/*! 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 12 \(x^{\prime}=x \sqrt{y}, y^{\pri... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

\(x^{\prime}=x \sqrt{y}, y^{\prime}=x-y, x(1)=1, y(1)=1, t=2\)

Short Answer

Expert verified
At \( t = 2 \), \( x(2) = 2 \) and \( y(2) = 1 \).

Step by step solution

01

- Recognize the System of Differential Equations

Given the system of equations: 1. \( x' = x \sqrt{y} \) 2. \( y' = x - y \) with initial conditions \( x(1)=1 \) and \( y(1)=1 \).
02

- Use Euler's Method

To solve numerically up to \( t = 2 \), use Euler's method with a step size \( h = 1 \). At \( t = 1 \), we have initial values \( x(1) = 1 \) and \( y(1) = 1 \).
03

- Calculate the Next Values for t = 2

Euler's method gives the next values as follows: - For \( x \): \( x(2) = x(1) + h \cdot x(1) \sqrt{y(1)} = 1 + 1 \cdot 1 \sqrt{1} = 1 + 1 = 2 \)- For \{ y \}: \( y(2) = y(1) + h \cdot (x(1) - y(1)) = 1 + 1 \cdot (1 - 1) = 1 + 0 = 1 \)

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 91Ó°ÊÓ!

Key Concepts

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

Numerical approximation
Numerical approximation is a powerful tool used when an exact solution to a problem is too difficult to obtain analytically. In the case of differential equations, numerical methods like Euler's method allow us to estimate the values of the variables at different points.
Euler's method provides a way to approximate solutions to ordinary differential equations (ODEs) using a step-by-step approach. This method is particularly useful when dealing with initial value problems, where you know the starting condition but want to find the behavior of the system at a later time.
The core idea behind Euler's method is to start from the known initial conditions and then use the slope of the function to estimate new values. This slope is given by the differential equation itself. As the step size decreases, the accuracy of the approximation generally improves. However, smaller steps also require more computations.
Initial conditions
Initial conditions are the starting values of the variables in a differential equation. They play a crucial role in determining the particular solution to the problem. For example, in our given exercise, we have initial conditions: \( x(1) = 1 \) and \( y(1) = 1 \).
The purpose of specifying initial conditions is to pinpoint the exact trajectory of the variables from a specific starting point. Without initial conditions, the differential equations offer a family of possible solutions. However, with initial conditions, we can narrow it down to a single, unique solution.
In Euler's method, the initial conditions serve as the starting point for the numerical approximation. We begin from these values and apply the iterative process to find the values at subsequent steps.
Step-by-step solution
A step-by-step solution is essential for understanding and applying Euler's method correctly. Let's break down the given exercise to illustrate this process:
- Step 1: Recognize the System of Differential Equations
We are given two differential equations: \( x' = x \sqrt{y} \) and \( y' = x - y \). With the initial conditions \( x(1)=1 \) and \( y(1)=1 \), our goal is to find the values of \( x \) and \( y \) at \( t=2 \).
- Step 2: Use Euler's Method
To solve this numerically up to \( t=2 \), we use Euler's method with a step size of \( h = 1 \). Starting from \( t=1 \), our known initial values are \( x(1) = 1 \) and \( y(1) = 1 \).
- Step 3: Calculate the Next Values for \( t=2 \)
Now, use Euler's method to find the next values:
For \( x \):\( x(2) = x(1) + h \cdot x(1) \sqrt{y(1)} = 1 + 1 \cdot 1 \sqrt{1} = 1 + 1 = 2 \)
For \( y \):\( y(2) = y(1) + h \cdot (x(1) - y(1)) = 1 + 1 \cdot (1 - 1) = 1 + 0 = 1 \)

