 1,\
C = 5,\
B^2 - AC = 1 - (1)(5) = -4 < 0 endalign$$ so it's elliptic.
I think the characteristics are to be found from the equation:
$$xi_x^2 + 2xi_x xi_y + 5xi_y^2 = 0$$
And then I tried to solve for $xi_x/xi_y$ as follows:
$$fracxi_xxi_y = -1 ± fracsqrt(1 - (1)(5)2 =-frac12 ± i$$
$$fracxi_xxi_y = -frac12 ± i =-fracdydx,$$
Trying to solve, I obtained:
$$xi = phi_+x + y$$ where $$phi_+x = -frac12 + i$$
and
$$eta = phi_–x + y$$ where $$phi_–x = -frac12 + i$$
But I'm really not sure where to go from here, or if I'm even on the right track. I'm finding reductions to canonical form really difficult, and now that imaginary numbers are in the mix I'm completely stuck. I appreciate any help. Thanks in advance!
pde
$endgroup$
add a comment |
$begingroup$
I'm having trouble reducing this elliptic equation to canonical form.
$$fracpartial^2 upartial x^2 + 2fracpartial^2 upartial x partial y + 5fracpartial^2 upartial y^2 + 3fracpartial upartial x + u = 0$$
I know it's elliptic because I checked: $B^2 - AC < 0$,
$$beginalign
A = 1,\
B = 1,\
C = 5,\
B^2 - AC = 1 - (1)(5) = -4 < 0 endalign$$ so it's elliptic.
I think the characteristics are to be found from the equation:
$$xi_x^2 + 2xi_x xi_y + 5xi_y^2 = 0$$
And then I tried to solve for $xi_x/xi_y$ as follows:
$$fracxi_xxi_y = -1 ± fracsqrt(1 - (1)(5)2 =-frac12 ± i$$
$$fracxi_xxi_y = -frac12 ± i =-fracdydx,$$
Trying to solve, I obtained:
$$xi = phi_+x + y$$ where $$phi_+x = -frac12 + i$$
and
$$eta = phi_–x + y$$ where $$phi_–x = -frac12 + i$$
But I'm really not sure where to go from here, or if I'm even on the right track. I'm finding reductions to canonical form really difficult, and now that imaginary numbers are in the mix I'm completely stuck. I appreciate any help. Thanks in advance!
pde
$endgroup$
I'm having trouble reducing this elliptic equation to canonical form.
$$fracpartial^2 upartial x^2 + 2fracpartial^2 upartial x partial y + 5fracpartial^2 upartial y^2 + 3fracpartial upartial x + u = 0$$
I know it's elliptic because I checked: $B^2 - AC < 0$,
$$beginalign
A = 1,\
B = 1,\
C = 5,\
B^2 - AC = 1 - (1)(5) = -4 < 0 endalign$$ so it's elliptic.
I think the characteristics are to be found from the equation:
$$xi_x^2 + 2xi_x xi_y + 5xi_y^2 = 0$$
And then I tried to solve for $xi_x/xi_y$ as follows:
$$fracxi_xxi_y = -1 ± fracsqrt(1 - (1)(5)2 =-frac12 ± i$$
$$fracxi_xxi_y = -frac12 ± i =-fracdydx,$$
Trying to solve, I obtained:
$$xi = phi_+x + y$$ where $$phi_+x = -frac12 + i$$
and
$$eta = phi_–x + y$$ where $$phi_–x = -frac12 + i$$
But I'm really not sure where to go from here, or if I'm even on the right track. I'm finding reductions to canonical form really difficult, and now that imaginary numbers are in the mix I'm completely stuck. I appreciate any help. Thanks in advance!
pde
pde
asked Jan 28 '14 at 3:18
user114014user114014
175312
175312
add a comment |
add a comment |
2 Answers
2
active
oldest
votes
$begingroup$
The characteristic equation congruent to the general partial equation:
$$Afracpartial^2partial x^2u
+Bfracpartial^2partial x partial yu
+Cfracpartial^2partial y^2u+Dfracpartialpartial xu+Efracpartialpartial yu+Fu=G $$
is:
$$Ay'^2-By'+C=0 text or Agamma^2-Bgamma+C=0$$
This will lead to the below equation if you choose $mathbf s=-gamma_1 x + y$ and $mathbf r = -gamma_2 x + y$
(Where $eta = gamma_1$ and $xi = gamma_2$)
$$left(frac4AC-B^2Aright) fracpartial ^2 upartial s partial r +(eta D+E)fracpartial upartial s +(xi D+E)fracpartial upartial r+Fu(s, r) = G(s,r)$$
If the $(4ac -b^2)$ is positive , same as yours, the answer is the elliptic canonical form of the main equation.
