/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 29 In Problems \(23-30\), verify th... [FREE SOLUTION] | 91Ó°ÊÓ

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In Problems \(23-30\), verify that the given functions form a fundamental set of solutions of the differential equation on the indicated interval. Form the general solution. $$ x^{3} y^{\prime \prime \prime}+6 x^{2} y^{\prime \prime}+4 x y^{\prime}-4 y=0 ; x, x^{-2}, x^{-2} \ln x,(0, \infty) $$

Short Answer

Expert verified
The general solution is \( y(x) = C_1 x + C_2 x^{-2} + C_3 x^{-2} \ln x \).

Step by step solution

01

Verify Linear Independence

To verify that the given functions form a fundamental set of solutions, we first need to check if they are linearly independent. Calculate the Wronskian of the functions \( y_1 = x \), \( y_2 = x^{-2} \), and \( y_3 = x^{-2} \ln x \). The Wronskian \( W(y_1, y_2, y_3) \) is given by:\[W(y_1, y_2, y_3) = \begin{vmatrix}y_1 & y_2 & y_3 \y_1' & y_2' & y_3' \y_1'' & y_2'' & y_3''\end{vmatrix}\]Compute the derivatives:* \( y_1' = 1, y_1'' = 0 \)* \( y_2' = -2x^{-3}, y_2'' = 6x^{-4} \)* \( y_3' = -2x^{-3} \ln x - x^{-3}, y_3'' = 6x^{-4} \ln x + 4x^{-4} \)Substitute into the Wronskian and solve the determinant to find it is non-zero on the given interval, confirming linear independence.
02

Check Differential Equation Form

The differential equation is cubic, highlighted by the third derivative \( y''' \) term. Ensure the functions are solutions by substituting them into the differential equation:For \( y_1 = x \), substitute to find that all terms equal zero, thus it is indeed a solution.For \( y_2 = x^{-2} \), substitute and confirm a zero result, verifying it as a solution.For \( y_3 = x^{-2} \ln x \), repeat the substitution. Simplification yields zero, verifying it as a solution.
03

General Solution Formation

Now that the functions form a fundamental set of solutions, use them to form the general solution of the differential equation:The general solution is a linear combination of the fundamental solutions:\[ y(x) = C_1 x + C_2 x^{-2} + C_3 x^{-2} \ln x \]where \( C_1, C_2, \) and \( C_3 \) are arbitrary constants.

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Key Concepts

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

Linear Independence
When dealing with solutions to differential equations, it's important to ensure that these solutions are linearly independent. This means that no function in the set can be written as a combination of the others. If they were dependent, one function could be "built" from another, which would mean the solutions aren't genuinely unique or original.
To verify linear independence, we often rely on the Wronskian, a kind of "determinant check" for functions. In our case, the functions given are: \( y_1 = x \), \( y_2 = x^{-2} \), and \( y_3 = x^{-2} \ln x \).
We compute the derivatives of these functions:
  • \( y_1' = 1 \) and \( y_1'' = 0 \)
  • \( y_2' = -2x^{-3} \) and \( y_2'' = 6x^{-4} \)
  • \( y_3' = -2x^{-3} \ln x - x^{-3} \) and \( y_3'' = 6x^{-4} \ln x + 4x^{-4} \)
By plugging these back into the Wronskian determinant and ensuring that the resulting determinant is non-zero over our interval \((0, \infty)\), we confirm that these functions are indeed linearly independent.
Fundamental Set of Solutions
Once we establish that the set of functions is linearly independent, we can call them a "fundamental set of solutions" for our differential equation on a given interval. A fundamental set is crucial because it forms the basis for all other solutions to the differential equation.
In simpler terms, any solution of the differential equation can be expressed as a combination of the functions in the fundamental set. This combination is weighted by constants, which adjust the "mix" of how much of each function is in our solution, depending on initial or boundary conditions.
In our exercise, the fundamental set of solutions is \( x, x^{-2}, \text{and} \ x^{-2} \ln x \). Since these functions solve our differential equation and are linearly independent, they create a solid foundation to construct the general solution. This general solution satisfies the differential equation for any partition of \((0, \infty)\).
Wronskian
The Wronskian is a powerful tool used in differential equations to test whether a set of functions is linearly independent. It's a determinant formed by the functions and their derivatives, structured in a matrix.
For three functions like \( y_1 = x \), \( y_2 = x^{-2} \), and \( y_3 = x^{-2} \ln x \), the Wronskian \( W(y_1, y_2, y_3) \) would be:
\[W(y_1, y_2, y_3) = \begin{vmatrix}y_1 & y_2 & y_3 \y_1' & y_2' & y_3' \y_1'' & y_2'' & y_3''\end{vmatrix}\]
Here, by calculating this determinant and finding it non-zero in the interval \((0, \infty)\), we verify linear independence. Hence, these functions are suitable to form a fundamental set of general solutions. It's essential to remember that a zero Wronskian isn't the only determinant of dependence — it hints towards potential dependence, which requires further analysis.

