Laplace equation on a semi infinite slab

In summary, the conversation revolved around a problem involving partial derivatives and boundary conditions. The given equations were \frac{\partial^2u}{\partial x^2}(x,y)+\frac{\partial^2u}{\partial y^2}(x,y)=0 and \ddot{X}-\mu X=0 and \ddot{Y}+\mu Y=0. The solution involved finding the coefficients A_0 and A_r and using them to solve for u(x,y). It was also mentioned that the A coefficients were all equal to 1.
  • #1
bobred
173
0

Homework Statement


Could someone check my work plaese.
[tex]\frac{\partial^2u}{\partial x^2}(x,y)+\frac{\partial^2u}{\partial y^2}(x,y)=0[/tex]

[tex](0<x<1, 0<y)[/tex]

[tex]\frac{\partial u}{\partial x}(0,y)=\frac{\partial u}{\partial y}(1,y)=0[/tex]

[tex]u(x,y)\rightarrow k[/tex] as [tex]y\rightarrow\infty[/tex]

[tex]u(x,0)=f(x)[/tex] [tex](0\leqx\leq1)[/tex]

Homework Equations


[tex]\ddot{X}-\mu X=0[/tex] and [tex]\ddot{Y}+\mu Y=0[/tex], [tex]\mu = k^2[/tex] and [tex]k=\pi r[\tex]

[tex]X(x)=A \cos(kx)+B \sin(kx)[/tex] so [tex]\dot{X}=-Ak\sin(kx)+Bk\cos(kx)[/tex]

With the boundary conditions we have [tex]X_r(x)=A_r \cos(r\pi x)[/tex]

[tex]\ddot{Y}+\mu Y=0[/tex] gives [tex]Y(y)=Ce^{r\pi y}+De^{-r\pi y}[/tex] with the boundary conditions and setting C=0, [tex]Y(y)=De^{-r\pi y}[/tex]

The Attempt at a Solution



So we have [tex]u(x,y)=A_0+\sum^\infty _{r=1} {A_r\cos(r\pi x)e^{-r\pi y}}[/tex]

[tex]u(x,0)=f(x)=A_0+\sum^\infty _{r=1} {A_r\cos(r\pi x)[/tex]

[tex]A_0 = \int^1 _0 \cos(r\pi x) dx[/tex] Here r=0 so [tex]A_0 = 1[/tex]

[tex]A_r =2 \int^1 _0 \cos(r\pi x)\cos(r\pi x) dx[/tex] Here I get all A coefficients as 1, is this right?

Thanks
 
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  • #2
Any ideas anyone?
 

1. What is the Laplace equation on a semi infinite slab?

The Laplace equation on a semi infinite slab is a partial differential equation that describes the distribution of a scalar quantity, such as temperature or electric potential, on a semi infinite slab with insulated boundaries. It is a special case of the Laplace equation, which is a fundamental equation in physics and mathematics.

2. What are the boundary conditions for the Laplace equation on a semi infinite slab?

The boundary conditions for the Laplace equation on a semi infinite slab are that the quantity being studied remains constant along the edges of the slab that are parallel to the semi infinite dimension. In other words, the derivative of the quantity with respect to the normal direction must be equal to zero at these boundaries. This represents the fact that there is no flow or change in the quantity at the edges of the slab.

3. How is the Laplace equation on a semi infinite slab solved?

The Laplace equation on a semi infinite slab can be solved using various mathematical techniques, such as separation of variables, Fourier series, or the method of images. These methods involve breaking down the equation into simpler equations that can be solved using standard techniques, and then combining the solutions to obtain a complete solution for the Laplace equation on the semi infinite slab.

4. What are the practical applications of the Laplace equation on a semi infinite slab?

The Laplace equation on a semi infinite slab has many practical applications in physics, engineering, and other fields. It can be used to model heat conduction in materials with insulated boundaries, the distribution of electric potential in a semi infinite region, and fluid flow in porous media. It is also used as a building block for more complex equations and models in these fields.

5. What are the limitations of the Laplace equation on a semi infinite slab?

The Laplace equation on a semi infinite slab is a simplified model that does not take into account certain real-world factors, such as variations in material properties, non-uniform boundary conditions, and three-dimensional effects. Therefore, its solutions may not accurately reflect the behavior of the physical system being studied. Additionally, the Laplace equation on a semi infinite slab is only valid for steady-state problems, meaning that the quantity being studied does not change over time.

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