PDE uniqueness

renegade05

Full Member
Joined
Sep 10, 2010
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260
Hello there!

I am having problems with the following question:

\(\displaystyle x u_x+y u_y - 3u=0\)
With \(\displaystyle u(x,1)=\phi(x)\)

I solved it using method of characteristics to find the solution to be:

\(\displaystyle u(x,y) = \phi(\frac{x}{y}) y^3\)

With the data curve being \(\displaystyle y=1\) (red line)
And characteristic base curves being \(\displaystyle y=\frac{1}{\xi}x\) (black lines)

So plotting this with different values of \(\displaystyle \xi\) we get the following idea:

save.jpg

Now the question asks to:
"explain how the problem needs to be restricted in order to have a unique solution."

So this is where I am stuck. Everything looks good to me - so what am I missing? What are these restrictions?

THANKS!
 
Hi,
Lets back up a step or two. By the (present) method of characteristics we have
x = a es
y = b es
u = c e3s
putting these together we have
(x/y) = d
which is your equation \(\displaystyle y=\frac{1}{\xi}x\) with d = \(\displaystyle \xi\) = a/b. From that, letting
\(\displaystyle \alpha_{\lambda} (\frac{x}{y})^{\lambda} = 1\)
we have a solution of
u(x,y) = \(\displaystyle \alpha_{\lambda} (\frac{x}{y})^{\lambda} y^3\)
where the a, b, and c have been absorbed into the \(\displaystyle \alpha_{\lambda}\). Since this is a homogenous equation, the full solution is the 'sum' of the general solutions, so
u(x,y) = \(\displaystyle \Sigma_{\lambda} \alpha_{\lambda} (\frac{x}{y})^{\lambda} y^3\)
Since
u(x,1) = \(\displaystyle \Sigma_{\lambda} \alpha_{\lambda} x^{\lambda} = \phi(x)\)
a further restriction is that \(\displaystyle \phi(x)\) be expressible as such.

For example \(\displaystyle \phi(x)\) is infinitely differentiable in some neighborhood of x=0 so that
u(x,y) = \(\displaystyle \Sigma_{0}^{\infty}\space \alpha_{n} x^{n} y^{3-n}\)
and
\(\displaystyle \alpha_{n} = \frac{\phi^{(n)}(0)}{n!}\).

BTW: The old method of characteristics (separation of variables) which I learned gives the same answer, i.e. let u = X(x) Y(y) and go from there.
 
Hi,
Lets back up a step or two. By the (present) method of characteristics we have
x = a es
y = b es
u = c e3s
putting these together we have
(x/y) = d
which is your equation \(\displaystyle y=\frac{1}{\xi}x\) with d = \(\displaystyle \xi\) = a/b. From that, letting
\(\displaystyle \alpha_{\lambda} (\frac{x}{y})^{\lambda} = 1\)
we have a solution of
u(x,y) = \(\displaystyle \alpha_{\lambda} (\frac{x}{y})^{\lambda} y^3\)
where the a, b, and c have been absorbed into the \(\displaystyle \alpha_{\lambda}\). Since this is a homogenous equation, the full solution is the 'sum' of the general solutions, so
Since this is a linear homogeneous equation.

u(x,y) = \(\displaystyle \Sigma_{\lambda} \alpha_{\lambda} (\frac{x}{y})^{\lambda} y^3\)
Since
u(x,1) = \(\displaystyle \Sigma_{\lambda} \alpha_{\lambda} x^{\lambda} = \phi(x)\)
a further restriction is that \(\displaystyle \phi(x)\) be expressible as such.

For example \(\displaystyle \phi(x)\) is infinitely differentiable in some neighborhood of x=0 so that
u(x,y) = \(\displaystyle \Sigma_{0}^{\infty}\space \alpha_{n} x^{n} y^{3-n}\)
and
\(\displaystyle \alpha_{n} = \frac{\phi^{(n)}(0)}{n!}\).

BTW: The old method of characteristics (separation of variables) which I learned gives the same answer, i.e. let u = X(x) Y(y) and go from there.
 
HMMMMMMMMMMMMM..... This is what I did:

\(\displaystyle \frac{dx}{x}=\frac{dy}{y}=\frac{du}{3u}\)
\(\displaystyle \frac{dx}{ds}=x \qquad x(0)=\xi \qquad x(s)=\xi e^s\)
\(\displaystyle \frac{dy}{ds}=y \qquad y(0)=1 \qquad y(s)=e^s\)
\(\displaystyle \frac{du}{ds}=3u \qquad u(0)=\phi(\xi) \qquad u(s)=\phi(\xi)e^{3s}\)

Eliminating \(\displaystyle \xi \enspace and \enspace s\):

\(\displaystyle \xi=\frac{x}{e^s}=\frac{x}{y}\)
\(\displaystyle s=ln(y)\)

Thus:
\(\displaystyle u(x,y)=\phi(\frac{x}{y})y^3\)

Then my restriction was because the data curve is at y=1 and the base curves are \(\displaystyle y=\frac{x}{\xi}\) then all the characteristic base curves cross at (0,0), but have different values of u(x,y)- therefore there is a singularity. So we need to restrict y>0.

Is this wrong? If yes, I am still not sure of the reasoning and to what restrictions I must make. THANKS!
 
If we let
\(\displaystyle \phi(x) = x\)
then what you have is
u(x,y) = (x/y) y3 = x y2
x ux(x,y) = u(x,y)
y uy(x,y) = 2 u(x,y)
and
x ux + y uy - 3 U = 0
and u is infinitely (partial) differential is all closed neighborhoods in the real plane. So there is no need for the y>0 restriction in this case. But, putting the y>0 together with \(\displaystyle \phi(\frac{x}{y})\), maybe the restriction is
"If \(\displaystyle \phi\) has at pole of order more than 3 at x=0, y must be restricted to y>0."

Now that you have pointed it out, also note that the solution I gave can also be written as
\(\displaystyle u(x,y) = \Sigma_0^{\infty}\space \alpha_n\space (\frac{x}{y})^n y^3 = \phi(\frac{x}{y}) y^3\)
 
If we let
\(\displaystyle \phi(x) = x\)
then what you have is
u(x,y) = (x/y) y3 = x y2
x ux(x,y) = u(x,y)
y uy(x,y) = 2 u(x,y)
and
x ux + y uy - 3 U = 0
and u is infinitely (partial) differential is all closed neighborhoods in the real plane. So there is no need for the y>0 restriction in this case. But, putting the y>0 together with \(\displaystyle \phi(\frac{x}{y})\), maybe the restriction is
"If \(\displaystyle \phi\) has at pole of order more than 3 at x=0, y must be restricted to y>0."

Now that you have pointed it out, also note that the solution I gave can also be written as
\(\displaystyle u(x,y) = \Sigma_0^{\infty}\space \alpha_n\space (\frac{x}{y})^n y^3 = \phi(\frac{x}{y}) y^3\)

So I am confused - what is the restriction?
 
So I am confused - what is the restriction?

I would say something like "If [FONT=MathJax_Math]ϕ[/FONT] has at pole of order more than 3 at x=0, y must be restricted to y\(\displaystyle \ge \epsilon \gt 0\)." but I'm not sure of that. I would appreciate it if someone else could chime in here or if you would check with your instructor and post the answer here.
 
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