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In each of Problems I through 6 determine (without solving the problem) an interval in which the solution of the given initial value problem is certain to exist. $$ y^{\prime}+(\tan t) y=\sin t, \quad y(\pi)=0 $$

Short Answer

Expert verified
Question: Determine an interval in which the solution of the following initial value problem is certain to exist without actually solving the problem: \(y' + (\tan t)y = \sin t, y(\pi) = 0\). Answer: The solution of the given initial value problem is certain to exist on the interval \((\frac{\pi}{2}, \frac{3\pi}{2})\).

Step by step solution

01

Identify the given ODE and initial condition

We are given the first-order linear ODE: $$ y' + (\tan t)y = \sin t $$ and the initial condition: $$ y(\pi) = 0 $$
02

Analyze the continuity of the functions p(t) and q(t)

We have the functions \(p(t) = \tan t\) and \(q(t) = \sin t\). Both of these functions have points of discontinuity. In this case, \(\tan t\) is discontinuous at its asymptotes, which occur at \((2n + 1)\frac{\pi}{2}\) for all integers \(n\). \(\sin t\) is continuous for all real t.
03

Determine the open interval containing the initial value t = π

We need to find an open interval containing the initial value \(t = \pi\) in which both \(p(t)\) and \(q(t)\) are continuous. The discontinuities of the function \(p(t) = \tan t\) are of the form \((2n + 1)\frac{\pi}{2}\). Specifically, to the left of \(t = \pi\), the closest asymptote is \(t = \frac{3\pi}{2}\), and to the right, the closest asymptote is \(t = \frac{\pi}{2}\). Therefore, the open interval \((\frac{\pi}{2}, \frac{3\pi}{2})\) contains the initial value \(t = \pi\) and is a region where both \(p(t)\) and \(q(t)\) are continuous.
04

Conclusion

We have found an interval, \((\frac{\pi}{2}, \frac{3\pi}{2})\), in which the solution of the given initial value problem is certain to exist. This is because the functions \(p(t) = \tan t\) and \(q(t) = \sin t\) are continuous on this interval, which contains the initial value of \(t = \pi\). The Existence and Uniqueness Theorem guarantees a unique solution on this interval.

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Key Concepts

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

Initial Value Problem
An initial value problem consists of a differential equation accompanied by a specific value, known as the initial condition. This condition typically is in the form of a point on the solution curve that the resulting function must satisfy.
For example, in our exercise, the differential equation is given by: - \( y' + (\tan t)y = \sin t \) and the initial condition by: - \( y(\pi) = 0 \)
In essence, solving an initial value problem involves finding the function \( y(t) \) that not only satisfies the differential equation but also passes through the given point \((\pi, 0)\).
Initial value problems are crucial in many scientific and engineering fields as they often describe systems at a given starting point and help predict future behaviors.
First-order Linear ODE
A first-order linear ordinary differential equation (ODE) is a type of equation used to model various real-world scenarios, from physics to finance. It is called "first-order" because it involves only the first derivative of the unknown function. An ODE of this kind typically takes the form:
\[ y' + p(t)y = q(t) \]
In our case,
- \( p(t) = \tan(t) \) - \( q(t) = \sin(t) \)
The task is to find the function \( y(t) \) that satisfies this equation. First-order linear ODEs have various methods of solutions, such as the integrating factor method or matrix exponentials for systems, making them highly versatile in application.
The presence of functions \( p(t) \) and \( q(t) \) determines the path of solution and the techniques used. This type of ODE is foundational in understanding dynamic systems and processes.
Continuity of Functions
Continuity is a fundamental concept when discussing differential equations, particularly due to the Existence and Uniqueness Theorem. For the theorem to apply, specific functions within the equation must be continuous over a certain interval.
In our exercise, we have: - \( p(t) = \tan t \) - \( q(t) = \sin t \)
The function \( \sin t \) is continuous everywhere on the real line. However, \( \tan t \) is discontinuous at points \( (2n + 1)\frac{\pi}{2} \), where \( n \) is any integer.
This discontinuity caused by \( \tan t \) impacts where we can assure the existence of a unique solution. Thus, we focus on finding intervals where both functions are continuous. Understanding continuity helps in setting the stage for solving differential equations and is essential for ensuring predictions or models are reliable over specified domains.
Interval of Existence
The interval of existence refers to the region on the real number line where a unique solution to a differential equation is guaranteed by the Existence and Uniqueness Theorem.
In our particular problem, to find such an interval, both functions \( p(t) = \tan t \) and \( q(t) = \sin t \) must be continuous. We've identified that \( \tan t \) has discontinuities at every \( (2n + 1)\frac{\pi}{2} \).
Given the initial value \( t = \pi \), we determine the closest points of discontinuity are \( \frac{\pi}{2} \) and \( \frac{3\pi}{2} \). Thus, an open interval where both functions are continuous, and that includes \( t = \pi \), is \( (\frac{\pi}{2}, \frac{3\pi}{2}) \).
In this interval, a unique solution is assured by the theorem, indicating where the system precisely behaves according to our constraints. This step is critical in ensuring proper predictive capabilities in modeling scenarios via differential equations.

