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A differential equation of the form $$ y^{\prime}=p_{1}(t)+p_{2}(t) y+p_{3}(t) y^{2} $$ is known as a Riccati equation. \({ }^{5}\) Equations of this form arise when we model onedimensional motion with air resistance; see Section 2.9. In general, this equation is not separable. In certain cases, however (such as in Exercises 24-26), the equation does assume a separable form. Solve the given initial value problem and determine the \(t\)-interval of existence. $$ y^{\prime}=t\left(5+4 y+y^{2}\right), \quad y(0)=-3 $$

Short Answer

Expert verified
Question: Solve the initial value problem involving the Riccati equation: \(ty' = 5t + 4ty + ty^2\) for \(y(0) = -3\). Determine the t-interval of existence for the solution. Answer: The solution of the initial value problem is given by: \(\left|\frac{1+y}{5+y}\right|^{1/4} = -\sqrt[4]{2}e^t\). The t-interval of existence is \((-\infty, +\infty)\).

Step by step solution

01

Check if the equation is separable

Let's first rewrite the given equation in its standard form by dividing both sides by t, so that we can check if it's separable: $$ y' = 5 + 4y + y^2 $$ In this case, the differential equation becomes separable, as we can write it as $$ y' = (1+y)(5+ y) $$
02

Solve the separable equation

Now, since we have a separable equation, we can separate the variables and integrate both sides: $$ \frac{dy}{(1+y)(5+y)} = dt $$ Next we integrate both sides with respect to their respective variables: $$ \int \frac{dy}{(1+y)(5+y)} = \int dt $$
03

Performing partial fractions decomposition

Now we perform partial fraction decomposition to integrate the left-hand side. For that, we will represent the integrand in terms of its partial fractions: $$ \frac{1}{(1+y)(5+y)} = \frac{A}{1+y} + \frac{B}{5+y} $$ Solving for A and B using a system of linear equations, we find that: $$ A = -\frac{1}{4}, \quad B = \frac{1}{4} $$ Now, we can rewrite the fractions as: $$ \int\left(-\frac{1}{4}\frac{1}{1+y}+\frac{1}{4}\frac{1}{5+y}\right)dy = \int dt $$
04

Integrating both sides

Now we integrate both sides: $$ -\frac{1}{4}\int\frac{1}{1+y}dy+\frac{1}{4}\int\frac{1}{5+y}dy = \int dt $$ We have: $$ -\frac{1}{4}\ln|1+y|+\frac{1}{4}\ln|5+y|=t+C $$
05

Finding the general solution

Taking the exponent of both sides and simplifying, we have: $$ \left|\frac{1+y}{5+y}\right|^{1/4} = e^{t+C} $$ Replacing \(e^C\) by another constant \(K\), we have: $$ \left|\frac{1+y}{5+y}\right|^{1/4} = Ke^t $$
06

Applying the initial condition

Now apply the initial condition \(y(0) = -3\): $$ \left|\frac{1-3}{5-3}\right|^{1/4} = K\cdot e^{0} $$ This gives us \(K=-\sqrt[4]{2}\).
07

Finding the particular solution

Now, we plug the value of K back into the general solution: $$ \left|\frac{1+y}{5+y}\right|^{1/4} = -\sqrt[4]{2}e^t $$ We find the t-interval of existence for the solution is \((-\infty, +\infty)\) as there aren't any specific restrictions on t in the above expression.

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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 (IVP) in the context of differential equations is a problem where not only a differential equation is provided, but also the value of the unknown function at a particular point, which is known as the initial condition.

Specifically, in the case of the Riccati differential equation provided, the IVP requires us to find a solution to the equation that satisfies the condition \(y(0) = -3\). This additional piece of information is crucial because it pinpoints exactly one particular solution out of the potentially infinite family of solutions that satisfy the differential equation.

When solving an IVP, the objective is first to find the general solution to the differential equation, and then use the initial condition to find the particular solution that exactly fits the initial value. The initial condition essentially determines the constant of integration in the solution process, turning a broad solution into a precise one. The existence and uniqueness theorem for first-order IVPs also tells us that, under suitable conditions, there is one and only one solution to an IVP, which will exist in some interval around the initial point.
Separable Differential Equations
In differential equations, a separable equation is one that can be rewritten in a way that allows all terms involving the independent variable (usually \(t\)) to be separated on one side of the equation and all terms involving the dependent variable (usually \(y\)) on the other.

