Computing the Integral of a Harmonic Function with Boundary Conditions.

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In summary, the conversation discusses computing the integral $\int_{x^2+y^2 \leq 4} v(x,y) dxdy$, where $v$ is a harmonic function in a given space $L$ with $\Omega \subset L$ and $(0,0)$ belonging to $\Omega$. The conversation explores different methods, including the second version of the mean value theorem, to compute the integral. Ultimately, it is determined that the integral can be computed using the second version of the mean value theorem, and the answer is $\frac{4 \pi}{3}$.
  • #1
evinda
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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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  • #2
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?
 
  • #3
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?
 
  • #4
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?
 
  • #5
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)
 
  • #6
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?
 
  • #7
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)
 
  • #8
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)
 
  • #9
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)
 

FAQ: Computing the Integral of a Harmonic Function with Boundary Conditions.

What is an integral?

An integral is a mathematical concept that represents the area under a curve in a graph. It is used to find the cumulative effect of continuously changing quantities and is an essential tool in calculus.

How do I compute an integral?

To compute an integral, you can use various techniques such as the Fundamental Theorem of Calculus, substitution, and integration by parts. The specific method used will depend on the complexity of the function being integrated.

What is the difference between indefinite and definite integrals?

An indefinite integral is the most general form of an integral and represents the antiderivative of a function. It does not have any specified limits of integration. On the other hand, a definite integral has specific upper and lower limits of integration and gives a numerical value.

Can integrals be solved analytically?

In some cases, integrals can be solved analytically, meaning they can be expressed as an exact algebraic expression. However, there are many functions for which an analytical solution does not exist, and numerical methods are used to approximate the integral.

What are some real-world applications of integrals?

Integrals are used in many fields, including physics, engineering, and economics, to model and analyze real-world phenomena. They are used to calculate areas, volumes, and rates of change, making them vital in solving problems related to motion, growth, and optimization.

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