/*! 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 30 As stated in this section, the s... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

As stated in this section, the separation of equation (2) on page 42 requires division by \( p(y) \), and this may disguise the fact that the roots of the equation \( p(y)=0 \) are actually constant solutions to the differential equation. (a) To explore this further, separate the equation $$ \frac{d y}{d x}=(x-3)(y+1)^{2 / 3} $$ to derive the solution, $$ y=-1+\left(x^{2} / 6-x+C\right)^{3} $$ (b) Show that \( y \equiv-1 \) satisfies the original equation \( d y / d x=(x-3)(y+1)^{2 / 3} \) (c) Show that there is no choice of the constant \( C \) that will make the solution in part (a) yield the solution \( y \equiv-1 \) Thus, we lost the solution \( y=-1 \) when we divided by \((y+1)^{2 / 3}\).

Short Answer

Expert verified
The solution to the given differential equation is \(y = -1 + (x^2/6 -x +C)^3\). The solution \(y \equiv -1\) satisfies the original differential equation. However, there's no choice of constant \(C\) that would make the solution fit \(y \equiv -1\), implying that the solution was lost in the process of dividing by \((y+1)^{2/3}\).

Step by step solution

01

Separate the equation

First, we need to separate the variables. The given differential equation is \(\frac{dy}{dx} = (x-3)(y+1)^{2/3}\). To separate, we consider \(dy/(y+1)^{2/3} = (x-3)dx\).
02

Integrate the equation

Next, integrate both sides with respect to their respective variables. This results in \(\int dy/(y+1)^{2/3} = \int (x-3) dx\). Solving the integrals ends up with \(3(y+1)^{1/3} = x^2/2 - 3x + C.\)
03

Derive the solution

After the integration, arrange the solution in the form of \(y\). That is, \(y = -1 + (x^2/6 -x +C)^3\).
04

Verify that \(y \equiv -1\)

substituting \(y \equiv -1\) into the original equation, we get \(dy/dx = (x-3)(-1+1)^{2/3}\) which simplifies to 0 = 0, indicating that \(y \equiv -1\) is indeed a solution.
05

Realize the lost solution

Lastly, the solution that we found could not be made to fit \(y \equiv -1\) regardless of the constant \(C\) chosen. This highlights the lost solution when we divided by \((y+1)^{2/3}\)

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.

Differential Equations
Differential equations are mathematical expressions that relate a function with its derivatives. They are used to describe a variety of phenomena such as movement, growth, and decay across different fields like physics, biology, and engineering.
Their structure often involves derivatives, which are rates of change, helping us understand dynamic systems.
  • The simplest form is an ordinary differential equation which involves functions of one variable and their derivatives.
  • Partial differential equations deal with functions of multiple variables.
  • Solving these equations involves finding a function or a set of functions that satisfy the given relationship.
In our exercise, we started with the differential equation \( \frac{dy}{dx} = (x-3)(y+1)^{2/3} \), which means we're looking at how the variable \( y \) changes with respect to \( x \).
Solving such equations often requires techniques like separation of variables, which we'll explore a bit further.
Constant Solutions
Constant solutions are specific solutions to differential equations where the function's value does not change. This means the derivative of the function is zero.
In other words, constant solutions occur when the rate of change of the function is not affected by any variable changes.
  • They are crucial in identifying stability within systems.
  • In our problem, \( y \equiv -1 \) represents a constant solution, implying no change in the \( y \) value as \( x \) varies.
  • To verify, substitute \( y = -1 \) back into the original differential equation. If both sides simplify to 0, it confirms the solution is constant.
Constant solutions can be easily overlooked during algebraic manipulation but serve as important solutions providing insights into the system behavior, such as equilibria in physical systems.
Integration
Integration is the mathematical process of finding the antiderivative, which is essentially the reverse of taking a derivative.
It plays a key role in solving differential equations by allowing us to find functions given their rates of change.
  • When dealing with separable differential equations, we often use integration to find \( y \) in terms of \( x \).
  • In our step-by-step solution, we integrated both sides of the equation \( \int \frac{dy}{(y+1)^{2/3}} = \int (x-3) dx \), resulting in a new relationship involving \( y \) and \( x \).
  • After integration, rearranging gives us our solution: \( y = -1 + (x^2/6 - x + C)^3 \), where \( C \) is the constant of integration.
Careful integration helps us derive the general solution and often reveals information about the constants that particularize specific solutions, yet it can also lead to challenges, including potential lost solutions.
Lost Solutions in Separation of Variables
Using separation of variables is a common method for solving differential equations.
However, it involves isolating each variable on a different side of the equation before integrating, which might sometimes overlook important solutions.
  • This occurs particularly when you divide by an expression that could equal zero. Doing so may eliminate valid solutions from consideration.
  • In our exercise, the division by \( (y+1)^{2/3} \) caused us to ignore the solution \( y = -1 \).
  • This is because when \( y+1 \) equates to zero, division results in an undefined state, potentially masking certain solutions.
  • Thus, it's pivotal to consider these points where the denominator could be zero separately to ensure no solutions are lost.
Being mindful of these challenges prevents misunderstandings and ensures a more comprehensive grasp of the problem's solution space.

