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In each exercise, (a) Show that the given differential equation is not exact. (b) Multiply the equation by the function \(\mu\), if it is provided, and show that the resulting differential equation is exact. If the function \(\mu\) is not given, use the ideas of Exercise 22 to determine \(\mu\). (c) Solve the given problem, obtaining an explicit solution if possible. \(t y^{2} y^{\prime}+2 y^{3}=1, \quad y(1)=-1\)

Short Answer

Expert verified
Short Answer: The given differential equation is \(t y^2 y' + 2y^3 = 1\), and it is not exact. After finding the integrating factor \(\mu(t) = t^5\), we multiply the differential equation by \(\mu(t)\) to obtain an exact equation \((t^6 y^2) y' + 2t^5y^3 = t^5\). The solution to this exact equation is \(t^5y^4 = \frac{1}{7}t^7y^2\). However, applying the initial condition \(y(1) = -1\) leads to a contradiction, which means there is no explicit solution for the given problem under the given initial condition.

Step by step solution

01

Checking for exactness and finding integrating factor (\(\mu\))

First, let's identify the given differential equation, which is \(t y^2 y' + 2y^3 = 1\). To check whether this equation is exact or not, let's identify \(M(t, y) = 2y^3\) and \(N(t, y) = ty^2\). We need to find the partial derivatives \(\frac{\partial M}{\partial y}\) and \(\frac{\partial N}{\partial t}\), and check for exactness: \(\frac{\partial M}{\partial y} = 6y^2\) \(\frac{\partial N}{\partial t} = y^2\) Since \(\frac{\partial M}{\partial y} \neq \frac{\partial N}{\partial t}\), the given equation is not exact. So, we need to find an integrating factor, \(\mu\). According to the ideas of Exercise 22, if \(\mu\) depends only on \(t\), then \(\frac{\mu_t}{\mu} = \frac{\partial M/\partial y - \partial N/\partial t}{N}\). Let's find \(\mu_t\): \(\frac{\mu'_t}{\mu} = \frac{6y^2 - y^2}{ty^2} = \frac{5}{t}\) Integrating both sides with respect to \(t\): \(\int \frac{\mu'_t}{\mu} dt = \int \frac{5}{t} dt\) \(\ln |\mu| = 5 \ln |t| + C\) Now, we find the integrating factor \(\mu\): \(\mu(t) = t^5\)
02

Multiply by integrating factor and find exact equation

Let's multiply the given differential equation by the integrating factor, \(\mu(t) = t^5\), and obtain the exact equation: \(t^5(t y^2 y' + 2y^3) = t^5\) \((t^6 y^2) y' + 2t^5y^3 = t^5\) Now, check for exactness by finding partial derivatives of new \(M(t, y) = 2t^5y^3\) and \(N(t, y) = t^6y^2\): \(\frac{\partial M}{\partial y} = 6t^5y^2\) \(\frac{\partial N}{\partial t} = 6t^5y^2\) Since \(\frac{\partial M}{\partial y} = \frac{\partial N}{\partial t}\), the equation is now exact.
03

Solve the exact differential equation and apply initial condition

The exact differential equation is \((t^6 y^2) y' + 2t^5y^3 = t^5\). To solve the exact equation, we integrate \(M(t, y)\) with respect to \(y\), and \(N(t, y)\) with respect to \(t\): \(\int M(t, y) dy = \int 2t^5y^3 dy = t^5y^4 + c_1(t)\) \(\int N(t, y) dt = \int t^6y^2 dt = \frac{1}{7}t^7y^2 + c_2(y)\) Comparing these two expressions, we can infer that \(c_1(t) = 0\) and \(c_2(y) = 0\). Thus, the solution to the exact equation is: \(t^5y^4 = \frac{1}{7}t^7y^2\) Now, applying the initial condition \(y(1) = -1\), we get: \(1(-1)^4 = \frac{1}{7}(1)^7(-1)^2\) \(1 = \frac{1}{7}\) This is a contradiction, which means that there is no explicit solution for the given problem under the given initial condition.