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

(a) Find a general solution of \(\mathbf{X}^{\prime}=\mathbf{A X}\) if \(\mathbf{X}(t)=\left(\begin{array}{l}x_{1} \\ x_{2} \\ x_{3} \\\ x_{4}\end{array}\right)\) and (i) \(\mathbf{A}=\left(\begin{array}{cccc}\lambda & 0 & 0 & 0 \\ 0 & \lambda & 0 & 0 \\ 0 & 0 & \lambda & 0 \\ 0 & 0 & 0 & \lambda\end{array}\right)\) (ii) \(\mathbf{A}=\left(\begin{array}{cccc}\lambda & 1 & 0 & 0 \\ 0 & \lambda & 0 & 0 \\ 0 & 0 & \lambda & 0 \\ 0 & 0 & 0 & \lambda\end{array}\right)\), (iii) \(\mathbf{A}=\left(\begin{array}{llll}\lambda & 1 & 0 & 0 \\ 0 & \lambda & 1 & 0 \\ 0 & 0 & \lambda & 0 \\ 0 & 0 & 0 & \lambda\end{array}\right)\), and (iv) \(\mathbf{A}=\left(\begin{array}{cccc}\lambda & 1 & 0 & 0 \\ 0 & \lambda & 1 & 0 \\ 0 & 0 & \lambda & 1 \\ 0 & 0 & 0 & \lambda\end{array}\right)\). (b) For each system in (a), find the solution that satisfies the initial condition \(\mathbf{X}(0)=\left(\begin{array}{c}-1 \\ 0 \\ 1 \\\ 2\end{array}\right)\) if \(\lambda=-1 / 2\) and then graph \(x_{1}, x_{2}, x_{3}\), and \(x_{4}\) for \(0 \leq t \leq 10\). How are the solutions similar? How are they different? (c) Indicate how to generalize the results obtained in (a). How would you find a general solution of \(\mathbf{X}^{\prime}=\mathbf{A} \mathbf{X}\) for the \(5 \times 5\) matrix \(\mathbf{A}=\) \(\left(\begin{array}{lllll}\lambda & 1 & 0 & 0 & 0 \\ 0 & \lambda & 1 & 0 & 0 \\\ 0 & 0 & \lambda & 1 & 0 \\ 0 & 0 & 0 & \lambda & 1 \\ 0 & 0 & 0 & 0 & \lambda\end{array}\right)\) ? How would you find a general solution of \(\mathbf{X}^{\prime}=\mathbf{A X}\) for the \(n \times n\) $$ \text { matrix } \mathbf{A}=\left(\begin{array}{cccccc} \lambda & 1 & 0 & \cdots & 0 & 0 \\ 0 & \lambda & 1 & \cdots & 0 & 0 \\ \vdots & \vdots & \ddots & \ddots & \vdots & \vdots \\ \vdots & \vdots & \vdots & \ddots & \ddots & \vdots \\ 0 & 0 & 0 & \cdots & \lambda & 1 \\ 0 & 0 & 0 & \cdots & 0 & \lambda \end{array}\right) ? $$ Let \(\mathbf{X}=\mathbf{X}(t)=\left(\begin{array}{c}x_{1}(t) \\ x_{2}(t) \\\ \vdots \\ x_{n}(t)\end{array}\right), \mathbf{A}=\mathbf{A}(t)=\) \(\left(\begin{array}{cccc}a_{11}(t) & a_{12}(t) & \cdots & a_{1 n}(t) \\\ a_{21}(t) & a_{22}(t) & \cdots & a_{2 n}(t) \\ \vdots & \vdots & \ddots & \vdots \\ a_{n 1}(t) & a_{n 2}(t) & \cdots & a_{n n}(t)\end{array}\right), \mathbf{F}(t)=\left(\begin{array}{c}f_{1}(t) \\ f_{2}(t) \\ \vdots \\\ f_{n}(t)\end{array}\right)\), and \(\boldsymbol{\Phi}(t)\) be a fundamental matrix of the corresponding homogeneous system \(\mathbf{X}^{\prime}=\mathbf{A X}\). Then a general solution to the corresponding homogeneous system \(\mathbf{X}^{\prime}=\mathbf{A X}\) is \(\mathbf{X}_{h}=\boldsymbol{\Phi}(t) \mathbf{C}\) where \(\mathbf{C}=\left(\begin{array}{c}c_{1} \\ c_{2} \\ \vdots \\\ c_{n}\end{array}\right)\) is an \(n \times 1\) constant matrix. To find a general solution to the linear nonhomogeneous system \(\mathbf{X}^{\prime}=\mathbf{A} \mathbf{X}+\mathbf{F}(t)\), we proceed in the same way we did with linear nonhomogeneous equations in Chapter 4 . If \(\mathbf{X}_{p}(t)\) is a particular solution of the nonhomogeneous system, then all other solutions \(\mathbf{X}\) of the system can be written in the form \(\mathbf{X}(t)=\mathbf{X}_{h}(t)+\mathbf{X}_{p}(t)=\) \(\boldsymbol{\Phi}(t) \mathbf{C}+\mathbf{X}_{p}(t)\) (see Exercise 36).

