The initial value problem $$ \frac{d y}{d x}=\frac{y^{2}+x y}{x^{2}}, \quad y(1)=1 $$ does not fall into the class of problems considered in this chapter. However, if one substitutes \(y(x)=x z(x)\) into the differential equation, one obtains an equation for \(z(x)\) that can be solved. Use this substitution to solve the initial value problem for \(y(x)\).

Short Answer

Expert verified
The solution to the initial value problem is \(y(x) = \frac{x^2}{1 +x}\).

Step by step solution

01

Substitute Given Function

We start by substituting \(y(x) = xz(x)\) into the given differential equation. Taking derivative of both sides gives \(\frac{d y}{d x} = z(x) + x \frac{d z}{d x}\). We substitute these into the original differential equation, obtaining \(\frac{d y}{d x} = z(x) + x \frac{d z}{d x} = \frac{(x z(x))^2+ x (x z(x))}{x^2}\). Simplifying, we find \(z + x \frac{d z}{d x} = z^2 + z\).
02

Rearrange Equation

We now rearrange the differential equation to isolate the derivative on one side. This gives us \(\frac{d z}{d x} = z(z - 1)\).
03

Solve Separable Differential Equation

This equation is now separable, meaning we can rearrange it as a product of functions of z and x and then integrate. \( \frac{d z}{z(z - 1)} = \frac{d x}{x} \). Integrate both sides as \(\int \frac{d z}{z(z - 1)} = \int \frac{d x}{x}\) to get \( \ln|x| = - \ln|z - 1| + \ln|z|\). This simplifies to \( \ln|x| = \ln \left|\frac{z}{z-1}\right|\). Taking exponential of both sides, we get \(|x| = \left|\frac{z}{z-1}\right|\). Since we started with y(1) = 1, we know that z(1) = 1 and therefore, we can drop the absolute value on the right side but keep it on the left side.
04

Rearrange and Substitute Back for y

We rearrange the result to solve for z: \(z = \frac{x}{1 \pm x}\). Because the initial condition is y(1) = 1, we choose the upper sign, so \(z = \frac{x}{1 +x}\). Finally, remembering our substitution y(x) = xz(x), this gives us the solution for our original differential equation: \(y(x) = x \cdot \frac{x}{1 +x} = \frac{x^2}{1 +x}\).

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Most popular questions from this chapter

17\. A piece of a satellite falls to the ground from a height of \(10,000 \mathrm{~m}\). Ignoring air resistance, find the height as a function of time. [Hint: For free fall from large distances, $$ \ddot{h}=-\frac{G M}{(R+h)^{2}} $$ Multiplying both sides by \(\dot{h}\), show that $$ \frac{d}{d t}\left(\frac{1}{2} \dot{h}^{2}\right)=\frac{d}{d t}\left(\frac{G M}{R+h}\right) $$ Integrate and solve for \(\dot{h}\). Further integrating gives \(h(t) .]\)

Consider the nonhomogeneous differential equation \(x^{\prime \prime}-3 x^{\prime}+2 x=6 e^{3 t}\). a. Find the general solution of the homogenous equation. b. Find a particular solution using the Method of Undetermined Coefficients by guessing \(x_{p}(t)=A e^{3 t}\). c. Use your answers in the previous parts to write the general solution for this problem.

Consider the case of free fall with a damping force proportional to the velocity, \(f_{D}=\pm k v\) with \(k=0.1 \mathrm{~kg} / \mathrm{s}\). a. Using the correct sign, consider a \(50-\mathrm{kg}\) mass falling from rest at a height of \(100 \mathrm{~m}\). Find the velocity as a function of time. Does the mass reach terminal velocity? b. Let the mass be thrown upward from the ground with an initial speed of \(50 \mathrm{~m} / \mathrm{s}\). Find the velocity as a function of time as it travels upward and then falls to the ground. How high does the mass get? What is its speed when it returns to the ground?

In Example 2.32, \(a(t)\) was determined for a curved universe with nonrelativistic matter for \(\Omega_{0}>1\). Derive the parametric equations for \(\Omega_{0}<1\), $$ \begin{aligned} &a=\frac{\Omega_{0}}{2\left(1-\Omega_{0}\right)}(\cosh \eta-1) \\ &t=\frac{\Omega_{0}}{2 H_{0}\left(1-\Omega_{0}\right)^{3 / 2}}(\sinh \eta-\eta) \end{aligned} $$ for \(\eta \geq 0\)

Use the transformations relating polar and Cartesian coordinates to prove that $$ \frac{d \theta}{d t}=\frac{1}{r^{2}}\left[x \frac{d y}{d t}-y \frac{d x}{d t}\right] $$

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