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Most popular questions from this chapter

Epidemics. The use of mathematical methods to study the spread of contagious diseases goes back at least to some work by Daniel Bernoulli in 1760 on smallpox. In more recent years many mathematical models have been proposed and studied for many different diseases. Deal with a few of the simpler models and the conclusions that can be drawn from them. Similar models have also been used to describe the spread of rumors and of consumer products. Suppose that a given population can be divided into two parts: those who have a given disease and can infect others, and those who do not have it but are susceptible. Let \(x\) be the proportion of susceptible individuals and \(y\) the proportion of infectious individuals; then \(x+y=1 .\) Assume that the disease spreads by contact between sick and well members of the population, and that the rate of spread \(d y / d t\) is proportional to the number of such contacts. Further, assume that members of both groups move about freely among each other, so the number of contacts is proportional to the product of \(x\) and \(y .\) since \(x=1-y\) we obtain the initial value problem $$ d y / d t=\alpha y(1-y), \quad y(0)=y_{0} $$ where \(\alpha\) is a positive proportionality factor, and \(y_{0}\) is the initial proportion of infectious individuals. (a) Find the equilibrium points for the differential equation (i) and determine whether each is asymptotically stable, semistable, or unstable. (b) Solve the initial value problem (i) and verify that the conclusions you reached in part (a) are correct. Show that \(y(t) \rightarrow 1\) as \(t \rightarrow \infty,\) which means that ultimately the disease spreads through the entire population.

Find an integrating factor and solve the given equation. $$ \left(3 x^{2} y+2 x y+y^{3}\right) d x+\left(x^{2}+y^{2}\right) d y=0 $$

Determine whether or not each of the equations is exact. If it is exact, find the solution. $$ \left(3 x^{2}-2 x y+2\right) d x+\left(6 y^{2}-x^{2}+3\right) d y=0 $$

Find the value of \(b\) for which the given equation is exact and then solve it using that value of \(b\). $$ \left(x y^{2}+b x^{2} y\right) d x+(x+y) x^{2} d y=0 $$

Consider the initial value problem $$ y^{\prime}=3 t^{2} /\left(3 y^{2}-4\right), \quad y(1)=0 $$ (a) Use the Euler formula ( 6) with \(h=0.1\) to obtain approximate values of the solution at \(t=1.2,1.4,1.6,\) and 1.8 . (b) Repeat part (a) with \(h=0.05\). (c) Compare the results of parts (a) and (b). Note that they are reasonably close for \(t=1.2,\) \(1.4,\) and 1.6 but are quite different for \(t=1.8\). Also note (from the differential equation) that the line tangent to the solution is parallel to the \(y\) -axis when \(y=\pm 2 / \sqrt{3} \cong \pm 1.155 .\) Explain how this might cause such a difference in the calculated values.

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