(Operator Notation) Recall the differential operator \(D=d / d t\), which was introduced in Exercises 4.2. Using this notation, we can write the system \(y^{\prime \prime}+2 y^{\prime}-x^{\prime}+4 x=\cos t\) \(x^{\prime \prime}+x+y^{\prime \prime}-y^{\prime}-2 y=e^{t}\) \(\left(D^{2}+2 D\right) y-(D-4) x=\cos t\) \(\left(D^{2}+1\right) x+\left(D^{2}-D-2\right) y=e^{t}\) Operator notation can be used to solve a system. For example, if we consider the system \(D x=y, D y=-x\) or \(D x-y=0\), \(-D x-D^{2} y=0\), we can eliminate one of the variables by applying the operator \(-D\) to the second equation to obtain \(D x-y=0\), \(-D x-D^{2} y=0\). When these two equations are added, we have the second order ODE \(-D^{2} y-y=0\) or \(D^{2} y+y=0\). This equation has the characteristic equation \(r^{2}+1=\) 0 , with roots \(r_{1,2}=\pm i\). Therefore, \(y(t)=\) \(c_{1} \cos t+c_{2} \sin t\). At this point, we can repeat the elimination procedure to solve for \(x\), or we can use the equation \(D y+x=0\) or \(x=-D y\) to find \(x\). Applying \(-D\) to \(y\) yields $$ \begin{aligned} x(t) &=-D y(t)=-D\left(c_{1} \cos t+c_{2} \sin t\right) \\ &=c_{1} \sin t-c_{2} \cos t . \end{aligned} $$ Therefore, a general solution of the system is \(x(t)=c_{1} \sin t-c_{2} \cos t, y(t)=c_{1} \cos t+\) \(c_{2} \sin t\).

(Principle of Superposition) (a) Show that any linear combination of solutions of the homogeneous system \(\mathbf{X}^{\prime}(t)=\mathbf{A}(t) \mathbf{X}(t)\) is also a solution of the homogeneous system. (b) Is the Principle of Superposition ever valid for nonhomogeneous systems of equations? Explain.

\(\left\\{\begin{array}{l}\left(2 t^{2}-t-1\right) x^{\prime}=2 t x-y-z \\\ \left(2 t^{2}-t-1\right) y^{\prime}=-x+2 t y-z+2 t^{2}-t-1 \\ \left(2 t^{2}-t-1\right) z^{\prime}=-x-y+2 t z\end{array}\right.\)

Given the nonlinear system $$ \begin{aligned} &d x / d t=y+\mu x\left(x^{2}+y^{2}\right) \\ &d y / d t=-x+\mu y\left(x^{2}+y^{2}\right) \end{aligned} $$ (a) Show that this system has the equilibrium point \((0,0)\) and the linearized system about this point is \(\left\\{\begin{array}{l}d x / d t=y \\ d y / d t=-x\end{array} .\right.\) Also show that \((0,0)\) is classified as a center of the linearized system. (b) Consider the change of variables to polar coordinates \(x=r \cos \theta\) and \(y=r \sin \theta\). Use these equations with the chain rule to show that \(\frac{d x}{d t}=\cos \theta \frac{d r}{d t}-r \sin \theta \frac{d \theta}{d t}\) and \(\frac{d y}{d t}=\) \(\sin \theta \frac{d r}{d t}+r \cos \theta \frac{d \theta}{d t}\). Use elimination with these equations to show that \(\frac{d r}{d t}=\cos \theta \frac{d x}{d t}+\sin \theta \frac{d y}{d t}\) and \(r \frac{d \theta}{d t}=\) \(-\sin \theta \frac{d x}{d t}+\cos \theta \frac{d y}{d t}\). Transform the original system to polar coordinates and substitute the equations that result in the equations for \(d r / d t\) and \(r d \theta / d t\) to obtain the system in polar coordinates \(\left\\{\begin{array}{l}d r / d t=\mu r^{3} \\ d \theta / d t=-1\end{array}\right.\) (c) What does the equation \(d \theta / d t=-1\) indicate about the rotation of solutions to the system? According to \(d r / d t=\mu r^{3}\), does \(r\) increase or decrease for \(r>0\) ? Using these observations, is the equilibrium point \((0,0)\), which was classified as a center for the linearized system, also classified as a center for the nonlinear system? If not, how would you classify it?

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.