MHB Computing the Integral of a Harmonic Function with Boundary Conditions.

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The discussion focuses on computing the integral of a harmonic function \( v(x,y) \) defined in a domain \( L \) with specific boundary conditions. The integral of interest is \( \int_{x^2+y^2 \leq 4} v(x,y) dx dy \), where \( v \) equals 1 on the boundary of a subdomain \( \Omega \). Participants explore the application of the mean value theorem for harmonic functions, concluding that the integral evaluates to \( 4\pi \) based on the properties of harmonic functions and their behavior at boundaries. The final agreement is that the integral can be computed using the mean value theorem, confirming the result through various approaches. The conversation emphasizes the relationship between boundary values and the integral of harmonic functions.
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Hello! (Wave)

Let $L=\{ (x,y): x^2+y^2<5\}$.
Suppose that we have a function $v(x,y)$ that is harmonic in $L$ and $\Omega \subset L$ an arbitrary space such that $(0,0)$ belongs to that space.
Suppose that $v$ is equal to $1$ at the boundary of $\Omega$.
How can we compute the integral $\int_{x^2+y^2 \leq 4} v(x,y) dxdy$ ?

First I thought that we could use the second version of the mean value theorem. But then we couldn't use the fact that $v$ is equal to $1$ at the boundary of $\Omega$. Could we? If not, could you give me a hint how else we could compute the integral?
 
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Do you know of any relation between the value of a harmonic function on the boundary of a set and its value inside the set?
 
HallsofIvy said:
Do you know of any relation between the value of a harmonic function on the boundary of a set and its value inside the set?

We have the following theorem.

Let $u$ be harmonic in $\Omega$ and $x \in \Omega$ an arbitrary point. Then $\forall \rho \in (0,d)$ where $d=dist(x, \partial{\Omega})$ it holds that $u(x)=\frac{1}{w_n \rho^{n-1}} \int_{|x-\xi|=\rho} u ds$.In order to apply this theorem, we have to assume that $\Omega$ is the unit ball of radius $2$, right?

If so, then we have $u(x,y)=\frac{1}{ w_2 2^{2-1}} \int_{|(x,y)-(\xi_1, \xi_2)|=2} u ds \Rightarrow u(x,y)=\frac{1}{2w_2} \int_{\sqrt{(x- \xi_1)^2+(x- \xi_2)^2}=2} u ds $.

For $(x,y)=(0,0)$ we have that $u(0,0)=\frac{1}{2 w_2} \int_{\xi_1^2+ \xi_2^2=4} u ds$.

Is it right so far? How could we continue?
 
Using polar coordinates we have the following:

$$\int_{x^2+y^2 \leq 4} u(x,y) dx dy=\int_{0}^2 \int_{0}^{2 \pi} u(r \cos{\phi}, r \sin{\phi}) r dr d{\phi}$$

Right?

Can we integrate now as for $\phi$? How can we do so?
Or how else can we continue?
 
evinda said:
Hello! (Wave)

Let $L=\{ (x,y): x^2+y^2<5\}$.
Suppose that we have a function $v(x,y)$ that is harmonic in $L$ and $\Omega \subset L$ an arbitrary space such that $(0,0)$ belongs to that space.
Suppose that $v$ is equal to $1$ at the boundary of $\Omega$.
How can we compute the integral $\int_{x^2+y^2 \leq 4} v(x,y) dxdy$ ?

First I thought that we could use the second version of the mean value theorem. But then we couldn't use the fact that $v$ is equal to $1$ at the boundary of $\Omega$. Could we? If not, could you give me a hint how else we could compute the integral?

Hey evinda! (Smile)

What is $\Omega$?
And can you state the second version of the mean value theorem?

If $\Omega$ is what I suspect it is, the mean value property should help us out. (Happy)
 
I like Serena said:
What is $\Omega$?

It is now given any further. But I think that we have to pick $\Omega=\{ (x,y): x^2+y^2< 2^2\}$, do you agree?

