Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Convert the following higher-order equations to systems of first-order equations: (a) \(Y^{\prime \prime \prime}+4 Y^{\prime \prime}+5 Y^{\prime}+2 Y=2 x^{2}+10 x+8\), \(Y(0)=1, \quad Y^{\prime}(0)=-1, \quad Y^{\prime \prime}(0)=3\) The true solution is \(Y(x)=e^{-x}+x^{2}\). (b) \(Y^{\prime \prime}+4 Y^{\prime}+13 Y=40 \cos (x), \quad Y(0)=3, \quad Y^{\prime}(0)=4\) The true solution is \(Y(x)=3 \cos (x)+\sin (x)+e^{-2 x} \sin (3 x)\).

Short Answer

Expert verified
(a) \[\begin{cases} y_1' = y_2 \ y_2' = y_3 \ y_3' = 2x^2 + 10x + 8 - 4y_3 - 5y_2 - 2y_1 \ \text{with } y_1(0) = 1, y_2(0) = -1, y_3(0) = 3 \ \end{cases}\](b) \[\begin{cases} y_1' = y_2 \ y_2' = 40\cos(x) - 4y_2 - 13y_1 \ \text{with } y_1(0) = 3, y_2(0) = 4 \ \end{cases}\]}

Step by step solution

01

- Define the new variables for part (a)

Let us define the new variables to convert the third-order differential equation to a system of first-order equations: \[y_1 = Y, \quad y_2 = Y', \quad y_3 = Y''\]
02

- Write the equations for part (a)

From the definitions, the following first-order differential equations are derived:\[y_1' = y_2\]\[y_2' = y_3\]The original differential equation can be written in terms of these new variables:\[y_3' + 4y_3 + 5y_2 + 2y_1 = 2x^2 + 10x + 8\]
03

- Write the system for part (a)

Now compile the first-order system:\[y_1' = y_2\]\[y_2' = y_3\]\[y_3' = 2x^2 + 10x + 8 - 4y_3 - 5y_2 - 2y_1\]Initial conditions:\[y_1(0) = 1, \quad y_2(0) = -1, \quad y_3(0) = 3\]
04

- Define new variables for part (b)

Similarly, define the new variables to convert the second-order differential equation to a first-order system:\[y_1 = Y, \quad y_2 = Y'\]
05

- Write the equations for part (b)

From the definitions, the following first-order differential equations are derived:\[y_1' = y_2\]The original differential equation can be written in terms of these new variables:\[y_2' + 4y_2 + 13y_1 = 40\cos(x)\]
06

- Write the system for part (b)

Compile the first-order system:\[y_1' = y_2\]\[y_2' = 40\cos(x) - 4y_2 - 13y_1\]Initial conditions:\[y_1(0) = 3, \quad y_2(0) = 4\]

