Question 16.13: The Laplace equation ∇²u = uxx + uyy = 0 is defined over th...
The Laplace equation \nabla^2 u=u_{x x}+u_{y y}=0 is defined over the following triangular region, {x = 0; y = 0; x + y = 5}. The following boundary conditions are prescribed
i) u = 0 over the edges x = 0, y = 0
ii) u = 25 − x² − y² at the edge x + y = 5
Find the values of u(x, y) at the nodal points of the square region with mess length 1, with the aid of Gauss–Seidel method till the last two iterations have same values up to three decimal points.
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Since we have to compute the values of u(x, y) at the nodal points of the triangular region {x = 0; y = 0; x + y = 5} with mess length 1. Therefore, mesh points are given by
\begin{aligned} &x_0=0, x_1=1, x_2=2, x_3=3, x_4=4, x_5=5 \\ &y_0=0, y_1=1, y_2=2, y_3=3, y_4=4, y_5=5 \end{aligned}
Let u_{i j}=u\left(x_i, y_j\right) . We have to compute the values of u_{11}, u_{21}, u_{31}, u_{12}, u_{22}, u_{13} .
The following boundary conditions are defined
i) u = 0 over the edges x = 0, y = 0
ii) u = 25 − x² − y² at the edge x + y = 5
So, we have
\begin{aligned} &u_{00}=u_{10}=u_{20}=u_{30}=u_{40}=u_{50}=0 \\ &u_{01}=u_{02}=u_{03}=u_{04}=u_{05}=0 \\ &u_{14}=u_{41}=8 \\ &u_{23}=u_{32}=12 \end{aligned}
It is easy to apply standard 5-points formula for calculations at each nodal point to get following equations
\begin{array}{ll} \text { At }(1,1) & u_{21}+u_{12}-4 u_{11}=0 \\ \text { At }(2,1) & u_{31}+u_{11}+u_{22}-4 u_{21}=0 \\ \text { At }(3,1) & u_{21}-4 u_{31}=-20 \\ \text { At }(1,2) & u_{22}+u_{11}+u_{13}-4 u_{12}=0 \\ \text { At }(2,2) & u_{12}+u_{21}-4 u_{22}=-24 \\ \text { At }(1,3) & u_{12}-4 u_{13}=-20 \end{array}
We get following iterations of Gauss–Seidel method for u_{11}, u_{21}, u_{31}, u_{12}, u_{22}, u_{13}
Iteration 1 | |||||
5.000000 | 6.000000 | 0.000000 | 5.000000 | 0.000000 | 0.000000 |
Iteration 2 | |||||
5.687500 | 7.375000 | 2.750000 | 5.687500 | 2.750000 | 0.000000 |
Iteration 3 | |||||
5.902344 | 7.804688 | 3.609375 | 5.902344 | 3.609375 | 1.375000 |
Iteration 4 | |||||
5.969482 | 7.938965 | 3.877930 | 5.969482 | 3.877930 | 1.804688 |
Iteration 5 | |||||
5.990463 | 7.980927 | 3.961853 | 5.990463 | 3.961853 | 1.938965 |
Iteration 6 | |||||
5.997020 | 7.994040 | 3.988079 | 5.997020 | 3.988079 | 1.980927 |
Iteration 7 | |||||
5.999069 | 7.998137 | 3.996275 | 5.999069 | 3.996275 | 1.994040 |
Iteration 8 | |||||
5.999709 | 7.999418 | 3.998836 | 5.999709 | 3.998836 | 1.998137 |
Iteration 9 | |||||
5.999909 | 7.999818 | 3.999636 | 5.999909 | 3.999636 | 1.999418 |
Iteration 10 | |||||
5.999971 | 7.999943 | 3.999887 | 5.999971 | 3.999887 | 1.999818 |
The final solution is given by
u_{11}=2, u_{21}=4, u_{31}=6, u_{12}=4, u_{22}=8, u_{13}=6
Note: The Laplace equation and boundary conditions are symmetrical about the line y = x. So, the problem can also be discussed with following symmetry consideration
u_{21}=u_{12} \text { and } u_{31}=u_{13}