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

Compound Interest. If \(P(t)\) is the amount of dollars in a savings bank account that pays a yearly interest rate of \(r \%\) compounded continuously, then $$\frac{d P}{d t}=\frac{r}{100} P, \quad t$$ in years. Assume the interest is 5\(\%\) annually, \(P(0)=\$ 1000,\) and no monies are withdrawn. (a) How much will be in the account after 2 yr? (b) When will the account account every 12 months, (c) If \(\$ 1000\) is added to the account every 12 months, how much will be in the account after 3\(\frac{1}{2}\) yr?

Newton's Law of Cooling. According to Newton's law of cooling, if an object at temperature \( T \) is immersed in a medium having the constant temperature \( M \), then the rate of change of \( T \) is proportional to the difference of temperature \( M-T \). This gives the differential equation $$ d T / d t=k(M-T) $$ (a) Solve the differential equation for \( T \) (b) A thermometer reading \( 100^{\circ} \mathrm{F} \) is placed in a medium having a constant temperature of \( 70^{\circ} \mathrm{F} \). After 6 min, the thermometer reads \( 80^{\circ} \mathrm{F} \). What is the reading after 20 min? (Further applications of Newton's law of cooling appear in Section 3.3.)

Consider the initial value problem $$ \frac{d y}{d x}+\sqrt{1+\sin ^{2} x} y=x, \quad y(0)=2 $$. (a) Using definite integration, show that the integrating factor for the differential equation can be written as $$ \mu(x)=\exp \left(\int_{0}^{x} \sqrt{1+\sin ^{2} t} d t\right) $$ and that the solution to the initial value problem is $$ y(x)=\frac{1}{\mu(x)} \int_{0}^{x} \mu(s) s d s+\frac{2}{\mu(x)} $$. (b) Obtain an approximation to the solution at \( x=1 \) by using numerical integration (such as Simpson's rule, Appendix C) in a nested loop to estimate values of \( \mu(x) \) and, thereby, the value of $$ \int_{0}^{1} \mu(s) s d s $$. [Hint: First, use Simpson's rule to approximate \( \mu(x) \) at \( x=0.1,0.2, \dots, 1 \). Then use these values and apply Simpson's rule again to approximate \( \int_{0}^{1} \mu(s) s d s . ] \) (c) Use Euler's method (Section 1.4) to approximate the solution at \( x=1 \), with step sizes \( h=0.1 \) and 0.05. [A direct comparison of the merits of the two numerical schemes in parts (b) and (c) is very complicated, since it should take into account the number of functional evaluations in each algorithm as well as the inherent accuracies.]

Mixing. Suppose a brine containing 0.3 kilogram (kg) of salt per liter (L) runs into a tank initially filled with 400 L of water containing 2 kg of salt. If the brine enters at 10 L/min, the mixture is kept uniform by stirring, and the mixture flows out at the same rate. Find the mass of salt in the tank after 10 min (see Figure 2.4). [Hint: Let A denote the number of kilograms of salt in the tank at t min after the process begins and use the fact that rate of increase in $$A =$$ rate of input - rate of exit. A further discussion of mixing problems is given in Section 3.2.]

Free Fall. In Section 2.1, we discussed a model for an object falling toward Earth. Assuming that only air resistance and gravity are acting on the object, we found that the velocity \( \boldsymbol{v} \) must satisfy the equation $$ m \frac{d v}{d t}=m g-b v $$ where \( m \) is the mass, \( \boldsymbol{g} \) is the acceleration due to gravity, and \( b>0 \) is a constant (see Figure 2.1). If \( m=100 \mathrm{kg} \), \( g=9.8 \mathrm{m} / \mathrm{sec}^{2}, b=5 \mathrm{kg} / \mathrm{sec} \) and \( v(0)=10 \mathrm{m} / \mathrm{sec} \), solve for \( v(t) \). What is the limiting (i.e., terminal) velocity of the object?

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.