(Wikipedia elliptical resource)
Which the two complex answers are conjugate of each other which means:
$$xi = eta^*$$
We have to change our variables once more(to cancel the unreal part):
$$alpha= xi+eta = 2Reeta$$
$$beta= j(xi-eta) =2Imeta$$
$endgroup$
add a comment |
$begingroup$
The equation
$$a(x,y)u_xx+2b(x,y)u_xy+c(x,y)u_yy=Phi(x,y,u,u_x,u_y)qquad(1)$$
is
$mathbf hyperbolic quad mathrm ifquad b^2-ac>0$,
$mathbf parabolic quad mathrm ifquad b^2-ac=0$,
$mathbf elliptic quad mathrm ifquad b^2-ac<0$.
The charateristic equation
$$a,dy^2-2b,dx,dy+c,dx^2=0qquad(2)$$
splits into two equations
$$a,dy-(b+sqrtb^2-ac),dx=0,qquad(3)$$
$$a,dy-(b-sqrtb^2-ac),dx=0.qquad(4)$$
Elliptic case. Let $quadphi(x,y) + ipsi(x,y)=cquad$ solution of $(3)$ or $(4)$.
Then change variables
$$xi=phi(x,y),quadeta=psi(x,y)$$
reduces equation $(1)$ to canonical form
$$u_xixi+u_etaeta=Phi_1(x,y,u,u_xi,u_eta).$$
In our case $a=1,;b=1,;c=5,; b^2-ac=-4<0$. From $(4)$ we get
$$mathitdy-left( 1-2 iright) , mathitdx=0,$$
$$y-x+2x,i=c,$$
$$xi=y-x,quadeta=2x.qquad(5)$$
Finaly canonical form of equation $u_xx+2u_xy+5u_yy+3u_x+u=0quad$ is
$$4u_xixi+4u_etaeta-3u_xi+6u_eta+u=0$$
or
$$u_xixi+u_etaeta=frac3 u_xi 4-frac3 u_eta2-fracu4.$$
$endgroup$
add a comment |
Your Answer
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2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
The characteristic equation congruent to the general partial equation:
$$Afracpartial^2partial x^2u
+Bfracpartial^2partial x partial yu
+Cfracpartial^2partial y^2u+Dfracpartialpartial xu+Efracpartialpartial yu+Fu=G $$
is:
$$Ay'^2-By'+C=0 text or Agamma^2-Bgamma+C=0$$
This will lead to the below equation if you choose $mathbf s=-gamma_1 x + y$ and $mathbf r = -gamma_2 x + y$
(Where $eta = gamma_1$ and $xi = gamma_2$)
$$left(frac4AC-B^2Aright) fracpartial ^2 upartial s partial r +(eta D+E)fracpartial upartial s +(xi D+E)fracpartial upartial r+Fu(s, r) = G(s,r)$$
If the $(4ac -b^2)$ is positive , same as yours, the answer is the elliptic canonical form of the main equation.
(Wikipedia elliptical resource)
Which the two complex answers are conjugate of each other which means:
$$xi = eta^*$$
We have to change our variables once more(to cancel the unreal part):
$$alpha= xi+eta = 2Reeta$$
$$beta= j(xi-eta) =2Imeta$$
$endgroup$
add a comment |
$begingroup$
The characteristic equation congruent to the general partial equation:
$$Afracpartial^2partial x^2u
+Bfracpartial^2partial x partial yu
+Cfracpartial^2partial y^2u+Dfracpartialpartial xu+Efracpartialpartial yu+Fu=G $$
is:
$$Ay'^2-By'+C=0 text or Agamma^2-Bgamma+C=0$$
This will lead to the below equation if you choose $mathbf s=-gamma_1 x + y$ and $mathbf r = -gamma_2 x + y$
(Where $eta = gamma_1$ and $xi = gamma_2$)
$$left(frac4AC-B^2Aright) fracpartial ^2 upartial s partial r +(eta D+E)fracpartial upartial s +(xi D+E)fracpartial upartial r+Fu(s, r) = G(s,r)$$
If the $(4ac -b^2)$ is positive , same as yours, the answer is the elliptic canonical form of the main equation.