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

first-order systems
Converting higher-order differential equations into first-order systems is a common technique in solving complex problems. This method involves breaking down a higher-order equation into multiple first-order equations.
An equation's order is determined by the highest derivative present. For example, a third-order equation involves up to third derivatives. By introducing new variables to represent these derivatives, you can simplify the problem.
Consider the given problem: we have higher-order differential equations of orders three and two, respectively. To transform them into first-order systems, follow these steps:
  • Introduce new variables for each derivative. For example, for the equation with a third derivative, define:
    \text{\(y_1 = Y\)}, \(y_2 = Y'\), and \(y_3 = Y''\).
  • Rewrite the higher-order equation using these new variables.
  • Establish first-order differential equations from the definitions and the original equation.
  • After this process, you will have transformed the problem into a more manageable system of first-order differential equations.
initial conditions
Initial conditions are critical when solving differential equations. They provide the specific values of the function and its derivatives at a given point, usually when \(x = 0\).
In this exercise, initial conditions for part (a) are \(Y(0) = 1\), \(Y'(0) = -1\), and \(Y''(0) = 3\). These conditions ensure a unique solution. For part (b), the initial conditions are \(Y(0) = 3\) and \(Y'(0) = 4\).
These initial conditions translate directly to the values of the newly defined variables at \(x = 0\). For example:
  • For part (a): \(y_1(0) = 1\), \(y_2(0) = -1\), and \(y_3(0) = 3\).
  • For part (b): \(y_1(0) = 3\) and \(y_2(0) = 4\).
By incorporating initial conditions, you can solve the first-order systems accurately. They help in determining the constants of integration and ensuring the solution matches the problem's specifics.
step-by-step solutions
Step-by-step solutions are essential for understanding complex mathematical problems. Breaking down the problem into manageable steps makes it easier to follow and solve efficiently.
Consider the solution process for the given exercise:
  • Step 1: Define new variables for each derivative to simplify the higher-order equation into a first-order system. For part (a), we define: \(y_1 = Y\), \(y_2 = Y'\), and \(y_3 = Y''\).
  • Step 2: Use these variables to rewrite the original higher-order differential equation in terms of the new variables. For example, \(Y^{\text{'''}} + 4Y'' + 5Y' + 2Y = 2x^2 + 10x + 8\) becomes \(y_3' + 4y_3 + 5y_2 + 2y_1 = 2x^2 + 10x + 8\).
  • Step 3: Write the resulting system of first-order equations. For instance, \(y_1' = y_2\), \(y_2' = y_3\), and \(y_3' = 2x^2 + 10x + 8 - 4y_3 - 5y_2 - 2y_1\).
  • Step 4: Apply the initial conditions to these new variables.
Following these steps ensures a clear and structured approach to solving differential equations.
differential equations
Differential equations involve functions and their derivatives. They are fundamental in modeling numerous phenomena in science and engineering.
In the given exercise, we deal with higher-order differential equations. For example, \(Y^{\text{'''}} + 4Y'' + 5Y' + 2Y = 2x^2 + 10x + 8\) and \(Y'' + 4Y' + 13Y = 40\text{cos}(x)\). These equations describe how a function and its derivatives relate to each other.
To solve these equations, especially when dealing with higher-order ones, converting them into a system of first-order differential equations is beneficial. It simplifies the process and makes numerical solutions more feasible.
Understanding the basic principles of differential equations is crucial. They help in predicting the behavior of various systems, from mechanical vibrations to electrical circuits. By learning to convert and solve these equations, one can unlock a deeper understanding of dynamic systems and their behaviors.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Consider the solutions \(Y(x)\) of $$ Y^{\prime}(x)+a Y(x)=d e^{-b x} $$ with \(a, b, d\) constants and \(a, b>0 .\) Calculate $$ \lim _{x \rightarrow \infty} Y(x) $$ Hint: \(\quad\) Consider separately the cases \(a \neq b\) and \(a=b\).

To make the error term in (8.94) a bit more believable, prove $$ \int_{0}^{h} g(x) d x-\frac{h}{2}[3 g(0)-g(-h)]=\frac{5}{12} h^{3} g^{\prime \prime}(0)+O\left(h^{4}\right) $$ Hint: Expand \(g(x)\) as a quadratic Taylor polynomial about the origin, with an error term \(R_{3}(x)\). Substitute that into the left side of the above equation, and obtain the right side.

Consider the differential equation $$ Y^{\prime}(x)=f_{1}(x) f_{2}(Y(x)) $$ for some given functions \(f_{1}(x)\) and \(f_{2}(z) .\) This is called a separable differential equation, and it can be solved by direct integration. Write the equation as $$ \frac{Y^{\prime}(x)}{f_{2}(Y(x))}=f_{1}(x) $$ and find the antiderivative of each side: $$ \int \frac{Y^{\prime}(x) d x}{f_{2}(Y(x))}=\int f_{1}(x) d x $$ On the left side, change the integration variable by letting \(z=Y(x)\). Then the equation becomes $$ \int \frac{d z}{f_{2}(z)}=\int f_{1}(x) d x $$ After integrating, replace \(z\) by \(Y(x)\); then solve for \(Y(x)\), if possible. If these integrals can be evaluated, then the differential equation can be solved. Do so for the following problems, finding the general solution and the solution satisfying the given initial condition: \(\begin{array}{ll}\text { (a) } Y^{\prime}(x)=x / Y(x), & Y(0)=2\end{array}\) (b) \(Y^{\prime}(x)=x e^{-Y(x)}, \quad Y(1)=0\) (c) \(\quad Y^{\prime}(x)=Y(x)[a-Y(x)], \quad Y(0)=a / 2, \quad a>0\)

In general, the study of the existence and uniqueness of a solution for boundary value problems is more complicated. Consider the boundary value problem $$ \left\\{\begin{array}{l} Y^{\prime \prime}=0, \quad 0

Consider the linear equation $$ Y^{\prime}(x)=\lambda Y(x)+(1-\lambda) \cos (x)-(1+\lambda) \sin (x), \quad Y(0)=1 $$ from (8.3) of Section 8.1. The true solution is \(Y(x)=\sin (x)+\cos (x)\). Solve this problem using Euler's method with several values of \(\lambda\) and \(h\), for \(0 \leq x \leq 10\). Comment on the results. (a) \(\quad \lambda=-1 ; \quad h=0.5,0.25,0.125\) (b) \(\lambda=1 ; \quad h=0.5,0.25,0.125\) (c) \(\quad \lambda=-5 ; \quad h=0.5,0.25,0.125,0.0625\) (d) \(\quad \lambda=5 ; \quad h=0.0625\)

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free