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

Direction fields with technology Plot a direction field for the following differential equation with a graphing utility. Then find the solutions that are constant and determine which initial conditions \(y(0)=A\) lead to solutions that are increasing in time. $$y^{\prime}(t)=(y-1) \sin \pi t, 0 \leq t \leq 2,0 \leq y \leq 2$$

Short Answer

Expert verified
Question: Determine if there are any initial conditions, y(0) = A, that lead to solutions that are increasing in time for the differential equation y'(t) = (y - 1) sin πt. Answer: No initial conditions y(0) = A lead to solutions that are increasing in time for the given differential equation.

Step by step solution

01

Plot the direction field

Use a graphing utility or online tool to plot the direction field of the given differential equation: $$y^{\prime}(t)=(y - 1) \sin \pi t$$ for \(0 \leq t \leq 2\) and \(0 \leq y \leq 2\). By observing the graph, one can get an idea of how the solutions will behave for different initial conditions.
02

Find the constant solutions of the differential equation

For a solution to be constant, its derivative must be equal to 0. Therefore, set the right-hand side of the differential equation equal to 0. $$(y-1) \sin \pi t = 0$$ Now, either \((y-1)\) or \(\sin \pi t\) must be equal to 0 for the equation to hold. If \(\sin \pi t = 0\), then \(t\) is an integer. However, we are looking for constant solutions, i.e., solutions that don't depend on \(t\). So, we need to consider the case where \((y-1) = 0\). Thus, \(y=1\) is a constant solution, which means that there exists a horizontal line at \(y=1\) on the direction field plot.
03

Determine the initial conditions that lead to increasing solutions

To determine which initial conditions \(y(0)=A\) lead to increasing solutions, we need to analyze the sign of the right-hand side of the differential equation. If the right-hand side of the equation is positive, then \(y^{\prime}(t) > 0\) and the solution is increasing at that point. Conversely, if the right-hand side is negative, the solution is decreasing. Consider the interval \(0 \leq t \leq 2\). In this interval, we have a complete period of the sine function, so \(\sin \pi t\) changes its sign from positive to negative and vice versa. Now, let's look at the other term: \((y-1)\). For \(0 \leq y < 1\), \((y-1)\) is negative. For \(y = 1\), \((y-1)\) is equal to 0. Finally, for \(1 < y \leq 2\), \((y-1)\) is positive. Since we are looking for increasing solutions at \(t=0\), we must have \((y - 1) \sin \pi t > 0\) at \(t=0\). Since \(\sin(\pi (0)) = 0\), there are no points at \(t=0\) where \((y - 1) \sin \pi t > 0\). Thus, no initial conditions \(y(0)=A\) lead to solutions that are increasing in time.

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.

Graphing Utility
A graphing utility is an invaluable tool when it comes to understanding differential equations and their direction fields. This digital tool allows us to visualize how solutions to these equations behave under different circumstances. By inputing the differential equation \(y'(t) = (y - 1) \sin \pi t\) into a graphing utility, we can quickly generate a direction field that graphically represents the slope of solutions at various points in the plane defined by time \(t\) and function value \(y\).

These slopes, indicated by small lines or arrows, show the direction in which a solution curve would move if it passed through that point. The graph provides a snapshot of all possible solution trajectories, serving as a detailed map from which you can predict the behavior of solutions given particular initial conditions. As such, using a graphing utility simplifies complex numerical or algebraic methods and enhances our intuition about the system we're studying.
Constant Solutions
Constant solutions to differential equations are those where the value of the function does not change over time. Essentially, these are the steady states of our equation. In our exercise, finding the constant solutions involves setting the derivative equal to zero, \((y-1) \sin \pi t = 0\).

Identifying Constant Solutions

In this context, to find a constant solution, we focus on the \((y-1)\) term. This is because the value of \(y\) that makes \((y-1)=0\) will render our derivative zero for all values of \(t\), indicating that \(y=1\) is indeed a constant solution. This result corresponds to a horizontal line on the direction field, showing no change in \(y\) over time, regardless of the value of .

This understanding of constant solutions is particularly helpful if we're considering long-term behavior of a system modeled by the differential equation, as it informs us of the conditions under which the system will not evolve further.
Initial Conditions
Initial conditions, often denoted as \(y(0)=A\), play a crucial role in defining the specific solution to a differential equation out of a family of possible solutions. These conditions serve as a 'starting point' for the solution, dictating its behavior as time progresses.

Impact on Solution Trajectories

For the given differential equation, we're specially interested in distinguishing initial conditions leading to increasing solutions over time. The primary challenge here is the effect of the sine function, \(\sin \pi t\), which oscillates and changes sign. At \(t=0\), the sine function is zero, therefore, no positive value of \((y-1)\sin \pi t\) can be found, implying that no initial condition at this point leads to increasing solutions.

This conclusion is drawn by analyzing the derivative at \(t=0\); for an increasing solution, the derivative must be positive, but here it is zero. Thus, it is crucial to realize that the behavior of solutions is inherently tied to both initial conditions and the nature of the function encapsulated within the differential equation.

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

Equilibrium solutions \(A\) differential equation of the form \(y^{\prime}(t)=f(y)\) is said to be autonomous (the function \(f\) depends only on y. The constant function \(y=y_{0}\) is an equilibrium solution of the equation provided \(f\left(y_{0}\right)=0\) (because then \(y^{\prime}(t)=0\) and the solution remains constant for all \(t\) ). Note that equilibrium solutions correspond to horizontal lines in the direction field. Note also that for autonomous equations, the direction field is independent of t. Carry out the following analysis on the given equations. a. Find the equilibrium solutions. b. Sketch the direction field, for \(t \geq 0\). c. Sketch the solution curve that corresponds to the initial condition \(y(0)=1\). $$y^{\prime}(t)=y(2-y)$$

Consider the general first-order linear equation \(y^{\prime}(t)+a(t) y(t)=f(t) .\) This equation can be solved, in principle, by defining the integrating factor \(p(t)=\exp \left(\int a(t) d t\right) .\) Here is how the integrating factor works. Multiply both sides of the equation by \(p\) (which is always positive) and show that the left side becomes an exact derivative. Therefore, the equation becomes $$p(t)\left(y^{\prime}(t)+a(t) y(t)\right)=\frac{d}{d t}(p(t) y(t))=p(t) f(t)$$ Now integrate both sides of the equation with respect to t to obtain the solution. Use this method to solve the following initial value problems. Begin by computing the required integrating factor. $$y^{\prime}(t)+2 t y(t)=3 t, y(0)=1$$

Solving initial value problems Solve the following initial value problems. $$u^{\prime \prime}(x)=4 e^{2 x}-8 e^{-2 x}, u(0)=1, u^{\prime}(0)=3$$

In this section, several models are presented and the solution of the associated differential equation is given. Later in the chapter, we present methods for solving these differential equations. The growth of cancer tumors may be modeled by the Gompertz growth equation. Let \(M(t)\) be the mass of a tumor, for \(t \geq 0 .\) The relevant initial value problem is $$\frac{d M}{d t}=-r M(t) \ln \left(\frac{M(t)}{K}\right), M(0)=M_{0}$$ where \(r\) and \(K\) are positive constants and \(0

Solving initial value problems Solve the following initial value problems. $$y^{\prime}(x)=4 \sec ^{2} 2 x, y(0)=8$$

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