(Wikipedia elliptical resource)
Which the two complex answers are conjugate of each other which means:
$$xi = eta^*$$
We have to change our variables once more(to cancel the unreal part):
$$alpha= xi+eta = 2Reeta$$
$$beta= j(xi-eta) =2Imeta$$
$endgroup$
add a comment |
$begingroup$
The characteristic equation congruent to the general partial equation:
$$Afracpartial^2partial x^2u
+Bfracpartial^2partial x partial yu
+Cfracpartial^2partial y^2u+Dfracpartialpartial xu+Efracpartialpartial yu+Fu=G $$
is:
$$Ay'^2-By'+C=0 text or Agamma^2-Bgamma+C=0$$
This will lead to the below equation if you choose $mathbf s=-gamma_1 x + y$ and $mathbf r = -gamma_2 x + y$
(Where $eta = gamma_1$ and $xi = gamma_2$)
$$left(frac4AC-B^2Aright) fracpartial ^2 upartial s partial r +(eta D+E)fracpartial upartial s +(xi D+E)fracpartial upartial r+Fu(s, r) = G(s,r)$$
If the $(4ac -b^2)$ is positive , same as yours, the answer is the elliptic canonical form of the main equation.
(Wikipedia elliptical resource)
Which the two complex answers are conjugate of each other which means:
$$xi = eta^*$$
We have to change our variables once more(to cancel the unreal part):
$$alpha= xi+eta = 2Reeta$$
$$beta= j(xi-eta) =2Imeta$$
$endgroup$
The characteristic equation congruent to the general partial equation:
$$Afracpartial^2partial x^2u
+Bfracpartial^2partial x partial yu
+Cfracpartial^2partial y^2u+Dfracpartialpartial xu+Efracpartialpartial yu+Fu=G $$
is:
$$Ay'^2-By'+C=0 text or Agamma^2-Bgamma+C=0$$
This will lead to the below equation if you choose $mathbf s=-gamma_1 x + y$ and $mathbf r = -gamma_2 x + y$
(Where $eta = gamma_1$ and $xi = gamma_2$)
$$left(frac4AC-B^2Aright) fracpartial ^2 upartial s partial r +(eta D+E)fracpartial upartial s +(xi D+E)fracpartial upartial r+Fu(s, r) = G(s,r)$$
If the $(4ac -b^2)$ is positive , same as yours, the answer is the elliptic canonical form of the main equation.
(Wikipedia elliptical resource)
Which the two complex answers are conjugate of each other which means:
$$xi = eta^*$$
We have to change our variables once more(to cancel the unreal part):
$$alpha= xi+eta = 2Reeta$$
$$beta= j(xi-eta) =2Imeta$$
edited Dec 30 '17 at 4:48
answered Dec 14 '17 at 19:03
Ali FarbooodiAli Farbooodi
12
12
add a comment |
add a comment |
$begingroup$
The equation
$$a(x,y)u_xx+2b(x,y)u_xy+c(x,y)u_yy=Phi(x,y,u,u_x,u_y)qquad(1)$$
is
$mathbf hyperbolic quad mathrm ifquad b^2-ac>0$,
$mathbf parabolic quad mathrm ifquad b^2-ac=0$,
$mathbf elliptic quad mathrm ifquad b^2-ac<0$.
The charateristic equation
$$a,dy^2-2b,dx,dy+c,dx^2=0qquad(2)$$
splits into two equations
$$a,dy-(b+sqrtb^2-ac),dx=0,qquad(3)$$
$$a,dy-(b-sqrtb^2-ac),dx=0.qquad(4)$$
Elliptic case. Let $quadphi(x,y) + ipsi(x,y)=cquad$ solution of $(3)$ or $(4)$.
Then change variables
$$xi=phi(x,y),quadeta=psi(x,y)$$
reduces equation $(1)$ to canonical form
$$u_xixi+u_etaeta=Phi_1(x,y,u,u_xi,u_eta).$$
In our case $a=1,;b=1,;c=5,; b^2-ac=-4<0$. From $(4)$ we get
$$mathitdy-left( 1-2 iright) , mathitdx=0,$$
$$y-x+2x,i=c,$$
$$xi=y-x,quadeta=2x.qquad(5)$$
Finaly canonical form of equation $u_xx+2u_xy+5u_yy+3u_x+u=0quad$ is
$$4u_xixi+4u_etaeta-3u_xi+6u_eta+u=0$$
or
$$u_xixi+u_etaeta=frac3 u_xi 4-frac3 u_eta2-fracu4.$$
$endgroup$
add a comment |
$begingroup$
The equation
$$a(x,y)u_xx+2b(x,y)u_xy+c(x,y)u_yy=Phi(x,y,u,u_x,u_y)qquad(1)$$
is
$mathbf hyperbolic quad mathrm ifquad b^2-ac>0$,
$mathbf parabolic quad mathrm ifquad b^2-ac=0$,
$mathbf elliptic quad mathrm ifquad b^2-ac<0$.
