/*! 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 14 Find the general solution of eac... [FREE SOLUTION] | 91Ó°ÊÓ

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Find the general solution of each of the following differential equations. \(\frac{d y}{d x}=\frac{3 y}{3 y^{2 / 3}-x}\)

Short Answer

Expert verified
\frac{3}{5} y^{5/3} - \frac{1}{2} y^2 = 3x + C

Step by step solution

01

Identify the form of the differential equation

The given differential equation is \(\frac{d y}{d x}=\frac{3 y}{3 y^{2 / 3}-x}\). It can be identified as a separable differential equation.
02

Rewrite the equation to separate variables

To separate the variables, rewrite the equation: \(\frac{dy}{dx} = \frac{3y}{3y^{2/3} - x}\). Multiply both sides by \(3y^{2/3} - x\) and \(dx\) to get \( (3y^{2/3} - x) dy = 3y dx \).
03

Simplify and further separate the variables

Rearrange terms to isolate all terms involving \(y\) on one side and all terms involving \(x\) on the other. \((3y^{2/3} - x) dy = 3y dx \). Simplify to \((3y^{2/3} dy - y dy) = 3 dx \).
04

Integrate both sides

Integrate both sides to solve for \(y\). For the left-hand side, the integral becomes \(\frac{3}{5} y^{5/3} - \frac{1}{2} y^2\). For the right-hand side, the integral is \(3x + C\). Combining these, we get \(\frac{3}{5} y^{5/3} - \frac{1}{2} y^2 = 3x + C \).
05

Simplify the general solution

Combine and simplify the constants to write the general solution. The final form of the general solution will be \(\frac{3}{5} y^{5/3} - \frac{1}{2} y^2 = 3x + C \).

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Key Concepts

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

differential equations
A differential equation is an equation that involves unknown functions and their derivatives. These equations play a crucial role in various fields like physics, engineering, and economics.
By finding solutions to these equations, we can predict how systems change over time. There are different types of differential equations, but one of the simplest forms is a first-order differential equation.
In this exercise, we are dealing with a first-order differential equation represented as \(\frac{dy}{dx} = \frac{3y}{3y^{2/3} - x}\).
Our goal is to find the general solution, which helps us understand how the dependent variable, y, changes concerning the independent variable, x.
integration
Integration is a fundamental concept in calculus that can be thought of as the reverse process of differentiation. In the context of differential equations, integration is used to solve equations involving derivatives.
When we integrate, we effectively find the original function given its derivative. For example, if we have \(dy = f(x)dx\), integrating both sides with respect to x will give us the original function y in terms of x.
In our exercise, after separating the variables, we perform integration on both sides of the equation. Specifically, we integrate \(3y^{2/3} - y\) with respect to y and 3 with respect to x. The integration results help us combine the terms to form the general solution.
variables separation
Separation of variables is a method for solving first-order differential equations. The idea is to rearrange the equation so that all terms involving the dependent variable (y) are on one side, and all terms involving the independent variable (x) are on the other.
For our differential equation \(\frac{dy}{dx} = \frac{3y}{3y^{2/3} - x}\), we multiply both sides by \(3y^{2/3} - x\) and \(dx\) to separate the variables. This step yields \( (3y^{2/3} - x) dy = 3y dx\).
Next, we isolate the terms to get \(3y^{2/3} dy - y dy = 3 dx\). This format allows us to integrate both sides easily.
general solution
The general solution to a differential equation is a family of functions that includes an arbitrary constant, usually denoted as C. This constant represents an infinite number of possible solutions, each corresponding to a different initial condition.
After performing the necessary integrations, we get a combined solution involving the constant C. In our exercise, after integrating both sides, we obtain \( \frac{3}{5} y^{5/3} - \frac{1}{2} y^2 = 3x + C \). This is the general solution to our differential equation.
This form provides a complete description of all possible solutions and how y changes concerning x for various initial conditions.

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Most popular questions from this chapter

Solve the following differential equations. \(y^{\prime \prime}-4 y^{\prime}+4 y=0\)

Find the orthogonal trajectories of each of the following families of curves. In each case sketch several of the given curves and several of their orthogonal trajectories. Be careful to eliminate the constant from \(d y / d x\) for the original curves; this constant takes different values for different curves of the original family and you want an expression for \(d y / d x\) which is valid for all curves of the family crossed by the orthogonal trajectory you are trying to find. \(y=k x^{2}\)

Consider an equation for damped forced vibrations (mechanical or electrical) in which the right-hand side is a sum of several forces or emfs of different frequencies. For example, in (6.32) let the right-hand side be $$ F_{1} e^{i \omega_{1}^{\prime} t}+F_{2} e^{\operatorname{ior}_{2} l}+F_{3} e^{i \operatorname{cog} T} $$ Write the solution by the principle of superposition. Suppose, for given \(\omega_{1}^{\prime}, \omega_{2}^{\prime}, \omega_{3}^{\prime}\), that we adjust the system so that \(\omega=\omega_{1}^{\prime}\); show that the principal term in the solution is then the first one. Thus the system acts as a "filter" to select vibrations of one frequency from a given set (for example, a radio tuned to one station selects principally the vibrations of the frequency of that station).

Find the "general solution" (that is, a solution containing an arbitrary constant) of each of the following differential equations, by separation of variables. Then find a particular solution of each equation satisfying the given boundary conditions. \(y^{\prime}=\frac{2 x y^{2}+x}{x^{2} y-y}\) \(y=0\) when \(x=\sqrt{2}\)

(a) Consider a light beam traveling downward into the ocean. As the beam progresses, it is partially absorbed and its intensity decreases. The rate at whieh the intensity is decreasing with depth at any point is proportional to the intensity at that depth. The proportionality constant \(\mu\) is called the linear absorption coefficient. Show that if the intensity at the surface is \(I_{0}\), the intensity at a distance \(s\) below the surface is \(l=\) \(I_{0} e^{-\mu s} .\) The linear absorption coefficient for water is of the order of \(10^{-2} \mathrm{ft}^{-1}\) (the exact value depending on the wavelength of the light and the impurities in the water). For this value of \(\mu\), find the intensity as a fraction of the surface intensity at a depth of \(1 \mathrm{ft}, 50 \mathrm{ft}, 500 \mathrm{ft}, 1\) mile. When the intensity of a light beam has been reduced to half. its surface intensity \(\left(I=\frac{1}{2} I_{0}\right)\), the distance the light has penetrated into the absorbing substance is called the half-value thickness of the substance. Find the half-value thickness in terms of \(\mu\). Find the half-value thickness for water for the value of \(\mu\) given above. (b) Note that the differential equation and its solution in this problem are mathematically the same as those in Example I, although the physical problem and the terminology are different. In discussing radioactive decay, we call \(\lambda\) the decay constant, and we define the half-life \(T\) of a radioactive substance as the time when \(N=\frac{1}{2} N_{0}\) (compare half-value thickness). Find the relation between \(\lambda\) and \(T\).

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