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State whether the given boundary value problem is homogeneous or non homogeneous. $$ y^{\prime \prime}+4 y=\sin x, \quad y(0)=0, \quad y(1)=0 $$

Short Answer

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Answer: The boundary value problem is non-homogeneous.

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01

Determine the form of the differential equation

We have the differential equation $$y^{\prime \prime} + 4y = \sin x.$$ Observe that the right-hand side is a function of \(x\), namely, \(\sin x\). Since the right-hand side is not equal to zero, the differential equation is non-homogeneous.
02

Examine the boundary conditions

The given boundary conditions are $$y(0) = 0$$ and $$y(1) = 0.$$ These conditions do not affect whether the given problem is homogeneous or non-homogeneous.
03

State the type of boundary value problem

Since the given differential equation is non-homogeneous, the overall boundary value problem is considered non-homogeneous.

Key Concepts

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

Differential Equations
Differential equations are a mathematical way to describe the relationship between a function and its derivatives. Think of them like a recipe that tells you how something changes over time or space. They can describe a wide range of phenomena, including how populations grow, how heat distributes in a room, or how a spring oscillates.

In simple terms, a differential equation will contain an unknown function, let's say \( y \), that we are trying to find, and its derivatives, represented as \( y' \) for the first derivative, \( y'' \) for the second derivative, and so on. The equation will equal some function of \( x \), or it could be just zero. When we solve a differential equation, we are looking for the mystery function \( y \) that makes the equation true for all values of \( x \).

To understand the differential equation presented in the exercise, \( y'' + 4y = \(sin x\) \), imagine a scenario where you're studying the movement of a pendulum. This equation could be telling you how the position of the pendulum changes over time.
Boundary Conditions
Now, let's discuss boundary conditions. They are additional pieces of information that specify the value of the solution of a differential equation at certain points. Think of them as rules that the solution must follow at the start and/or end points, much like rules in a game. For example, if we're still imagining our pendulum, a boundary condition might tell us where the pendulum is when we first start the clock.

In the context of our exercise, the boundary conditions are \( y(0) = 0 \) and \( y(1) = 0 \). This means that at the start (when \( x = 0 \)), the solution \( y \) must be zero, and it must again be zero at the end (when \( x = 1 \)). Boundary conditions are crucial when solving differential equations because they often allow us to pin down the exact solution we're after, eliminating other possible functions that don't meet these 'rules'.
Homogeneous vs Non-Homogeneous
In the world of differential equations, we categorize problems as either homogeneous or non-homogeneous. Homogeneous problems are simpler and come with a uniformity that lets us know that if we multiply a solution by any constant, we will still have a solution. They are characterized by having zero on one side of the equation after setting the function and its derivatives to zero.

On the other hand, non-homogeneous problems, like the one in our exercise, are a bit more complex. They have something other than zero on the opposite side of the differential equation, like the \( \sin x \) in \( y'' + 4y = \sin x \). This little twist means that the solutions to these problems aren't as straightforward, as we need to deal with an extra piece, the non-zero term, which represents some external influence acting on the system.

A quick way to spot a non-homogeneous equation is to look for any terms that don't involve the function being solved for or its derivatives. If you find any function of the independent variable—like \( \sin x \) in our case—that's your clue that the problem is non-homogeneous.

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Most popular questions from this chapter

Solve the given problem by means of an eigenfunction expansion. $$ y^{\prime \prime}+2 y=-x, \quad y(0)=0, \quad y^{\prime}(1)=0 ; \quad \text { see Section } 11.2, \text { Problem } 7 $$

Let \(\phi_{1}, \phi_{2}, \ldots, \phi_{n}, \ldots\) be the normalized eigenfunctions of the Sturm-Liouville problem \((11),(12) .\) Show that if \(a_{n}\) is the \(n\) th Fourier coefficient of a square integrable function \(f,\) then \(\lim _{n \rightarrow \infty} a_{n}=0\) Hint: Use Bessel's inequality, Problem \(9(b)\).

In the spherical coordinates \(\rho, \theta, \phi(\rho>0,0 \leq \theta<2 \pi, 0 \leq \phi \leq \pi)\) defined by the equations $$ x=\rho \cos \theta \sin \phi, \quad y=\rho \sin \theta \sin \phi, \quad z=\rho \cos \phi $$ Laplace's equation is $$ \rho^{2} u_{\rho \rho}+2 \rho u_{\rho}+\left(\csc ^{2} \phi\right) u_{\theta \theta}+u_{\phi \phi}+(\cot \phi) u_{\phi}=0 $$ (a) Show that if \(u(\rho, \theta, \phi)=\mathrm{P}(\rho) \Theta(\theta) \Phi(\phi),\) then \(\mathrm{P}, \Theta,\) and \(\Phi\) satisfy ordinary differential equations of the form $$ \begin{aligned} \rho^{2} \mathrm{P}^{\prime \prime}+2 \rho \mathrm{P}^{\prime}-\mu^{2} \mathrm{P} &=0 \\ \Theta^{\prime \prime}+\lambda^{2} \Theta &=0 \\\\\left(\sin ^{2} \phi\right) \Phi^{\prime \prime}+(\sin \phi \cos \phi) \Phi^{\prime}+\left(\mu^{2} \sin ^{2} \phi-\lambda^{2}\right) \Phi &=0 \end{aligned} $$ The first of these equations is of the Euler type, while the third is related to Legendre's equation. (b) Show that if \(u(\rho, \theta, \phi)\) is independent of \(\theta,\) then the first equation in part (a) is unchanged, the second is omitted, and the third becomes $$ \left(\sin ^{2} \phi\right) \Phi^{\prime \prime}+(\sin \phi \cos \phi) \Phi^{\prime}+\left(\mu^{2} \sin ^{2} \phi\right) \Phi=0 $$ (c) Show that if a new independent variable is defined by \(s=\cos \phi\), then the equation for \(\Phi\) in part (b) becomes $$ \left(1-s^{2}\right) \frac{d^{2} \Phi}{d s^{2}}-2 s \frac{d \Phi}{d s}+\mu^{2} \Phi=0, \quad-1 \leq s \leq 1 $$ Note that this is Legendre's equation.

Determine whether there is any value of the constant \(a\) for which the problem has a solution. Find the solution for each such value. $$ y^{\prime \prime}+4 \pi^{2} y=a+x, \quad y(0)=0, \quad y(1)=0 $$

Show that the problem $$ y^{\prime \prime}+\pi^{2} y=\pi^{2} x, \quad y(0)=1, \quad y(1)=0 $$ has the solution $$ y=c_{1} \sin \pi x+\cos \pi x+x $$ Also show that this solution cannot be obtained by splitting the problem as suggested in Problem \(15,\) since neither of the two subsidiary problems can be solved in this case.

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