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(For this exercise you have to know about \(3 \times 3\) determinants.) Show that if \(y_{1}\) and \(y_{2}\) are twice continuously differentiable on \((a, b)\) and the Wronskian \(W\) of \(\left\\{y_{1}, y_{2}\right\\}\) has no zeros in \((a, b)\) then the equation $$\frac{1}{W}\left|\begin{array}{ccc} y & y_{1} & y_{2} \\ y^{\prime} & y_{1}^{\prime} & y_{2}^{\prime} \\ y^{\prime \prime} & y_{1}^{\prime \prime} & y_{2}^{\prime \prime} \end{array}\right|=0$$ can be written as $$y^{\prime \prime}+p(x) y^{\prime}+q(x) y=0$$ where \(p\) and \(q\) are continuous on \((a, b)\) and \(\left\\{y_{1}, y_{2}\right\\}\) is a fundamental set of solutions of (A) on \((a, b) .\) HINT: Expand the determinant by cofactors of its first column.

Short Answer

Expert verified
Question: Show that the given determinant equation can be written as a linear second-order differential equation of the form \(y^{\prime \prime}+p(x) y^{\prime}+q(x) y=0\), with \(p(x)\) and \(q(x)\) continuous on \((a, b)\) and \(\{y_{1}, y_{2}\}\) as a fundamental set of solutions of the differential equation on \((a, b)\). Solution: Following the step-by-step analysis and solution provided, we have successfully transformed the determinant equation into the desired linear second-order differential equation form \(y^{\prime \prime}+p(x) y^{\prime}+q(x) y=0\), where \(p(x)\) and \(q(x)\) are continuous on \((a, b)\) and \(\{y_{1}, y_{2}\}\) is a fundamental set of solutions of the differential equation on \((a, b)\).

Step by step solution

01

Expand the determinant

The determinant is given by $$\frac{1}{W}\left|\begin{array}{ccc} y & y_{1} & y_{2} \\ y^{\prime} & y_{1}^{\prime} & y_{2}^{\prime} \\ y^{\prime \prime} & y_{1}^{\prime \prime} & y_{2}^{\prime \prime} \end{array}\right|$$ Expanding by cofactors of the first column using the definition of a 3x3 determinant, we get: $$\frac{1}{W}(y\left|\begin{array}{cc} y_{1}^{\prime} & y_{2}^{\prime}\\ y_{1}^{\prime \prime} & y_{2}^{\prime \prime} \end{array}\right| - y'\left|\begin{array}{cc} y_{1} & y_{2}\\ y_{1}^{\prime \prime} & y_{2}^{\prime \prime} \end{array}\right| + y''\left|\begin{array}{cc} y_{1} & y_{2}\\ y_{1}^{\prime} & y_{2}^{\prime} \end{array}\right|)=0$$
02

Simplify expressions

Evaluate each of the 2x2 determinants and simplify as needed: $$\frac{1}{W}(y(y_{1}^{\prime}y_{2}^{\prime \prime}-y_{1}^{\prime \prime}y_{2}^{\prime})- y'(y_{1}y_{2}^{\prime \prime}-y_{1}^{\prime \prime}y_{2}) + y''(y_{1}y_{2}^{\prime}-y_{1}^{\prime}y_{2}))=0$$
03

Multiply both sides by the Wronskian, W

To get rid of the \(\frac{1}{W}\) term, multiply both sides by W: $$y(y_{1}^{\prime}y_{2}^{\prime \prime}-y_{1}^{\prime \prime}y_{2}^{\prime})- y'(y_{1}y_{2}^{\prime \prime}-y_{1}^{\prime \prime}y_{2}) + y''(y_{1}y_{2}^{\prime}-y_{1}^{\prime}y_{2})=0$$
04

Rearrange the terms

Rearrange the terms to get the equation into the desired form, \(y^{\prime \prime}+p(x) y^{\prime}+q(x) y=0\), where p(x) and q(x) are continuous functions of x: $$y''(y_{1}y_{2}^{\prime}-y_{1}^{\prime}y_{2})+ y'(y_{1}^{\prime \prime}y_{2} - y_{1}y_{2}^{\prime \prime}) + y(y_{1}^{\prime \prime}y_{2}^{\prime}-y_{1}^{\prime}y_{2}^{\prime \prime})=0$$
05

Define p(x) and q(x)

Define the continuous functions p(x) and q(x) as follows: $$p(x) = \frac{y_{1}^{\prime \prime}y_{2} - y_{1}y_{2}^{\prime \prime}}{y_{1}y_{2}^{\prime}-y_{1}^{\prime}y_{2}}$$ $$q(x) = \frac{y_{1}^{\prime \prime}y_{2}^{\prime}-y_{1}^{\prime}y_{2}^{\prime \prime}}{y_{1}y_{2}^{\prime}-y_{1}^{\prime}y_{2}}$$ Now we have the differential equation in the desired form: $$y^{\prime \prime}+p(x) y^{\prime}+q(x) y=0$$ The functions \(p(x)\) and \(q(x)\) are continuous on \((a, b)\) and \(\{y_{1}, y_{2}\}\) is a fundamental set of solutions of the differential equation on \((a, b)\).