For example, the differential equation \(y' = t(5 + 4y + y^2)\) from the exercise can be manipulated into a separable form as follows:\[\frac{{dy}}{{dt}} = (1+y)(5+y)\]By rearranging the terms, the variables can be separated:\[\frac{{dy}}{{(1+y)(5+y)}} = dt\]Separation of variables is a powerful technique because it transforms the problem of solving a differential equation into a problem of integrating two separate functions of single variables. After separation, we integrate both sides with respect to their respective variables to find the general solution. The separable form is especially valuable when the differential equation corresponds to a physically interpretable process, often simplifying complex dynamic systems into easier-to-solve integrals.
Partial Fraction Decomposition
The method of Partial Fraction Decomposition is used in integral calculus to simplify complex rational expressions before integrating. It's particularly useful when dealing with integrals of fractions that have polynomial expressions in the denominator.

For the given exercise, the integrand \(\frac{1}{{(1+y)(5+y)}}\) is a rational expression that is not straightforward to integrate. Through partial fraction decomposition, we break it down into simpler terms that can be easily integrated:\[\frac{1}{{(1+y)(5+y)}} = \frac{A}{{1+y}} + \frac{B}{{5+y}}\]To find the constants \(A\) and \(B\), we'll set up and solve a system of equations by equating coefficients or plugging in suitable values for \(y\) that simplify the equation.

Once \(A\) and \(B\) are determined, the integral becomes a sum of simpler integrals that can often be solved by direct integration or by recognizing them as standard integral forms. Through this process, we are able to integrate complex rational functions that might otherwise be difficult to tackle.

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Most popular questions from this chapter

Use the ideas of Exercise 32 to solve the given initial value problem. Obtain an explicit solution if possible. $$ y^{\prime}=(t+y)^{2}-1, \quad y(1)=2 $$

Consider a chemical reaction of the form \(A+B \rightarrow C\), in which the rates of change of the two chemical reactants, \(A\) and \(B\), are described by the two differential equations $$ A^{\prime}=-k A B, \quad B^{\prime}=-k A B, $$ where \(k\) is a positive constant. Assume that 5 moles of reactant \(A\) and 2 moles of reactant \(B\) are present at the beginning of the reaction. (a) Show that the difference \(A(t)-B(t)\) remains constant in time. What is the value of this constant? (b) Use the observation made in (a) to derive an initial value problem for reactant \(A\). (c) It was observed, after the reaction had progressed for \(1 \mathrm{sec}\), that 4 moles of reactant \(A\) remained. How much of reactants \(A\) and \(B\) will be left after \(4 \sec\) of reaction time?

Let \(S(t)\) represent the amount of a chemical reactant present at time \(t, t \geq 0\). Assume that \(S(t)\) can be determined by solving the initial value problem $$ S^{\prime}=-\frac{\alpha S}{K+S}, \quad S(0)=S_{0}, $$ where \(\alpha, K\), and \(S_{0}\) are positive constants. Obtain an implicit solution of the initial value problem. (The differential equation, often referred to as the Michaelis-Menten equation, arises in the study of biochemical reactions.)

Active oxygen and free radicals are believed to be exacerbating factors in causing cell injury and aging in living tissue. \({ }^{1}\) These molecules also accelerate the deterioration of foods. Researchers are therefore interested in understanding the protective role of natural antioxidants. In the study of one such antioxidant (Hsian-tsao leaf gum), the antioxidation activity of the substance has been found to depend on concentration in the following way: $$ \frac{d A(c)}{d c}=k\left[A^{*}-A(c)\right], \quad A(0)=0 . $$ In this equation, the dependent variable \(A\) is a quantitative measure of antioxidant activity at concentration \(c\). The constant \(A^{*}\) represents a limiting or equilibrium value of this activity, and \(k\) is a positive rate constant. (a) Let \(B(c)=A(c)-A^{*}\) and reformulate the given initial value problem in terms of this new dependent variable, \(B\). (b) Solve the new initial value problem for \(B(c)\) and then determine the quantity of interest, \(A(c)\). Does the activity \(A(c)\) ever exceed the value \(A^{*}\) ? (c) Determine the concentration at which \(95 \%\) of the limiting antioxidation activity is achieved. (Your answer is a function of the rate constant \(k\).)

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 \(\theta_{0}\).

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