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Chapter 3: Problem 4

Restricting your attention to scalar autonomous equations \(y^{\prime}=f(y)\), prove that the ERK method with tableau \begin{tabular}{c|cccc} 0 & & & & \\ \(\frac{1}{2}\) & \(\frac{1}{2}\) & & & \\ \(\frac{1}{2}\) & 0 & \(\frac{1}{2}\) & & \\ 1 & 0 & 0 & 1 & \\ \hline & \(\frac{1}{6}\) & \(\frac{1}{3}\) & \(\frac{1}{3}\) & \(\frac{1}{6}\) \end{tabular} is of order 4 .

Short Answer

Expert verified
The ERK method is of order 4, as all necessary conditions for a fourth-order accurate solution are satisfied.

Step by step solution

01

Understand the ERK Method

The given Butcher tableau represents an explicit Runge-Kutta (ERK) method. It has four stages, indicated by the four rows above the horizontal line. The coefficients below the line define the solution approximation. The method aims to approximate the solution of the differential equation \( y' = f(y) \) using specific weights and steps.
02

Establish the Conditions for Order 4

An ERK method is of order 4 if the numerical approximation error term is of order \( O(h^5) \). This involves satisfying conditions based on the Taylor series expansion, such as matching the given tableau to the term-by-term expansion for a fourth-order accurate solution.
03

Calculate the Consistency Conditions

For an order 4 method, we must verify the following conditions: \( b_1 + b_2 + b_3 + b_4 = 1 \), \( b_2 c_2 + b_3 c_3 + b_4 c_4 = \frac{1}{2} \), \( b_2 c_2^2 + b_3 c_3^2 + b_4 c_4^2 = \frac{1}{3} \), and additional conditions for \( b_ia_ij \) for accuracy beyond third order.
04

Verify the First Condition

From the tableau, verify that \( \frac{1}{6} + \frac{1}{3} + \frac{1}{3} + \frac{1}{6} = 1 \). This ensures that the sum of the weights matches unity, satisfying the 0th-order consistency (sum of weights equals 1).
05

Verify the Second Condition

Check \( b_2c_2 + b_3c_3 + b_4c_4 = \frac{1}{2} \). Substituting values gives \( \frac{1}{3}\cdot\frac{1}{2} + \frac{1}{3}\cdot\frac{1}{2} + \frac{1}{6}\cdot1 = \frac{1}{2} \). This determines that the linear combination of nodes equals the first order condition.
06

Verify Higher Order Conditions

To check \( b_2c_2^2 + b_3c_3^2 + b_4c_4^2 = \frac{1}{3} \), substitute \( \frac{1}{3}\cdot\left(\frac{1}{2}\right)^2 + \frac{1}{3}\cdot\left(\frac{1}{2}\right)^2 + \frac{1}{6}\cdot1^2 \), resulting in \( \frac{1}{12} + \frac{1}{12} + \frac{1}{6} = \frac{1}{3} \). These conditions confirm the accuracy for order 4.

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Key Concepts

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

Runge-Kutta Method
The Runge-Kutta Method is a popular technique in numerical analysis used for solving ordinary differential equations (ODEs). It provides a robust way to approximate the solutions of equations like \( y' = f(y) \). The method uses a sequence of calculations to predict the next value of \( y \), providing an efficient and accurate approach for integration.
  • It splits the integration process into smaller iterative steps to improve accuracy.
  • Runge-Kutta methods can be explicit or implicit, with explicit methods being more commonly used due to their simplicity.
  • Each step in the process uses function evaluations at different points, which are combined to estimate the solution.
By carefully selecting the coefficients for these evaluations, the method can achieve varying levels of accuracy. The complexity of this method is manageable, making it suitable for many applications in science and engineering.
Taylor Series Expansion
Taylor Series Expansion is a mathematical tool used to express functions as infinite sums of terms calculated from the values of its derivatives at a single point. In numerical analysis of differential equations, it helps in understanding how well a numerical method approximates a real-world problem.
  • A Taylor series can represent a function as \( f(x) = f(a) + f'(a)(x-a) + \frac{f''(a)}{2!}(x-a)^2 + \dots \).
  • This series allows us to develop numerical methods by approximating higher-order derivatives.
  • It is used to derive and verify the order of accuracy for numerical methods, like the Runge-Kutta methods.
The coefficients of the Taylor series give pivotal information that helps ensure that the numerical approximation matches the required accuracy by matching terms in the series.
Order of Accuracy
The Order of Accuracy in numerical methods specifies how well a method approximates the true solution of a differential equation. It indicates the convergence rate as the step size \( h \) tends to zero.
  • An algorithm is said to have an accuracy of order \( n \) if the error is proportional to \( O(h^{n+1}) \).
  • This means that as you refine the grid, or decrease \( h \), the solution error decreases proportionally.
  • For example, a fourth-order accurate method shows an error reduction by a factor of 16 when \( h \) is halved.
High order of accuracy in methods like the Runge-Kutta allows for greater precision with larger step sizes, making computations efficient while maintaining acceptable error margins.
Butcher Tableau
The Butcher Tableau is a standard notation used to describe Runge-Kutta methods succinctly. It organizes the coefficients and structure of the method into a neat format, which is crucial for the implementation of these methods.
  • It consists of three parts: the \( a \)-coefficients, the weights \( b \), and the nodes \( c \).
  • The \( a \)-coefficients dictate how each stage of the method depends on previous stages.
  • The weights \( b \) define how the stage results are combined to produce the next approximation.
Understanding and setting up the tableaux properly are key to creating efficient Runge-Kutta methods with desired levels of accuracy. The Butcher Tableau not only simplifies analysis but also aids in the design of methods that can be efficiently implemented.

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Most popular questions from this chapter

Write the theta method, (1.13), as a Runge-Kutta method.

Suppose that a \(\nu\)-stage ERK method of order \(\nu\) is applied to the linear scalar equation \(y^{\prime}=\lambda y\). Prove that $$ y_{n}=\left[\sum_{k=0}^{\nu} \frac{1}{k !}(h \lambda)^{k}\right]^{n} y_{0}, \quad n=0,1, \ldots $$
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