Chapter 17: Problem 14
Find an eigenfunction expansion for the solution with boundary conditions
\(y(0)=y(\pi)=0\) of the inhomogeneous equation
$$
\frac{d^{2} y}{d x^{2}}+\kappa y=f(x)
$$
where \(\kappa\) is a constant and
$$
f(x)= \begin{cases}x, & 0 \leq x \leq \pi / 2 \\ \pi-x, & \pi / 2
Short Answer
Expert verified
The eigenfunction expansion is \( y(x) = \sum_{n=1}^\infty c_n \sin(nx) \) where \( c_n = \frac{b_n}{n^2 - \kappa} \).
Step by step solution
01
Identify the boundary value problem
The given boundary value problem is \( \frac{d^2 y}{d x^2} + \kappa y = f(x) \) with boundary conditions \( y(0) = y(\pi) = 0 \).
02
Determine the corresponding homogeneous problem
Solve the homogeneous equation \( \frac{d^2 y}{d x^2} + \kappa y = 0 \) with the same boundary conditions \( y(0) = y(\pi) = 0 \).
03
Solve the homogeneous problem
Assuming \( y(x) = e^{\lambda x} \), the characteristic equation becomes \( \lambda^2 + \kappa = 0 \), giving us \( \lambda = \pm i\sqrt{\kappa} \). Thus, the general solution is \( y_h(x) = A\cos(\sqrt{\kappa}x) + B\sin(\sqrt{\kappa}x) \). Using the boundary conditions, solve for A and B. Applying \( y(0) = 0 \), we get A = 0. Applying \( y(\pi) = 0 \), we find \( B\sin(\sqrt{\kappa}\pi) = 0 \), leading us to \( \sqrt{\kappa} \pi = n\pi \) (where n is an integer), so \( \sqrt{\kappa} = n \). The homogeneous solution satisfying the boundary conditions is \( y_h(x) = B\sin(nx) \).
04
Find the particular solution
The particular solution for the inhomogeneous equation can be expressed as a series expansion \( y_p(x) = \sum_{n=1}^\infty c_n \sin(nx) \). Use Fourier sine series to find the coefficients \( c_n \).
05
Compute Fourier sine series coefficients
Given \( f(x) \), find the Fourier sine series coefficients \( c_n \) for \( f(x) \). The expansion is given by: \[ f(x) = \sum_{n=1}^{\infty} b_n \sin(nx) \], where \[ b_n = \frac{2}{\pi} \left( \int_0^{\pi/2} x \sin(nx) \, dx + \int_{\pi/2}^{\pi} (\pi - x) \sin(nx) \, dx \right) \]. Compute these integrals.
06
Solve the integrals for coefficients
Compute the integrals: \[ b_n = \frac{2}{\pi} \left( \int_0^{\pi/2} x \sin(nx) \, dx + \int_{\pi/2}^{\pi} (\pi - x) \sin(nx) \, dx \right) \]. Calculate each integral separately: \[ \int_0^{\pi/2} x \sin(nx) \, dx \] and \[ \int_{\pi/2}^{\pi} (\pi - x) \sin(nx) \, dx \]. Use integration by parts to solve these integrals.
07
Combine solutions
Combine the coefficients to form the series for the particular solution \( y_p(x) = \sum_{n=1}^{\infty} c_n \sin(nx)\) and add it to the homogeneous solution to form the eigenfunction expansion of the original equation. So, the final solution is \( y(x) = \sum_{n=1}^{\infty} \frac{b_n}{n^2 - \kappa} \sin(nx)\).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
inhomogeneous differential equations
Inhomogeneous differential equations are a type of differential equation that includes a non-zero forcing function, often denoted as \(f(x)\). Unlike homogeneous differential equations, which have zero on the right-hand side, inhomogeneous equations include an additional term. In this problem, we have: \begin{itemize} An inhomogeneous differential equation: \( \frac{d^2 y}{d x^2} + \kappa y = f(x) \) with \(\kappa\) as a constant. The forcing function \(f(x)\) varies with different segments defined piecewise. The approach to solving such equations involves:
- Solving the corresponding homogeneous equation (without \(f(x)\)).
- Finding a particular solution for the inhomogeneous equation.
- Combining these solutions to get the general solution.
boundary value problems
Boundary value problems (BVPs) are differential equations accompanied by a set of additional constraints called boundary conditions. They include:
- Conditions at the boundaries (endpoints) of the domain of the solution.
- For our problem: \(y(0)=y(\pi)=0\).
- Firstly solving the homogeneous problem which satisfies the boundary conditions.
- Secondly adding the particular solution of the inhomogeneous equation, which also must satisfy the boundary conditions.
Fourier sine series
The Fourier sine series is a way to represent a function as a sum of sine terms. It is particularly useful in solving boundary value problems, especially with conditions like \( y(0) = y(\pi) = 0 \). For our problem:
- We express the given function \(f(x)\) as a series of sines.
- The coefficients \(b_n\) of the sine series are computed using the formula: \( b_n = \frac{2}{\pi} \left( \int_0^{\pi/2} x \sin(nx) \, dx + \int_{\pi/2}^{\pi} (\pi - x) \sin(nx) \, dx \right) \).
homogeneous solutions
Homogeneous solutions are solutions to the differential equation without the non-homogeneous term (\(f(x)\)). For our problem, we solve:
- The equation: \(\frac{d^2 y} {d x^2} + \kappa y = 0 \).
- By assuming a solution form like \(y(x) = e^{\lambda x}\), we solve the characteristic equation \(\lambda^2 + \kappa = 0\).
- A general solution \(y_h(x) = A \cos(\sqrt{\kappa} x) + B \sin(\sqrt{\kappa} x)\).
- Using the boundary conditions \( y(0) = 0 \) and \( y(\pi) = 0 \), we determine coefficients \(A\) and \(B\).
- We find \( A = 0 \) and \( \sqrt{\kappa} = n \)
- Thus homogeneous solution becomes \( y_h(x) = B \sin(nx) \).