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What are the basic steps involved in solving a system of equations with Gauss- Seidel method?

Short Answer

Expert verified
Answer: The primary purpose of the Gauss-Seidel method is to iteratively solve systems of linear equations. The main steps involved in solving a system of linear equations using this method include: 1) understanding the given system of linear equations, 2) separating the diagonal, lower, and upper matrices, 3) forming the iterative formula, 4) initializing the starting solution estimates, 5) performing iterations, 6) checking the convergence, and 7) reporting the final solution.

Step by step solution

01

Understand the given system of linear equations

Write down the given system of linear equations in matrix form. The system will be represented as Ax=b, where A is the coefficient matrix, x is the solution vector, and b is the constant vector.
02

Separate the diagonal, lower, and upper matrices

Split the matrix A into three matrices: the diagonal matrix (D), the lower triangular matrix (L), and the upper triangular matrix (U). D contains the diagonal elements of A, L contains the elements below the diagonal, and U has the elements above the diagonal.
03

Form the iterative formula

Form the Gauss-Seidel iterative formula using the inverse of (D+L) matrix and the U matrix. The formula will be in the following format: x^{(k+1)} = (D+L)^{-1} * (b - U * x^{(k)}), where x^{(k)} is the current estimate of the solution and x^{(k+1)} is the updated estimate.
04

Initialize the starting solution estimates

Set an initial estimate for the solution vector x^{(0)}. In most cases, it is common to start with a zero vector. However, any initial guess can be used in the Gauss-Seidel method.
05

Perform iterations

Update the solution vector estimates using the iterative formula obtained in step 3: x^{(k+1)} = (D+L)^{-1} * (b - U * x^{(k)}). Continue updating the solution estimates until a specified convergence criterion is met. Common convergence criteria include a predefined number of iterations or a tolerance for the difference between consecutive estimates.
06

Check the convergence

Check if the sequence of estimates has converged to the true solution within the given tolerance or within the specified number of iterations. If the convergence criterion is not met, continue iterating using the iterative formula until convergence is achieved.
07

Report the final solution

Once the convergence criterion is met, the final estimate x^{(k+1)} of the solution vector is the approximate solution to the given system of linear equations.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Solving System of Linear Equations
The Gauss-Seidel method is an algorithm used for finding the solutions to a system of linear equations, which is one of the fundamental tasks in algebra and an essential tool in various scientific fields. To solve such a system, you usually need to find the values for variables that make all equations hold true simultaneously.

In mathematical terms, if you have equations with variables, the aim is to find the set of values for those variables that satisfy all the equations. This situation is often represented in matrix form as \( Ax = b \) where \( A \) is a square matrix representing the coefficients, \( x \) is a column vector of variables, and \( b \) is the result vector.

The Gauss-Seidel method dives into this matrix equation and employs an iterative approach to zero in on the solution. It starts with an initial guess and improves the solution incrementally until the results are satisfactory—an approach that is particularly useful when dealing with large systems where direct methods like matrix inversion might be computationally expensive or unfeasible.
Iterative Solution Methods
Iterative methods, such as the Gauss-Seidel method, are techniques that progressively improve estimates of the solution to a system of equations through repeated cycles or iterations. Unlike direct methods that aim to solve the system in a finite number of steps, iterative techniques refine the solution until it is close enough to the true answer within an acceptable error margin.

Each iteration of the Gauss-Seidel method involves updating the estimate of the solution vector. Starting from an initial guess, which could be as simple as a zero vector, the method applies the iteration formula derived from the matrix equation to obtain a new and improved estimate. This process is repeated, with each successive estimate hopefully closer to the true solution, demonstrating the core principle of iterative improvement.

The significant advantage of iterative methods is their ability to handle very large systems where other methods struggle due to computational or memory constraints. They are, therefore, often the go-to solution for numerical problems in engineering and computational sciences.
Convergence Criteria
An important concept when using iterative methods like Gauss-Seidel is 'convergence'. Convergence refers to the point at which successive estimates of the solution are close enough to each other and to the true solution that further iterations do not yield significant improvements.

