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

Solve the given differential equation. $$ x y^{\prime}=\left(1-y^{2}\right)^{1 / 2} $$

Short Answer

Expert verified
Question: Solve the first-order differential equation $xy' = (1-y^2)^{1/2}$, and find the general solution. Answer: The general solution for the given first-order differential equation is $y=\sin(\ln|x|+C)$.

Step by step solution

01

Separate the variables

Divide both sides by \(x(1-y^2)^{1/2}\) to separate the variables: $$ \frac{y'}{(1-y^2)^{1/2}}=\frac{1}{x} $$
02

Integrate both sides

Integrate both sides with respect to x: $$ \int\frac{y'}{(1-y^2)^{1/2}}dx=\int\frac{1}{x}dx $$ Now, let's integrate both sides. For the left side, we notice that the integral is an arctangent integral. For the right side, the integral results in a natural logarithm.
03

Perform the integration

We'll integrate the left side using arctangent and the right side using natural logarithm: $$ \int\frac{y'}{(1-y^2)^{1/2}}dx=\arcsin(y) + C_1 $$ $$ \int\frac{1}{x}dx=\ln|x| + C_2 $$ Now, we'll combine the constants of integration (C_1 and C_2) into one constant, C: $$ \arcsin(y) - \ln|x| = C $$
04

Solve for y

Now, let's solve for y to obtain an explicit formulation for our solution: $$ y=\sin(\ln|x|+C) $$ This is the general solution for the given first-order differential equation.

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.

Separation of Variables
Separation of Variables is a straightforward technique used to solve differential equations. The primary goal is to rearrange the equation such that each variable and its differential are on different sides of the equation.

In the example given, we started with the differential equation: \[ x y^{\prime} = \left(1-y^{2}\right)^{1/2} \] By dividing both sides of the equation by \( x(1-y^2)^{1/2} \), we successfully separated the variables, isolating terms involving \( y \) on one side and terms involving \( x \) on the other: \[ \frac{y'}{(1-y^2)^{1/2}} = \frac{1}{x} \] The trick is to arrange terms such that each variable can be integrated independently. This tool is particularly efficient when dealing with equations where direct integration is possible once separation is achieved.
Integration
Integration plays a crucial role in solving differential equations. Once a differential equation is separated into integrable components, the next task is to find antiderivatives.

In our case, we've transformed the original differential equation into: \[ \int \frac{y^\prime}{\sqrt{1-y^2}} \, dx = \int \frac{1}{x} \, dx \] The left-hand side can be recognized as a form that integrates into an arcsine function, while the right-hand side integrates into a natural logarithm. Integration for both sides is straightforward once they are in standard integrable forms:
  • The left-hand side: \( \int \frac{dy}{\sqrt{1-y^2}} \) is \( \arcsin(y) \).
  • The right-hand side: \( \int \frac{1}{x}dx \) is \( \ln|x| \).
Therefore, integration provides us with an interconnection between both expressions necessary for further steps toward solving the differential equation.
Arcsine Function
The Arcsine Function is a crucial component in solving certain types of differential equations, especially when the integral involves expressions of the form \( \frac{1}{\sqrt{1-y^2}} \).

In this exercise, noticing this form allows us to use the inverse trigonometric function, specifically, arcsine: \[ \int \frac{dy}{\sqrt{1-y^2}} = \arcsin(y) + C_1 \] The arcsine function, \( \arcsin(y) \), is the inverse of the sine function and ranges between -\( \frac{\pi}{2} \) and \( \frac{\pi}{2} \).

Recognizing patterns that resolve into such trigonometric inverses can greatly simplify the task of integration and lead to a concise form of the solution for the differential equation.
General Solution
The General Solution is the expression that incorporates all solutions of a differential equation. It typically includes arbitrary constants stemming from the integration process.

Once we've completed the integration in the exercise, we derive the following form: \[ \arcsin(y) - \ln|x| = C \] This expression holds for any permissible value of \( y \) and \( x \), giving a family of solutions which are encapsulated by the constant \( C \).

