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Estimate the lowest eigenvalue \(\lambda_{0}\) of the equation $$ \frac{d^{2} y}{d x^{2}}-x^{2} y+\lambda y=0, \quad y(-1)=y(1)=0 $$ using a quadratic trial function.

Short Answer

Expert verified
The lowest eigenvalue is \( \lambda_{0} = 2 \).

Step by step solution

01

- Choose a Trial Function

Select a quadratic trial function that satisfies the boundary conditions. A suitable choice is: \[ y(x) = a(1 - x^2) \] Here, the constant factor 'a' will be determined later.
02

- Compute the First and Second Derivatives

Compute the first derivative: \[ \frac{dy}{dx} = -2ax \] and the second derivative: \[ \frac{d^2y}{dx^2} = -2a \]
03

- Substitute into the Differential Equation

Substitute \( y(x) \), \( \frac{dy}{dx} \), and \( \frac{d^2y}{dx^2} \) back into the differential equation: \[ -2a - x^2a(1 - x^2) + \lambda a(1 - x^2) = 0 \] Simplify to: \[ -2a - ax^2 + ax^4 + \lambda a - \lambda ax^2 = 0 \]
04

- Simplify the Equation

Collect terms to obtain: \[ a(-2 - x^2 + x^4 + \lambda - \lambda x^2) = 0 \] For the equation to hold for all x, the coefficient of \( a \) in each term must be zero. Focus first on terms without \( x \): \[ -2 + \lambda = 0 \]
05

- Solve for the Eigenvalue

From the above equation, solve for the eigenvalue \( \lambda \): \[ \lambda = 2 \]

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Key Concepts

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

Differential Equations
Differential equations involve derivatives of a function and connect these derivatives to the function itself.
In our exercise, the differential equation is: \[ \frac{d^{2} y}{d x^{2}}-x^{2} y+\beta y=0 \], where
\( \beta \) is the eigenvalue we need to estimate. This is a second-order differential equation.
Second-order because the highest derivative is a second derivative. We use these equations to describe various physical phenomena, such as wave patterns or heat distribution.
In solving differential equations, we often seek solutions that satisfy given boundary conditions.
Trial Functions
A trial function is a guessed solution that we use to start solving a differential equation.
It should be a simple, known function that satisfies the boundary conditions of the problem.
For our problem, we chose \[ y(x) = a(1 - x^2) \], a quadratic function. This means it has terms up to \( x^2 \).
Our choice is guided by the equation’s boundary conditions. By substituting this back into the original equation, we can test and refine our guessed solution.
This iterative approach helps us approximate complex solutions.
Boundary Conditions
Boundary conditions are constraints on the values that the solution to a differential equation can take at certain boundaries.
In this exercise, the boundary conditions are: \( y(-1)=0 \) and \( y(1)=0 \).
These conditions tell us the value of function \( y \) at the points \( x = -1 \) and \( x = 1 \).
When we select our trial function, it must satisfy these boundary conditions. For our quadratic trial function \[ y(x) = a(1 - x^2) \], we see that \( y(-1) = a(1 - (-1)^2) = a(1 - 1) = 0 \), which meets the boundary condition. Similarly, \( y(1) = a(1 - 1) = 0 \), which also fits the requirement.
Ensuring that our trial function meets these conditions helps us find a valid solution.
Eigenvalues and Eigenvectors
Eigenvalues and eigenvectors are crucial in understanding systems of differential equations.
For our problem, eigenvalues \( \beta \) give us essential characteristics of the differential equation itself.
To find them, we applied our chosen trial function and boundary conditions. In the simplified equation \[ a(-2 + \beta) = 0 \],
we found that \( \beta = 2 \). This tells us that the lowest eigenvalue is 2.
Eigenvectors, although not discussed in detail in this problem, would be the respective solutions of the differential equation.

