Laplace and Poisson's equation.

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In summary, for v=\ln( r), we can see that for a disk centered at (x_0,y_0), the Laplacian is equal to zero, making v Harmonic. However, for a sphere centered at (x_0,y_0,z_0), the Laplacian is equal to \frac{1}{r^2}, making v not Harmonic. This is because the Laplacian is defined differently for two and three dimensions, resulting in different values for the Laplacian of v in each case.
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yungman
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Homework Statement



I want to verify for [itex]v=\ln( r)[/itex], that

a)[itex]\nabla^2 v=0[/itex] for [itex]v[/itex] on a disk center at [itex](x_0,y_0)[/itex]. Therefore [itex]v[/itex] is Harmonic.

b)[itex]\nabla^2 v=\frac{1}{r^2}[/itex] for [itex]v[/itex] on a sphere center at [itex](x_0,y_0,z_0)[/itex]. Therefore [itex]v[/itex] is not Harmonic.

The Attempt at a Solution



a) For circular disk, [itex]v=\frac{1}{2}\ln[(x-x_0)^2+(y-y_0)^2][/itex]
[tex]\nabla v=\frac{\hat x (x-x_0)+\hat y(y-y_0)}{[(x-x_0)^2+(y-y_0)^2]^2}[/tex]
[tex]\nabla^2 v=\nabla\cdot\nabla v=\frac{[(y-y_0)^2-(x-x_0)^2]+[(x-x_0)^2-(y-y_0)^2]}{[(x-x_0)^2+(y-y_0)^2]^2}[/tex]=0
b)For a sphere, [itex]v=\frac{1}{2}\ln[(x-x_0)^2+(y-y_0)^2+(z-z_0)^2][/itex]
[tex]\nabla v=\frac{\hat x (x-x_0)+\hat y(y-y_0)+\hat z(z-z_0)^2}{[(x-x_0)^2+(y-y_0)^2+(z-z_0)^2]^2}[/tex]
[tex]\nabla^2 v=\nabla\cdot\nabla v=\frac{[(y-y_0)^2+(z-z_0)^2-(x-x_0)^2]+[(x-x_0)^2+(z-z_0)^2-(y-y_0)^2]+[(x-x_0)^2+(y-y_0)^2-(z-z_0)^2]}{[(x-x_0)^2+(y-y_0)^2+(z-z_0)^2]^2]} [/tex]
[tex]\Rightarrow\;\nabla^2 v=\frac{(x-x_0)^2+(y-y_0)^2+(z-z_0)^2}{[(x-x_0)^2+(y-y_0)^2+(z-z_0)^2]^2]}=\frac{1}{r^2}[/tex]So [itex]v[/itex] is Harmonic only for a two dimension disk, not in three dimension sphere.
 
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  • #2
This is because the Laplace operator, or the Laplacian, is defined differently for two and three dimensions. In two dimensions, the Laplacian is equal to the sum of the second partial derivatives with respect to the two variables, while in three dimensions, it is equal to the sum of the second partial derivatives with respect to the three variables. Therefore, in three dimensions, the Laplacian of v is not equal to zero, making v not Harmonic.
 

FAQ: Laplace and Poisson's equation.

What is Laplace's equation?

Laplace's equation is a partial differential equation that describes the distribution of a scalar field in space. It is named after the French mathematician Pierre-Simon Laplace and is commonly used in physics, engineering, and other scientific fields.

What is Poisson's equation?

Poisson's equation is a partial differential equation that relates the distribution of a scalar field to its sources. It is named after the French mathematician Siméon Denis Poisson and is often used in electrostatics, fluid mechanics, and other areas of physics and engineering.

What is the difference between Laplace's and Poisson's equations?

Laplace's and Poisson's equations are similar in that they both describe the distribution of a scalar field. However, the main difference is that Laplace's equation assumes that the sources of the field are zero, while Poisson's equation takes into account non-zero sources.

What are some real-world applications of Laplace's and Poisson's equations?

Laplace's and Poisson's equations have a wide range of applications in various fields. Some examples include determining the electric potential in a circuit, modeling fluid flow in pipes, and predicting the temperature distribution in a heated object.

What are the boundary conditions for Laplace's and Poisson's equations?

The boundary conditions for Laplace's and Poisson's equations depend on the specific problem being solved. However, in general, they require the scalar field and its derivatives to be continuous at the boundaries of the region being studied.

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