I like Serena said:
And can you state the second version of the mean value theorem?

If $u$ is harmonic in $\Omega$ and $x \in \Omega$ then $u(x)=\frac{n}{w_n r^n} \int_{|x-\xi|\leq r} u d{\xi}, r \in (0,d)$ where $d=dist(x, \partial{\Omega})$.

I have thought the following:

From the mean value theorem we have that $u(x,y)=\frac{1}{4 \pi} \int_{\sqrt{(x- \xi_1)^2+(y- \xi_2)^2}=2} u ds$ and so we get that $u(0,0)=\frac{1}{4 \pi} \int_{\xi_1^2+\xi_2^2=4} 1 ds=1$.

Then from the second version of the mean value theorem we get that $\int_{x^2+y^2 \leq 4} u(x,y) dx dy=4 \pi$.

Is my idea right?
 
evinda said:
It is now given any further. But I think that we have to pick $\Omega=\{ (x,y): x^2+y^2< 2^2\}$, do you agree?

I guess we'll have to assume that yes.
If $u$ is harmonic in $\Omega$ and $x \in \Omega$ then $u(x)=\frac{n}{w_n r^n} \int_{|x-\xi|\leq r} u d{\xi}, r \in (0,d)$ where $d=dist(x, \partial{\Omega})$.

I have thought the following:

From the mean value theorem we have that $u(x,y)=\frac{1}{4 \pi} \int_{\sqrt{(x- \xi_1)^2+(y- \xi_2)^2}=2} u ds$ and so we get that $u(0,0)=\frac{1}{4 \pi} \int_{\xi_1^2+\xi_2^2=4} 1 ds=1$.

Then from the second version of the mean value theorem we get that $\int_{x^2+y^2 \leq 4} u(x,y) dx dy=4 \pi$.

Is my idea right?

The idea is right, but I think we have:
$$v(0,0)=\frac{1}{4 \pi} \oint_{\xi_1^2+\xi_2^2=4} 1 \,ds=1$$
and:
$$v(0,0)=\frac{3}{4 \pi} \iint_{\xi_1^2+\xi_2^2\le4} v(\xi_1,\xi_2)\,d\xi_1\,d\xi_2$$
Thus:
$$\iint_{x^2+y^2 \leq 4} v(x,y)\, dx\, dy=\frac{4 \pi}{3}$$
Don't we? (Wondering)
 
I like Serena said:
I guess we'll have to assume that yes.The idea is right, but I think we have:
$$v(0,0)=\frac{1}{4 \pi} \oint_{\xi_1^2+\xi_2^2=4} 1 \,ds=1$$
and:
$$v(0,0)=\frac{3}{4 \pi} \iint_{\xi_1^2+\xi_2^2\le4} v(\xi_1,\xi_2)\,d\xi_1\,d\xi_2$$
Thus:
$$\iint_{x^2+y^2 \leq 4} v(x,y)\, dx\, dy=\frac{4 \pi}{3}$$
Don't we? (Wondering)

I found the following from the second version of the mean value theorem:

$$u(x,y)=\frac{2}{2 \pi \cdot 4} \int_{\sqrt{(x- \xi_1)^2+(y-\xi_2)^2} \leq 2} u d{\xi}$$

and so $\int_{\xi_1^2+ \xi_2^2 \leq 4} u d{\xi}=4 \pi u(0,0)=4 \pi$

Am I wrong? (Thinking)
 
evinda said:
I found the following from the second version of the mean value theorem:

$$u(x,y)=\frac{2}{2 \pi \cdot 4} \int_{\sqrt{(x- \xi_1)^2+(y-\xi_2)^2} \leq 2} u d{\xi}$$

and so $\int_{\xi_1^2+ \xi_2^2 \leq 4} u d{\xi}=4 \pi u(0,0)=4 \pi$

Am I wrong? (Thinking)

My mistake. You're quite right. (Nod)
 
  • #10
I like Serena said:
My mistake. You're quite right. (Nod)

No problem... Thank you! (Smile)
 

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