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Most popular questions from this chapter

(a) Recast the problem of finding the lowest eigenvalue \(\lambda_{0}\) of the equation $$ \left(1+x^{2}\right) \frac{d^{2} y}{d x^{2}}+2 x \frac{d y}{d x}+\lambda y=0, \quad y(\pm 1)=0 $$ in variational form, and derive an approximation \(\lambda_{1}\) to \(\lambda_{0}\) by using the trial function \(y_{1}(x)=1-x^{2}\) (b) Show that an improved estimate \(\lambda_{2}\) is obtained by using \(y_{2}(x)=\cos (\pi x / 2)\) (c) Prove that the estimate \(\lambda(\gamma)\) obtained by taking \(y_{1}(x)+\gamma y_{2}(x)\) as the trial function is $$ \lambda(\gamma)=\frac{64 / 15+16 \gamma / \pi+\left(\pi^{2} / 3+1 / 2\right) \gamma^{2}}{16 / 15+64 \gamma / \pi^{3}+\gamma^{2}} $$ Investigate \(\lambda(\gamma)\) numerically as \(\gamma\) is varied, or, more simply, show that \(\lambda(1)=3.183\), a significant improvement on both \(\lambda_{1}\) and \(\lambda_{2-}\)

In cylindrical polar coordinates, the curve \((\rho(\theta), \theta, \alpha \rho(\theta))\) lies on the surface of the cone \(z=\alpha \rho\). Show that geodesics (curves of minimum length joining two points) on the cone satisfy $$ \rho^{4}=c^{2}\left[\beta^{2} \rho^{\prime 2}+\rho^{2}\right] $$ where \(c\) is an arbitrary constant, but \(\beta\) has to have a particular value. Determine the form of \(\rho(\theta)\) and hence find the equation of the shortest path on the cone between the points \(\left(R,-\theta_{0}, \alpha R\right)\) and \(\left(R, \theta_{0}, \alpha R\right)\). (You will find it useful to determine the form of the derivative of \(\cos ^{-1}\left(u^{-1}\right)\).)

For a system specified by the coordinates \(q\) and \(t\), show that the equation of motion is unchanged if the Lagrangian \(L(q, \dot{q}, t)\) is replaced by $$ L_{1}=L+\frac{d \phi(q, t)}{d t} $$ where \(\phi\) is an arbitrary function. Deduce that the equation of motion of a particle that moves in one dimension subject to a force \(-d V(x) / d x\) ( \(x\) being measured from a point \(O\) ) is unchanged if \(O\) is forced to move with a constant velocity \(v\) \((x\) still being measured from \(O)\).

A dam of capacity \(V\) (less than \(\left.\pi b^{2} h / 2\right)\) is to be constructed on level ground next to a long straight wall which runs from \((-b, 0)\) to \((b, 0) .\) This is to be achieved by joining the ends of a new wall, of height \(h\), to those of the existing wall. Show that, in order to minimise the length \(L\) of new wall to be built, it should form part of a circle, and that \(L\) is then given by $$ \int_{-b}^{b} \frac{d x}{\left(1-\lambda^{2} x^{2}\right)^{1 / 2}} $$ where \(\lambda\) is found from $$ \frac{V}{h b^{2}}=\frac{\sin ^{-1} \mu}{\mu^{2}}-\frac{\left(1-\mu^{2}\right)^{1 / 2}}{\mu} $$ and \(u=\lambda b\)

The Sturm-Liouville equation can be extended to two independent variables, \(x\) and \(z\), with little modification. In equation \((22.22) y^{\prime 2}\) is replaced by \((\nabla y)^{2}\) and the integrals of the various functions of \(y(x, z)\) become two-dimensional, i.e. the infinitesimal is \(d x d z\). The vibrations of a trampoline 4 units long and 1 unit wide satisfy the equation $$ \nabla^{2} y+k^{2} y=0 $$ By taking the simplest possible permissible polynomial as a trial function, show that the lowest mode of vibration has \(k^{2} \leq 10.63\) and, by direct solution, that the actual value is \(10.49\)

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