The charateristic equation
$$a,dy^2-2b,dx,dy+c,dx^2=0qquad(2)$$
splits into two equations
$$a,dy-(b+sqrtb^2-ac),dx=0,qquad(3)$$
$$a,dy-(b-sqrtb^2-ac),dx=0.qquad(4)$$
Elliptic case. Let $quadphi(x,y) + ipsi(x,y)=cquad$ solution of $(3)$ or $(4)$.
Then change variables
$$xi=phi(x,y),quadeta=psi(x,y)$$
reduces equation $(1)$ to canonical form
$$u_xixi+u_etaeta=Phi_1(x,y,u,u_xi,u_eta).$$
In our case $a=1,;b=1,;c=5,; b^2-ac=-4<0$. From $(4)$ we get
$$mathitdy-left( 1-2 iright) , mathitdx=0,$$
$$y-x+2x,i=c,$$
$$xi=y-x,quadeta=2x.qquad(5)$$
Finaly canonical form of equation $u_xx+2u_xy+5u_yy+3u_x+u=0quad$ is
$$4u_xixi+4u_etaeta-3u_xi+6u_eta+u=0$$
or
$$u_xixi+u_etaeta=frac3 u_xi 4-frac3 u_eta2-fracu4.$$
$endgroup$
add a comment |
$begingroup$
The equation
$$a(x,y)u_xx+2b(x,y)u_xy+c(x,y)u_yy=Phi(x,y,u,u_x,u_y)qquad(1)$$
is
$mathbf hyperbolic quad mathrm ifquad b^2-ac>0$,
$mathbf parabolic quad mathrm ifquad b^2-ac=0$,
$mathbf elliptic quad mathrm ifquad b^2-ac<0$.
The charateristic equation
$$a,dy^2-2b,dx,dy+c,dx^2=0qquad(2)$$
splits into two equations
$$a,dy-(b+sqrtb^2-ac),dx=0,qquad(3)$$
$$a,dy-(b-sqrtb^2-ac),dx=0.qquad(4)$$
Elliptic case. Let $quadphi(x,y) + ipsi(x,y)=cquad$ solution of $(3)$ or $(4)$.
Then change variables
$$xi=phi(x,y),quadeta=psi(x,y)$$
reduces equation $(1)$ to canonical form
$$u_xixi+u_etaeta=Phi_1(x,y,u,u_xi,u_eta).$$
In our case $a=1,;b=1,;c=5,; b^2-ac=-4<0$. From $(4)$ we get
$$mathitdy-left( 1-2 iright) , mathitdx=0,$$
$$y-x+2x,i=c,$$
$$xi=y-x,quadeta=2x.qquad(5)$$
Finaly canonical form of equation $u_xx+2u_xy+5u_yy+3u_x+u=0quad$ is
$$4u_xixi+4u_etaeta-3u_xi+6u_eta+u=0$$
or
$$u_xixi+u_etaeta=frac3 u_xi 4-frac3 u_eta2-fracu4.$$
$endgroup$
The equation
$$a(x,y)u_xx+2b(x,y)u_xy+c(x,y)u_yy=Phi(x,y,u,u_x,u_y)qquad(1)$$
is
$mathbf hyperbolic quad mathrm ifquad b^2-ac>0$,
$mathbf parabolic quad mathrm ifquad b^2-ac=0$,
$mathbf elliptic quad mathrm ifquad b^2-ac<0$.
The charateristic equation
$$a,dy^2-2b,dx,dy+c,dx^2=0qquad(2)$$
splits into two equations
$$a,dy-(b+sqrtb^2-ac),dx=0,qquad(3)$$
$$a,dy-(b-sqrtb^2-ac),dx=0.qquad(4)$$
Elliptic case. Let $quadphi(x,y) + ipsi(x,y)=cquad$ solution of $(3)$ or $(4)$.
Then change variables
$$xi=phi(x,y),quadeta=psi(x,y)$$
reduces equation $(1)$ to canonical form
$$u_xixi+u_etaeta=Phi_1(x,y,u,u_xi,u_eta).$$
In our case $a=1,;b=1,;c=5,; b^2-ac=-4<0$. From $(4)$ we get
$$mathitdy-left( 1-2 iright) , mathitdx=0,$$
$$y-x+2x,i=c,$$
$$xi=y-x,quadeta=2x.qquad(5)$$
Finaly canonical form of equation $u_xx+2u_xy+5u_yy+3u_x+u=0quad$ is
$$4u_xixi+4u_etaeta-3u_xi+6u_eta+u=0$$
or
$$u_xixi+u_etaeta=frac3 u_xi 4-frac3 u_eta2-fracu4.$$
answered May 30 '18 at 16:57
Aleksas DomarkasAleksas Domarkas
1,54817
1,54817
add a comment |
add a comment |
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