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Key Concepts

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

Determinants
Determinants are a mathematical concept that plays a vital role in various areas such as linear algebra, geometry, and differential equations. When working with matrices, determinants are a scalar value that can be computed from a square matrix, which provides significant insights into properties of the matrix. For a 3x3 matrix, the determinant provides information about the invertibility of the matrix: if the determinant is non-zero, the matrix is invertible.### Calculating DeterminantsFor the exercise at hand, the determinant of a 3x3 matrix is expanded using minors and cofactors. The formula for a 3x3 determinant, where the matrix is \[\begin{bmatrix}a & b & c \d & e & f \g & h & i\end{bmatrix}\]is computed as:\[a(ei - fh) - b(di - fg) + c(dh - eg)\]This calculation is crucial in the exercise to simplify expressions that eventually lead to forming a differential equation.Understanding determinants and their expansion are essential to solving problems involving linear systems and changes of variables in integrals.
Differential Equations
Differential equations are fundamental tools in mathematics and science used to describe how variables change over time. In this exercise, you are given a specific form of a second-order linear differential equation:\[y'' + p(x) y' + q(x) y = 0\]### Role in the ExerciseThe goal is to show how the given equation derived from the Wronskian's determinant can be transformed into the standard form of a linear homogeneous differential equation.This transformation involves using the relationships among continuous functions and the roots provided by the Wronskian to express unknown functions, such as p(x) and q(x), in terms of known quantities. These solutions satisfy the differential equation under certain conditions, providing a method to model natural phenomena, from physics to economics.
Fundamental Set of Solutions
In the context of differential equations, a fundamental set of solutions is a set of linearly independent solutions that can be used to express every solution of a differential equation.For a second-order linear differential equation, such as those in this exercise, any solution can be represented as a linear combination of two independent solutions. ### Importance in the ExerciseIn the exercise, \( \{y_1, y_2\} \) is a fundamental set of solutions to the differential equation:\[y'' + p(x) y' + q(x) y = 0\]This means that any solution y to this equation can be written as:\[y = c_1 y_1 + c_2 y_2\]where \(c_1\) and \(c_2\) are constants.When the Wronskian of these solutions is non-zero, it confirms their linear independence and validates that \( \{y_1, y_2\} \) can form a basis for the solution space, ensuring every solution is representable within this framework.
Continuous Functions
Continuous functions are important in analysis and differential equations because they ensure that there are no sudden jumps or breaks in the function values. Continuity allows for better predictability and smoothness of functions over an interval, which is crucial for analyzing dynamic systems.### Significance in the ExerciseThe functions p(x) and q(x), expressed in terms of the solutions \(y_1\) and \(y_2\), must be continuous over the interval \((a, b)\) for the differential equation to preserve its properties.When dealing with continuous functions, you can rely on the Intermediate Value Theorem, among other analytical tools, to make predictions about behavior within an interval:
  • They allow for the application of integral and differential calculus.
  • Ensure the solutions and transformations are valid across the entire interval.
Continuous differentiability further ensures that derivatives exist and are continuous, as required in the exercise for \(y_1\) and \(y_2\), essential in forming the Wronskian and maintaining the integrity of the solution set.

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Most popular questions from this chapter

In Exercises 20-23 solve the initial value problem and plot the solution. $$ y^{\prime \prime}+4 y^{\prime}+3 y=-e^{-x}(2+8 x), \quad y(0)=1, \quad y^{\prime}(0)=2 $$

