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Separate variables and use partial fractions to solve the initial value problems in Problems \(1-8 .\) Use either the exact solution or a computer- generated slope field to sketch the graphs of several solutions of the given differential equation, and highlight the indicated particular solution. $$ \frac{d x}{d t}=9-4 x^{2}, x(0)=0 $$

Short Answer

Expert verified
The particular solution is \( x = \frac{3}{2}\tanh(3t) \).

Step by step solution

01

Rearrange the Differential Equation

Start with the given differential equation \( \frac{d x}{d t}=9-4 x^{2} \). To use separation of variables, rewrite this as \( \frac{d x}{9-4 x^{2}} = dt \). This forms a separable differential equation, where terms involving \(x\) are on one side, and terms involving \(t\) are on the other.
02

Integrate Both Sides

Integrate both sides of the equation. The left side is \( \int \frac{d x}{9-4 x^{2}} \) and the right side is \( \int dt \). This results in \( \int \frac{d x}{9-4 x^{2}} = t + C \), where \( C \) is the integration constant.
03

Use Partial Fractions

To integrate \( \frac{1}{9-4x^2} \), recognize it as the form which allows for partial fraction decomposition. Rewrite \( \frac{1}{9-4x^2} \) as \( \frac{1}{9-(2x)^2} \), which can be integrated using the inverse hyperbolic tangent function formula: \( \int \frac{1}{a^2-x^2}dx = \frac{1}{a}\text{arctanh}\frac{x}{a} + C \). Here, \(a=\frac{3}{2}\), so integrating gives \( \frac{1}{3}\text{arctanh}\frac{2x}{3} = t + C \).
04

Solve for x

Solve \( \text{arctanh} \frac{2x}{3} = 3t + C \) for \(x\) by using the inverse hyperbolic function property: \( \frac{2x}{3} = \tanh(3t+C) \), thus \( x = \frac{3}{2}\tanh(3t+C) \).
05

Apply Initial Condition

Apply the initial condition \( x(0) = 0 \). Substitute into the equation to find \( C \). With \( 0 = \frac{3}{2}\tanh(C) \), \( \tanh(C) = 0 \), hence \( C = 0 \). So, the particular solution is \( x = \frac{3}{2}\tanh(3t) \).

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Key Concepts

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

Separation of Variables
In solving differential equations, one of the most effective and common techniques is the separation of variables. This method is handy for first-order differential equations and involves rearranging the equation so that each variable and its derivative are placed on opposite sides of the equation. This separation allows us to easily integrate each side with respect to its appropriate variable.

Consider the given differential equation: \( \frac{d x}{d t} = 9 - 4 x^2 \). Initially, all terms are mixed. By utilizing separation of variables, we rearrange the terms to get \( \frac{d x}{9-4 x^{2}} = dt \). This arrangement places all x-dependent terms (including the differential \( dx \)) on one side and \( dt \) on the other, creating a separable form. The ease of integration is achieved through this deception, allowing us to proceed methodically.
Partial Fractions
Partial fraction decomposition is a powerful tool in calculus, especially useful for integrating functions that are not straightforward polynomial forms. When confronting a fraction that cannot be integrated directly, like \( \frac{1}{9-4x^2} \), we look for opportunities to decompose it into simpler, integrable parts.

In this exercise, we identify this as an instance where the technique of inverse trigonometric functions can be readily applied. We rearrange as \( \frac{1}{9-(2x)^2} \) to recognize it as part of the inverse hyperbolic tangent function formula: \( \int \frac{1}{a^2-x^2}dx = \frac{1}{a}\text{arctanh}\frac{x}{a} + C \). Here, \( a \) is \( \frac{3}{2} \), making it possible to integrate and attain a result that imminently aids in solving the differential equation.
Initial Value Problems
Initial value problems (IVPs) are crucial in determining specific solutions to differential equations. Such problems provide a snapshot or starting value, typically denoted by a condition such as \( x(0) = 0 \), which we use to find the constant of integration, \( C \).

Applying this to our differential equation, after obtaining the general solution \( x = \frac{3}{2}\tanh(3t + C) \), we substitute the initial value \( x(0) = 0 \). Given \( 0 = \frac{3}{2}\tanh(C) \), it follows that \( \tanh(C) \) must be zero, thereby making \( C = 0 \). This step refines our solution to a specific function fitting the initial condition perfectly: \( x = \frac{3}{2}\tanh(3t) \), painting not just any curve but the precise response to this initial standpoint.
Integration Techniques
Diverse integration techniques are pivotal in solving differential equations, allowing the manipulation and solving of complex integrals. Here, choosing the right method is paramount. Whether utilizing simple antiderivatives, partial fraction decomposition, or specific function forms, these techniques are the backbone of calculus problem-solving.

In this problem, two integration avenues are seamlessly interwoven. Separating variables sets the scene for integrating \( \int \frac{d x}{9-4 x^{2}} \) and \( \int dt \). On the left side, recognizing its likeness to a hyperbolic tangent setup, we employ the formula for inverse hyperbolic functions to manage the integral efficiently. Meanwhile, integrating \( dt \) is straightforward, leading to \( t + C \).

Through these intertwined techniques, we navigate from a complex equation to a comprehensive solution, rendering the once formidable problem approachable and clear.

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Most popular questions from this chapter

Find the exact solution of the given initial value problem. Then apply Euler's method twice to approximate (to four decimal places) this solution on the given interval, first with step size \(h=0.01\), then with step size \(h=0.005 .\) Make a table showing the approximate values and the actual value, together with the percentage error in the more accurate approximation, for \(x\) an integral multiple of 0.2. Throughout, primes denote derivatives with respect to \(x\). $$ x y^{\prime}=3 x-2 y, y(2)=3 ; 2 \leqq x \leqq 3 $$

(a) Show that if a projectile is launched straight upward from the surface of the earth with initial velocity \(v_{0}\) less than escape velocity \(\sqrt{2 G M / R}\), then the maximum distance from the center of the earth attained by the projectile is $$ r_{\max }=\frac{2 G M R}{2 G M-R v_{0}^{2}} $$ where \(M\) and \(R\) are the mass and radius of the earth, respectively. (b) With what initial velocity \(v_{0}\) must such a projectile be launched to yield a maximum altitude of 100 kilometers above the surface of the earth? (c) Find the maximum distance from the center of the earth, expressed in terms of earth radii, attained by a projectile launched from the surface of the earth with \(90 \%\) of escape velocity.

Separate variables and use partial fractions to solve the initial value problems in Problems \(1-8 .\) Use either the exact solution or a computer- generated slope field to sketch the graphs of several solutions of the given differential equation, and highlight the indicated particular solution. $$ \frac{d x}{d t}=7 x(x-13), x(0)=17 $$

A hand-held calculator will suffice for Problems 1 through 10, where an initial value problem and its exact solution are given. Apply the improved Euler method to approximate this solution on the interval \([0,0.5]\) with step size \(h=0.1 .\) Construct a table showing four-decimal-place values of the approximate solution and actual solution at the points \(x=0.1,0.2,0.3\), \(0.4,0.5\) $$ y^{\prime}=x-y, y(0)=1 ; y(x)=2 e^{-x}+x-1 $$

Consider a population \(P(t)\) satisfying the extinctionexplosion equation \(d P / d t=a P^{2}-b P\), where \(B=a P^{2}\) is the time rate at which births occur and \(D=b P\) is the rate at which deaths occur. If the initial population is \(P(0)=P_{0}\) and \(B_{0}\) births per month and \(D_{0}\) deaths per month are occurring at time \(t=0\), show that the threshold population is \(M=D_{0} P_{0} / B_{0}\).

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