Convergence criteria are the rules that determine whether the iterative process can be halted. This might be a maximum number of iterations allowed, or more commonly, a threshold value for the change in the solution estimates from one iteration to the next. If the difference between successive iterations is less than this threshold, we say the method has 'converged'.

Careful attention to the convergence criteria is vital for ensuring the result is accurate without exhausting computational resources. However, it is also important to note that not all systems will converge using the Gauss-Seidel method. Checking the properties of the matrix \( A \), such as its diagonally dominant nature, can give us insights into whether the method is likely to be successful or not.
Matrix Decomposition
Matrix decomposition is the process of breaking a matrix down into a set of simpler matrices whose product equals the original matrix. In the context of the Gauss-Seidel method, the matrix \( A \) is decomposed into three components: the diagonal matrix \( D \), the lower triangular matrix \( L \), and the upper triangular matrix \( U \).

The importance of this decomposition comes into play when forming the iterative formula. The method leverages the inverted sum of the diagonal and the lower triangular matrix, \((D+L)^{-1}\), to compute the next estimate from the current one. This aspect of the Gauss-Seidel approach reflects the power of matrix decomposition; by simplifying the complex system into more manageable parts, we can employ efficient computation strategies to advance towards a solution.

Understanding matrix decomposition can also yield insights into the nature of linear systems and is a cornerstone of other numerical methods such as QR decomposition or singular value decomposition, each having their unique applications in solving linear systems or in other areas of linear algebra and beyond.

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Most popular questions from this chapter

Consider steady two-dimensional heat transfer in a long solid bar \((k=25 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) of square cross section \((3 \mathrm{~cm} \times 3 \mathrm{~cm})\) with the prescribed temperatures at the top, right, bottom, and left surfaces to be \(100^{\circ} \mathrm{C}, 200^{\circ} \mathrm{C}, 300^{\circ} \mathrm{C}\), and \(500^{\circ} \mathrm{C}\), respectively. Heat is generated in the bar uniformly at a rate of \(\dot{e}=5 \times 10^{6} \mathrm{~W} / \mathrm{m}^{3}\). Using a uniform mesh size \(\Delta x=\Delta y=1 \mathrm{~cm}\) determine \((a)\) the finite difference equations and \((b)\) the nodal temperatures with the Gauss-Seidel iterative method.

Consider a nuclear fuel element \((k=57 \mathrm{~W} / \mathrm{m} \cdot \mathrm{K})\) that can be modeled as a plane wall with thickness of \(4 \mathrm{~cm}\). The fuel element generates \(3 \times 10^{7} \mathrm{~W} / \mathrm{m}^{3}\) of heat uniformly. Both side surfaces of the fuel element are cooled by liquid with temperature of \(80^{\circ} \mathrm{C}\) and convection heat transfer coefficient of \(8000 \mathrm{~W} / \mathrm{m}^{2} \cdot \mathrm{K}\). Using a uniform nodal spacing of \(8 \mathrm{~mm},(a)\) obtain the finite difference equations, \((b)\) determine the nodal temperatures by solving those equations, and (c) compare the surface temperatures of both sides of the fuel element with analytical solution.

Consider transient one-dimensional heat conduction in a plane wall that is to be solved by the explicit method. If both sides of the wall are at specified temperatures, express the stability criterion for this problem in its simplest form.

Consider steady one-dimensional heat conduction in a composite plane wall consisting of two layers \(A\) and \(B\) in perfect contact at the interface. The wall involves no heat generation. The nodal network of the medium consists of nodes 0,1 (at the interface), and 2 with a uniform nodal spacing of \(\Delta x\). Using the energy balance approach, obtain the finite difference formulation of this problem for the case of insulation at the left boundary (node 0 ) and radiation at the right boundary (node 2) with an emissivity of \(\varepsilon\) and surrounding temperature of \(T_{\text {surr }}\)

Starting with an energy balance on a volume element, obtain the two- dimensional transient explicit finite difference equation for a general interior node in rectangular coordinates for \(T(x, y, t)\) for the case of constant thermal conductivity and no heat generation.

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