Let \(a, b, c,\) and \(\omega\) be constants, with \(a \neq 0\) and \(\omega>0\), and let $$ P(x)=p_{0}+p_{1} x+\cdots+p_{k} x^{k} \quad \text { and } \quad Q(x)=q_{0}+q_{1} x+\cdots+q_{k} x^{k} $$ where at least one of the coefficients \(p_{k}, q_{k}\) is nonzero, so \(k\) is the larger of the degrees of \(P\) and \(Q\). (a) Show that if \(\cos \omega x\) and \(\sin \omega x\) are not solutions of the complementary equation $$ a y^{\prime \prime}+b y^{\prime}+c y=0 $$ then there are polynomials $$ A(x)=A_{0}+A_{1} x+\cdots+A_{k} x^{k} \quad \text { and } \quad B(x)=B_{0}+B_{1} x+\cdots+B_{k} x^{k} $$ such that $$ \begin{aligned} \left(c-a \omega^{2}\right) A+b \omega B+2 a \omega B^{\prime}+b A^{\prime}+a A^{\prime \prime} &=P \\ -b \omega A+\left(c-a \omega^{2}\right) B-2 a \omega A^{\prime}+b B^{\prime}+a B^{\prime \prime} &=Q \end{aligned} $$ where \(\left(A_{k}, B_{k}\right),\left(A_{k-1}, B_{k-1}\right), \ldots,\left(A_{0}, B_{0}\right)\) can be computed successively by solving the systems $$ \begin{aligned} \left(c-a \omega^{2}\right) A_{k}+b \omega B_{k} &=p_{k} \\ -b \omega A_{k}+\left(c-a \omega^{2}\right) B_{k} &=q_{k} \end{aligned} $$ and, if \(1 \leq r \leq k,\) $$ \begin{aligned} \left(c-a \omega^{2}\right) A_{k-r}+b \omega B_{k-r} &=p_{k-r}+\cdots \\ -b \omega A_{k-r}+\left(c-a \omega^{2}\right) B_{k-r} &=q_{k-r}+\cdots \end{aligned} $$ where the terms indicated by "..." depend upon the previously computed coefficients with subscripts greater than \(k-r\). Conclude from this and Exercise \(36(\mathbf{b})\) that $$ y_{p}=A(x) \cos \omega x+B(x) \sin \omega x $$ is a particular solution of $$ a y^{\prime \prime}+b y^{\prime}+c y=P(x) \cos \omega x+Q(x) \sin \omega x . $$ (b) Conclude from Exercise \(36(\mathbf{c})\) that the equation $$ a\left(y^{\prime \prime}+\omega^{2} y\right)=P(x) \cos \omega x+Q(x) \sin \omega x $$ does not have a solution of the form (B) with \(A\) and \(B\) as in (A). Then show that there are polynomials $$ A(x)=A_{0} x+A_{1} x^{2}+\cdots+A_{k} x^{k+1} \quad \text { and } \quad B(x)=B_{0} x+B_{1} x^{2}+\cdots+B_{k} x^{k+1} $$ such that $$ \begin{aligned} a\left(A^{\prime \prime}+2 \omega B^{\prime}\right) &=P \\ a\left(B^{\prime \prime}-2 \omega A^{\prime}\right) &=Q \end{aligned} $$ where the pairs \(\left(A_{k}, B_{k}\right),\left(A_{k-1}, B_{k-1}\right), \ldots,\left(A_{0}, B_{0}\right)\) can be computed successively as follows: $$ \begin{aligned} A_{k} &=-\frac{q_{k}}{2 a \omega(k+1)} \\ B_{k} &=\frac{p_{k}}{2 a \omega(k+1)}, \end{aligned} $$ and, if \(k \geq 1\), $$ A_{k-j}=-\frac{1}{2 \omega}\left[\frac{q_{k-j}}{a(k-j+1)}-(k-j+2) B_{k-j+1}\right] $$ $$ B_{k-j}=\frac{1}{2 \omega}\left[\frac{p_{k-j}}{a(k-j+1)}-(k-j+2) A_{k-j+1}\right] $$ for \(1 \leq j \leq k\). Conclude that (B) with this choice of the polynomials \(A\) and \(B\) is a particular solution of \((\mathrm{C})\)

In Exercises \(24-29\) use the principle of superposition to find a particular solution. $$ y^{\prime \prime}+y=e^{-x}\left(2-4 x+2 x^{2}\right)+e^{3 x}\left(8-12 x-10 x^{2}\right) $$

Solve the initial value problem, given that \(y_{1}\) satisfies the complementary equation. \((3 x-1) y^{\prime \prime}-(3 x+2) y^{\prime}-(6 x-8) y=0, \quad y(0)=2, y^{\prime}(0)=3 ; \quad y_{1}=e^{2 x}\)

Use the principle of superposition to find a particular solution. Where indicated, solve the initial value problem. $$ y^{\prime \prime}-2 y^{\prime}-3 y=4 e^{3 x}+e^{x}(\cos x-2 \sin x) $$

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