Solve: $xu_x+(x+y)u_y=1$
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Solve the following PDE
$$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane
$$begin{cases}
a=x\
b=x+y\
c=1
end{cases}Rightarrow begin{cases}
frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
frac{du}{dt}=1iff du=dtiff u=t+c_2
end{cases}$$
How do I solve $?_1$ and what should be my next step?
differential-equations pde
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0
down vote
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Solve the following PDE
$$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane
$$begin{cases}
a=x\
b=x+y\
c=1
end{cases}Rightarrow begin{cases}
frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
frac{du}{dt}=1iff du=dtiff u=t+c_2
end{cases}$$
How do I solve $?_1$ and what should be my next step?
differential-equations pde
add a comment |
up vote
0
down vote
favorite
up vote
0
down vote
favorite
Solve the following PDE
$$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane
$$begin{cases}
a=x\
b=x+y\
c=1
end{cases}Rightarrow begin{cases}
frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
frac{du}{dt}=1iff du=dtiff u=t+c_2
end{cases}$$
How do I solve $?_1$ and what should be my next step?
differential-equations pde
Solve the following PDE
$$xu_x+(x+y)u_y=1$$ when $$u(1,y)=y$$ using method of characteristics and find the projections of the characteristics on the xy plane
$$begin{cases}
a=x\
b=x+y\
c=1
end{cases}Rightarrow begin{cases}
frac{dx}{dt}=xiff frac{dx}{x}=dtiff ln(x)=t+c_1iff x=ke^t\
frac{dy}{dt}=x+yiff frac{dy}{dt}=ke^t+yiff y=(kt+m)e^t\
frac{du}{dt}=1iff du=dtiff u=t+c_2
end{cases}$$
How do I solve $?_1$ and what should be my next step?
differential-equations pde
differential-equations pde
edited Nov 15 at 17:13
asked Nov 15 at 16:27
newhere
838311
838311
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add a comment |
2 Answers
2
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2
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$$xu_x+(x+y)u_y=1$$
You have got the correct system of equation which can be written on this form :
$$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
$$frac{y}{x}-ln|x|=c_1$$
Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
$$u-ln|x|=c_2$$
The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
$$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
where $F$ is an arbitrary function.
This function is determined according to the boundary condition :
$u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$
Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .
$u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$
The final solution is :
$$u(x,y)=frac{y}{x}$$
+ Hi JJacquelin i was just solving it I ended with the same answer..
– Isham
Nov 15 at 18:18
The method you used is Lagrange method?
– newhere
Nov 15 at 22:55
In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
– JJacquelin
Nov 16 at 7:12
add a comment |
up vote
1
down vote
The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
$$
frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
$$
add a comment |
2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
up vote
2
down vote
$$xu_x+(x+y)u_y=1$$
You have got the correct system of equation which can be written on this form :
$$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
$$frac{y}{x}-ln|x|=c_1$$
Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
$$u-ln|x|=c_2$$
The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
$$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
where $F$ is an arbitrary function.
This function is determined according to the boundary condition :
$u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$
Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .
$u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$
The final solution is :
$$u(x,y)=frac{y}{x}$$
+ Hi JJacquelin i was just solving it I ended with the same answer..
– Isham
Nov 15 at 18:18
The method you used is Lagrange method?
– newhere
Nov 15 at 22:55
In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
– JJacquelin
Nov 16 at 7:12
add a comment |
up vote
2
down vote
$$xu_x+(x+y)u_y=1$$
You have got the correct system of equation which can be written on this form :
$$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
$$frac{y}{x}-ln|x|=c_1$$
Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
$$u-ln|x|=c_2$$
The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
$$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
where $F$ is an arbitrary function.
This function is determined according to the boundary condition :
$u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$
Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .
$u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$
The final solution is :
$$u(x,y)=frac{y}{x}$$
+ Hi JJacquelin i was just solving it I ended with the same answer..
– Isham
Nov 15 at 18:18
The method you used is Lagrange method?
– newhere
Nov 15 at 22:55
In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
– JJacquelin
Nov 16 at 7:12
add a comment |
up vote
2
down vote
up vote
2
down vote
$$xu_x+(x+y)u_y=1$$
You have got the correct system of equation which can be written on this form :
$$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
$$frac{y}{x}-ln|x|=c_1$$
Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
$$u-ln|x|=c_2$$
The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
$$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
where $F$ is an arbitrary function.
This function is determined according to the boundary condition :
$u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$
Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .
$u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$
The final solution is :
$$u(x,y)=frac{y}{x}$$
$$xu_x+(x+y)u_y=1$$
You have got the correct system of equation which can be written on this form :
$$frac{dx}{x}=frac{dy}{x+y}=frac{du}{1}=dt$$
Solving $frac{dx}{x}=frac{dy}{x+y}$ gives a first characteristic
$$frac{y}{x}-ln|x|=c_1$$
Solving $frac{dx}{x}=frac{du}{1}$ gives a second characteristic
$$u-ln|x|=c_2$$
The general solution of the PDE is $u-ln|x|=Fleft(frac{y}{x}-ln|x|right)$
$$u(x,y)=ln|x|+Fleft(frac{y}{x}-ln|x|right)$$
where $F$ is an arbitrary function.
This function is determined according to the boundary condition :
$u(1,y)=y=ln|1|+Fleft(frac{y}{1}-ln|1|right)=F(y)$
Thus $F(y)=y$ and as a consequence $Fleft(frac{y}{x}-ln|x|right)=frac{y}{x}-ln|x|$ .
$u(x,y)=ln|x|+left(frac{y}{x}-ln|x|right)$
The final solution is :
$$u(x,y)=frac{y}{x}$$
edited Nov 15 at 18:20
answered Nov 15 at 18:16
JJacquelin
42k21750
42k21750
+ Hi JJacquelin i was just solving it I ended with the same answer..
– Isham
Nov 15 at 18:18
The method you used is Lagrange method?
– newhere
Nov 15 at 22:55
In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
– JJacquelin
Nov 16 at 7:12
add a comment |
+ Hi JJacquelin i was just solving it I ended with the same answer..
– Isham
Nov 15 at 18:18
The method you used is Lagrange method?
– newhere
Nov 15 at 22:55
In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
– JJacquelin
Nov 16 at 7:12
+ Hi JJacquelin i was just solving it I ended with the same answer..
– Isham
Nov 15 at 18:18
+ Hi JJacquelin i was just solving it I ended with the same answer..
– Isham
Nov 15 at 18:18
The method you used is Lagrange method?
– newhere
Nov 15 at 22:55
The method you used is Lagrange method?
– newhere
Nov 15 at 22:55
In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
– JJacquelin
Nov 16 at 7:12
In this very simple case, it is a parametrization invariant form of the Lagrange-Charpit equations. en.wikipedia.org/wiki/Method_of_characteristics
– JJacquelin
Nov 16 at 7:12
add a comment |
up vote
1
down vote
The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
$$
frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
$$
add a comment |
up vote
1
down vote
The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
$$
frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
$$
add a comment |
up vote
1
down vote
up vote
1
down vote
The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
$$
frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
$$
The second equation is a linear inhomogeneous ODE of first order. The standard solution methods apply. For instance, $e^{-t}$ is an integrating factor,
$$
frac{d}{dt}(e^{-t}y(t))=e^{-t}(y'(t)-y(t))=kimplies y(t)=(kt+m)e^t
$$
answered Nov 15 at 16:40
LutzL
53.7k41953
53.7k41953
add a comment |
add a comment |
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