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Most popular questions from this chapter

The indefinite integrals of the equations in (5) are nonelementary. Use a CAS to find the first four nonzero terms of a Maclaurin series of each integrand and then integrate the result. Find a particular solution of the given differential equation. $$ 4 y^{\prime \prime}-y=e^{x^{2}} $$

Find a homogeneous linear differential equation with constant coefficients whose general solution is given. $$ y \quad c_{1}+c_{2} e^{3 x} $$

In Problems, find the eigenvalues and eigenfunctions for the given boundary- value problem. $$ y^{\prime \prime}+\lambda y=0, y(-\pi)=0, y(\pi)=0 $$

Consider a pendulum that is released from rest from an initial displacement of \(\theta_{0}\) radians. Solving the linear model (7) subject to the initial conditions \(\theta(0)=\theta_{0}, \theta^{\prime}(0)=0\) gives \(\theta(t)=\theta_{0} \cos \sqrt{g} \| t .\) Theperiod of oscillations predicted by this modelisgivenbythefamiliarformula \(T=2 \pi / \sqrt{g l l}=2 \pi \sqrt{U g}\). The interesting thing about this formula for \(T\) is that it does not depend on the magnitude of the initial displacement \(\theta_{0}\). In other words, the linear model predicts that the time that it would take the pendulum to swing from an initial displacement of, say, \(\theta_{0}=\pi / 2\left(=90^{\circ}\right)\) to \(-\pi / 2\) and back again would be exactly the same time to cycle from, say, \(\theta_{0}=\pi / 360\left(=0.5^{\circ}\right)\) to \(-\pi / 360\). This is intuitively unreasonable; the actual period must depend on \(\theta_{0}\). If we assume that \(g=32 \mathrm{ft} / \mathrm{s}^{2}\) and \(l=32 \mathrm{ft}\), then the period of oscillation of the linear model is \(T=2 \pi \mathrm{s}\). Let us compare this last number with the period predicted by the nonlinear model when \(\theta_{0}=\pi / 4\). Using a numerical solver that is capable of generating hard data, approximate the solution of $$\frac{d^{2} \theta}{d t^{2}}+\sin \theta=0, \quad \theta(0)=\frac{\pi}{4}, \quad \theta^{\prime}(0)=0$$ for \(0 \leq t \leq 2\). As in Problem 24 , if \(t_{1}\) denotes the first time the pendulum reaches the position \(O P\) in Figure 3.11.3, then the period of the nonlinear pendulum is \(4 t_{1} .\) Here is another way of solving the equation \(\theta(t)=0\). Expeniment with small step sizes and advance the time staning at \(t=0\) and ending at \(t=2\). From your hard data, observe the time \(t_{1}\) when \(\theta(t)\) changes, for the first time, from positive to negative. Use the value \(t_{1}\) to determine the true value of the period of the nonlinear pendulum. Compute the percentage relative error in the period estimated by \(T=2 \pi\).

Solve the given initial-value problem. \(y^{\prime \prime}-y=\cosh x, y(0)=2, y^{\prime}(0)=12\)

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