Converting this implicit form to an explicit form for \( y \), we derive the general solution: \[ y = \sin(\ln|x| + C) \] This step elucidates the behavior of solutions across different values of \( x \) and indicates how they are controlled by the constant \( C \). The general solution is critical in understanding the complete solution space of the differential equation and how particular solutions can be extracted based on specific initial conditions or constraints.

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 mass of \(0.25 \mathrm{kg}\) is dropped from rest in a medium offering a resistance of \(0.2|v|,\) where \(v\) is measured in \(\mathrm{m} / \mathrm{sec}\). $$ \begin{array}{l}{\text { (a) If the mass is dropped from a height of } 30 \mathrm{m} \text { , find its velocity when it hits the ground. }} \\ {\text { (b) If the mass is to attain a velocity of no more than } 10 \mathrm{m} / \mathrm{sec} \text { , find the maximum height }} \\ {\text { from which it can be dropped. }} \\ {\text { (c) Suppose that the resistive force is } k|v| \text { , where } v \text { is measured in } \mathrm{m} / \mathrm{sec} \text { and } k \text { is a }} \\ {\text { constant. If the mass is dropped from a height of } 30 \mathrm{m} \text { and must hit the ground with a }} \\ {\text { velocity of no more than } 10 \mathrm{m} / \mathrm{sec} \text { , determine the coefficient of resistance } k \text { that is required. }}\end{array} $$

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. Some diseases (such as typhoid fever) are spread largely by carriers, individuals who can transmit the disease, but who exhibit no overt symptoms. Let \(x\) and \(y,\) respectively, denote the proportion of susceptibles and carriers in the population. Suppose that carriers are identified and removed from the population at a rate \(\beta,\) so $$ d y / d t=-\beta y $$ Suppose also that the disease spreads at a rate proportional to the product of \(x\) and \(y\); thus $$ d x / d t=\alpha x y $$ (a) Determine \(y\) at any time \(t\) by solving Eq. (i) subject to the initial condition \(y(0)=y_{0}\). (b) Use the result of part (a) to find \(x\) at any time \(t\) by solving Eq. (ii) subject to the initial condition \(x(0)=x_{0}\). (c) Find the proportion of the population that escapes the epidemic by finding the limiting value of \(x\) as \(t \rightarrow \infty\).

Solve the differential equation $$ \left(3 x y+y^{2}\right)+\left(x^{2}+x y\right) y^{\prime}=0 $$ using the integrating factor \(\mu(x, y)=[x y(2 x+y)]^{-1}\). Verify that the solution is the same as that obtained in Example 4 with a different integrating factor.

Show that if \(\left(N_{x}-M_{y}\right) /(x M-y N)=R,\) where \(R\) depends on the quantity \(x y\) only, then the differential equation $$ M+N y^{\prime}=0 $$ has an integrating factor of the form \(\mu(x y)\). Find a general formula for this integrating factor.

Chemical Reactions. A second order chemical reaction involves the interaction (collision) of one molecule of a substance \(P\) with one molecule of a substance \(Q\) to produce one molecule of a new substance \(X ;\) this is denoted by \(P+Q \rightarrow X\). Suppose that \(p\) and \(q\), where \(p \neq q,\) are the initial concentrations of \(P\) and \(Q,\) respectively, and let \(x(t)\) be the concentration of \(X\) at time \(t\). Then \(p-x(t)\) and \(q-x(t)\) are the concentrations of \(P\) and \(Q\) at time \(t,\) and the rate at which the reaction occurs is given by the equation $$ d x / d t=\alpha(p-x)(q-x) $$ where \(\alpha\) is a positive constant. (a) If \(x(0)=0\), determine the limiting value of \(x(t)\) as \(t \rightarrow \infty\) without solving the differential equation. Then solve the initial value problem and find \(x(t)\) for any \(l .\) (b) If the substances \(P\) and \(Q\) are the same, then \(p=q\) and \(\mathrm{Eq}\). (i) is replaced by $$ d x / d t=\alpha(p-x)^{2} $$ If \(x(0)=0,\) determine the limiting value of \(x(t)\) as \(t \rightarrow \infty\) without solving the differential equation. Then solve the initial value problem and determine \(x(t)\) for any \(t .\)

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