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Key Concepts

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

Integrating Factor
Exact differential equations can sometimes be difficult to solve when they aren't in an exact form. That's where an integrating factor can save the day. An integrating factor is a function that, when multiplied by a non-exact differential equation, transforms it into an exact one. This allows us to apply techniques for solving exact equations.
To find an integrating factor, often denoted as \(\mu(t)\), you must look for a function that, when multiplied by the given differential equation, makes the equation satisfy the exactness condition. In this scenario, we used the discrepancy between the partial derivatives of the components of the differential equation to find \(\mu\). The critical formula to remember is:
  • \(\frac{\mu_t}{\mu} = \frac{\partial M/\partial y - \partial N/\partial t}{N}\)
Once you determine the form of the integrating factor by integrating with respect to \(t\), you get a new form of the differential equation. With the integrating factor \(\mu(t) = t^5\), it simplified our equation to an exact form so we could proceed to solve it.
Partial Derivatives
In mathematics, particularly calculus, partial derivatives are a way to show how a function changes as one of its dimensions changes, while the other dimensions are held constant. When dealing with differential equations, partial derivatives are essential in checking the exactness of an equation.
For an equation to be considered exact, the partial derivatives of its terms must satisfy the condition:
  • \(\frac{\partial M}{\partial y} = \frac{\partial N}{\partial t}\)
Here, \(M(t, y)\) and \(N(t, y)\) represent two different components of the differential equation. In our example, by calculating the partial derivative \(\frac{\partial M}{\partial y} = 6y^2\) and \(\frac{\partial N}{\partial t} = y^2\), it's clear that the two are not equal, indicating the original differential equation is not exact. Therefore, using partial derivatives is a step toward identifying the need for an integrating factor.
Initial Condition
An initial condition in differential equations is like the starting point of your favorite hiking trail; it tells you where to begin the solution process. An initial condition is often given as a specific value of the function or its derivatives at a particular point. This allows you to find a unique solution to a differential equation rather than a whole family of solutions.
In the problem we are considering, the initial condition is given as \(y(1) = -1\). When solving exact equations, after integrating and forming the general solution of the equation, you apply the initial condition to solve for any constants that arise during the integration process.
Unfortunately, in our exercise, applying the initial condition revealed a contradiction, \(1 = \frac{1}{7}\). This tells us that no solution satisfies both the differential equation and the initial condition. Thus, understanding and correctly applying initial conditions is crucial in ensuring that the solutions obtained are feasible.

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Most popular questions from this chapter

Consider a population modeled by the initial value problem $$ \frac{d P}{d t}=(1-P) P+M, \quad P(0)=P_{0} $$ where the migration rate \(M\) is constant. [The model (8) is derived from equation (6) by setting the constants \(r\) and \(P_{*}\) to unity. We did this so that we can focus on the effect \(M\) has on the solutions.] For the given values of \(M\) and \(P(0)\), (a) Determine all the equilibrium populations (the nonnegative equilibrium solutions) of differential equation (8). As in Example 1, sketch a diagram showing those regions in the first quadrant of the \(t P\)-plane where the population is increasing \(\left[P^{\prime}(t)>0\right]\) and those regions where the population is decreasing \(\left[P^{\prime}(t)<0\right]\). (b) Describe the qualitative behavior of the solution as time increases. Use the information obtained in (a) as well as the insights provided by the figures in Exercises 11-13 (these figures provide specific but representative examples of the possibilities). $$ M=-\frac{1}{4}, \quad P(0)=1 $$

A tank initially holds 500 gal of a brine solution having a concentration of \(0.1 \mathrm{lb}\) of salt per gallon. At some instant, fresh water begins to enter the tank at a rate of 10 \(\mathrm{gal} / \mathrm{min}\) and the well- stirred mixture leaves at the same rate. How long will it take before the concentration of salt is reduced to \(0.01 \mathrm{lb} / \mathrm{gal}\) ?

State an initial value problem, with initial condition imposed at \(t_{0}=2\), having implicit solution \(y^{3}+t^{2}+\sin y=4\).

Suppose that at some initial time the pendulum is located at angle \(\theta_{0}\) with an angular velocity \(d \theta / d t=\omega_{0}\) radians/sec. (a) Equation (15) is a second order differential equation. Rewrite it as a first order separable equation by adopting angle \(\theta\) as the independent variable, using the fact that $$ \theta^{\prime \prime}=\frac{d}{d t}\left(\frac{d \theta}{d t}\right)=\frac{d \omega}{d t}=\frac{d \omega}{d \theta} \frac{d \theta}{d t}=\omega \frac{d \omega}{d \theta} . $$ Complete the specification of the initial value problem by specifying an appropriate initial condition. (b) Obtain the implicit solution $$ m l^{2} \frac{\omega^{2}}{2}-m g l \cos \theta=m l^{2} \frac{\omega_{0}^{2}}{2}-m g l \cos \theta_{0^{-}} $$ The pendulum is a conservative system; that is, energy is neither created nor destroyed. Equation (16) is a statement of conservation of energy. At a position defined by the angle \(\theta\), the quantity \(m l^{2} \omega^{2} / 2\) is the kinetic energy of the pendulum while the term \(-m g l \cos \theta\) is the potential energy, referenced to the horizontal position \(\theta=\pi / 2\). The constant right-hand side is the total initial energy. (c) Determine the angular velocity at the instant the pendulum reaches the vertically downward position, \(\theta=0\). Express your answer in terms of the constants \(\omega_{0}\) and \(\theta_{0}\).

(a) Obtain an implicit solution and, if possible, an explicit solution of the initial value problem. (b) If you can find an explicit solution of the problem, determine the \(t\)-interval of existence. $$ y^{\prime}-t y^{3}=0, \quad y(0)=2 $$

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