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

Solving initial value problems Determine whether the following equations are separable. If so, solve the initial value problem. $$y^{\prime}(x)=y \cos x, y(0)=3$$

Short Answer

Expert verified
Question: Determine the particular solution of the initial value problem \(y^{\prime}(x) = y \cos x\) with the initial condition \(y(0)=3\). Answer: The particular solution for the given initial value problem is \(y(x) = 3 e^{\sin x}\).

Step by step solution

01

Determine if the equation is separable

A differential equation is separable if it can be written in the form: \(\frac{dy}{dx} = f(x)g(y)\). If the given equation \(y^{\prime}(x) = y \cos x\) is separable, then we should be able to rewrite it in the required form. Let \(f(x) = \cos x\) and \(g(y) = y\). Therefore, the given equation is indeed separable.
02

Rewrite the equation in terms of separate variables

To rewrite the equation in terms of separate variables, we need to divide both sides by \(dy\) and \(g(y)\) such that: $$\frac{dy}{y} = f(x) dx$$$$\frac{dy}{y} = \cos x dx$$
03

Integrate both sides

Now, we need to integrate both sides of the equation with respect to their respective variables: $$\int \frac{dy}{y} = \int \cos x dx$$$$\ln |y| = \sin x + C_{1}$$Where \(C_{1}\) is the integration constant.
04

Solve for y(x)

To determine y(x), take the exponent of both sides of the equation: $$y(x) = e^{\sin x + C_{1}}$$$$y(x) = e^{\sin x} e^{C_{1}}$$We can denote \(e^{C_{1}}\) as another constant \(C\), so the equation will look like:$$y(x) = C e^{\sin x}$$
05

Use the initial value \(y(0)=3\) to find the constant C

Now that we have a general solution for y(x), we can apply the initial value \(y(0)=3\) to find the constant C.$$3 = C e^{\sin (0)}$$$$3 = C e^{0}$$$$3 = C$$Thus, the particular solution of the initial value problem is:$$y(x) = 3 e^{\sin x}$$

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.

Separable Differential Equation
A differential equation is termed 'separable' when it can be expressed as the product of functions, each depending solely on one variable—either independent or dependent. For example, the equation \(y'(x) = y \cos x\) is separable because it can be written in the form \(\frac{dy}{dx} = f(x)g(y)\), where \(f(x) = \cos x\) and \(g(y) = y\).

To solve a separable equation, you rearrange it so that all terms involving one variable, such as \(y\), appear on one side of the equation and all terms involving another variable, like \(x\), appear on the other. This technique ensures each side only contains one variable, allowing us to integrate both sides separately.
  • Identify functions \(f(x)\) and \(g(y)\).
  • Rewrite differential as \(\frac{1}{g(y)} dy = f(x) dx\).
  • Perform integration on both sides to progress towards a solution.
Recognizing and manipulating separable equations is fundamental in solving many initial value problems. It allows the equation to be split and solved step-by-step using straightforward integration.
Integration
Integration is a powerful mathematical process used to calculate accumulated quantities, like areas under curves or the antiderivatives of functions. In the context of differential equations, integration helps us find functions whose derivative matches the given differential equation.

When we separate the variables in a differential equation, each side of the equation is set up to be integrated individually. For example, in the problem \(\frac{dy}{y} = \cos x dx\), we need to integrate each side:
  • Integrate \(\int \frac{dy}{y}\) to find \(\ln|y|\).
  • Integrate \(\int \cos x dx\) to find \(\sin x\).
After integrating, you will often introduce a constant of integration to account for any constant that might have disappeared during differentiation. This process turns the isolated derivatives into actual functions, one step closer to finding the particular solution.
Particular Solution
A particular solution of a differential equation is a specific solution derived from the general solution by applying given conditions or constraints, often initial values. In this context, the initial value provided helps pinpoint one unique solution out of the infinite possibilities.

After finding the general solution, such as \(y(x) = Ce^{\sin x}\), you can use the initial value \(y(0) = 3\) to compute \(C\).
  • Substitute \(x = 0\) and \(y = 3\) into the equation.
  • Solve for \(C\), resulting in \(C = 3\).
This procedure narrows down the solution to one that satisfies the initial condition, yielding \(y(x) = 3e^{\sin x}\) as the particular solution. This approach ensures the solution not only solves the differential equation but also aligns with specified initial conditions.
Constant of Integration
The constant of integration is an essential concept in calculus representing any constant added to the antiderivative during integration. It emerges because differentiation obliterates constants, meaning when we work backward through integration, we must account for any original constant that might have existed.

In our problem, once each side of the separated differential equation was integrated, the results included \( \ln |y| = \sin x + C_1 \). Here, \(C_1\) is an arbitrary constant introduced during integration. This constant signifies the family of curves that satisfy our differential equation.
  • Constant arises in indefinite integration.
  • Represents an infinite number of potential solutions.
When dealing with initial value problems, exact values are often given, enabling us to address this "degree of freedom" and find a unique solution. The constant's value is determined by applying initial or boundary conditions as shown by setting \(y(0) = 3\) to solve for \(C\), which led to the particular solution.

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

Solving initial value problems Solve the following initial value problems. $$y^{\prime \prime}(t)=t e^{\prime}, y(0)=0, y^{\prime}(0)=1$$

A physiological model A common assumption in modeling drug assimilation is that the blood volume in a person is a single compartment that behaves like a stirred tank. Suppose the blood volume is a four-liter tank that initially has a zero concentration of a particular drug. At time \(t=0,\) an intravenous line is inserted into a vein (into the tank) that carries a drug solution with a concentration of \(500 \mathrm{mg} / \mathrm{L} .\) The inflow rate is \(0.06 \mathrm{L} / \mathrm{min} .\) Assume the drug is quickly mixed thoroughly in the blood and that the volume of blood remains constant. a. Write an initial value problem that models the mass of the drug in the blood, for \(t \geq 0\) b. Solve the initial value problem, and graph both the mass of the drug and the concentration of the drug. c. What is the steady-state mass of the drug in the blood? d. After how many minutes does the drug mass reach \(90 \%\) of its steady-state level?

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 \(y(0)=1\). $$y^{\prime}(t)=y(y-3)$$

Properties of stirred tank solutions a. Show that for general positive values of \(R, V, C_{i},\) and \(m_{0},\) the solution of the initial value problem $$m^{\prime}(t)=-\frac{R}{V} m(t)+C_{i} R, \quad m(0)=m_{0}$$is \(m(t)=\left(m_{0}-C_{i} V\right) e^{-R t / V}+C_{i} V\) b. Verify that \(m(0)=m_{0}\) c. Evaluate \(\lim _{t \rightarrow \infty} m(t)\) and give a physical interpretation of the result. d. Suppose \(m_{0}\) and \(V\) are fixed. Describe the effect of increasing \(R\) on the graph of the solution.

Solving initial value problems Solve the following initial value problems. $$y^{\prime}(t)=1+e^{t}, y(0)=4$$

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