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$$ \frac{d y}{d x}-\frac{y}{x(x+1)}=1 $$

Short Answer

Expert verified
The solution is \( y = x - \frac{x}{x+1} + \frac{x}{x+1}\ln|x| + \frac{Cx}{x+1} \).

Step by step solution

01

Identify the Type of Differential Equation

The given differential equation is \( \frac{dy}{dx} - \frac{y}{x(x+1)} = 1 \). This is a linear first-order differential equation since it can be written in the standard form \( \frac{dy}{dx} + P(x)y = Q(x) \). Here, \( P(x) = -\frac{1}{x(x+1)} \) and \( Q(x) = 1 \).
02

Find the Integrating Factor

The integrating factor, \( \mu(x) \), is computed using the formula \( \mu(x) = e^{\int P(x) \, dx} \). We have \( P(x) = -\frac{1}{x(x+1)} \). To find \( \mu(x) \), first find the antiderivative: \[ \int -\frac{1}{x(x+1)} \, dx = \int \left( \frac{1}{x+1} - \frac{1}{x} \right) \, dx = \ln|x+1| - \ln|x| \],this simplifies to \( \ln\left|\frac{x+1}{x}\right| \), hence the integrating factor is \( \mu(x) = \frac{x+1}{x} \).
03

Multiply Through by the Integrating Factor

Multiply the entire differential equation by the integrating factor:\[ \frac{x+1}{x} \left( \frac{dy}{dx} - \frac{y}{x(x+1)} \right) = \frac{x+1}{x} \cdot 1 \].This becomes:\[ \frac{x+1}{x} \frac{dy}{dx} - \frac{y}{x^2} = \frac{x+1}{x}. \]
04

Express as a Derivative

Recognize that the left side of the equation is now the derivative of a product of the integrating factor and \( y \):\( \frac{d}{dx} \left( \frac{x+1}{x} y \right) = \frac{x+1}{x} \).
05

Integrate Both Sides

Integrate both sides with respect to \( x \):\[ \int \frac{d}{dx} \left( \frac{x+1}{x} y \right) \, dx = \int \frac{x+1}{x} \, dx. \]The left side simplifies to \( \frac{x+1}{x} y \). The right side evaluates as:\[ \int \frac{x+1}{x} \, dx = \int 1 \, dx + \int \frac{1}{x} \, dx = x + \ln|x| + C, \]where \( C \) is the constant of integration.
06

Solve for y

Solve for \( y \) by dividing both sides by \( \frac{x+1}{x} \):\[ y = \frac{x}{x+1} (x + \ln|x| + C). \]
07

Simplify the Expression

Finally, distribute to obtain the solution:\[ y = x - \frac{x}{x+1} + \frac{x}{x+1}\ln|x| + \frac{Cx}{x+1}. \]

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Key Concepts

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

Integrating Factor
In solving linear first-order differential equations, one of the most crucial steps is finding and using an integrating factor. An integrating factor is a mathematical function that is used to simplify differential equations, specifically making them easier to solve.

How do we find the integrating factor? For a differential equation in the form \( \frac{dy}{dx} + P(x)y = Q(x) \), the integrating factor \( \mu(x) \) is determined by:\[ \mu(x) = e^{\int P(x) \, dx} \].

The integrating factor itself creates a kind of "balance," allowing us to transform the differential equation into a form that can be directly integrated. This is critical because it turns a potentially complex equation into something manageable and straightforward.

In our exercise, the integrating factor \( \mu(x) \) was derived from \( P(x) = -\frac{1}{x(x+1)} \), resulting in \( \mu(x) = \frac{x+1}{x} \). By multiplying the entire differential equation by this integrating factor, we effectively "line up" the terms that allow the differential equation to become a derivative of the product \( \frac{x+1}{x} y \).

This concept highlights the transformative power of the integrating factor, essentially replacing a more difficult operation (solving a complex differential equation) with simpler integration.
Linear First-Order Differential Equation
A linear first-order differential equation is one of the simplest types of differential equations often encountered in calculus. These equations take the form \( \frac{dy}{dx} + P(x)y = Q(x) \), where \( P(x) \) and \( Q(x) \) are functions of \( x \).

The hallmarks of this type of equation are that it is linear with respect to \( y \) and its derivative \( \frac{dy}{dx} \). This means that there are no products or powers of \( y \) other than the first power, making it "first-order" and linear.

Understanding how to identify and handle these equations is crucial as they serve as foundational blocks in more complex mathematical models. When dealing with linear first-order differential equations, we commonly use techniques such as direct integration or an integrating factor to solve them.

In our specific exercise, we rearranged the original equation \( \frac{dy}{dx} - \frac{y}{x(x+1)} = 1 \) to fit this standard form by identifying \( P(x) = -\frac{1}{x(x+1)} \) and \( Q(x) = 1 \). This identification paved the way for finding an integrating factor and simplifying the solution process.
Antiderivative
The antiderivative, or the indefinite integral, plays an essential role in solving many differential equations. An antiderivative of a function \( f(x) \) is another function \( F(x) \) such that \( F'(x) = f(x) \).

In the context of our differential equation, finding the antiderivative is a crucial step when solving for the integrating factor. To determine the integrating factor, we needed \( \int P(x) \, dx \). In our example, we calculated the antiderivative of \( P(x) = -\frac{1}{x(x+1)} \). By decomposing this fraction using partial fraction decomposition, we found that:
  • \( \int -\frac{1}{x(x+1)} \, dx = \int \left( \frac{1}{x+1} - \frac{1}{x} \right) \, dx \)
  • This integrates to \( \ln|x+1| - \ln|x| \), or \( \ln\left| \frac{x+1}{x} \right| \).
This operation allowed us to replace a seemingly complex integration problem with a straightforward logarithmic solution, fitting perfectly into the framework of using an integrating factor.

Thus, understanding how to compute antiderivatives is an indispensable skill when solving differential equations, as they often appear in the formulation and simplification of solutions.

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Most popular questions from this chapter

A cell constantly gains or loses small molecules to its environment because the small molecules are able to diffuse through the cell membrane. We will build a model for this process. Suppose a molecule is present in the cell at a concentration \(C(t)\), and present in its environment at a concentration \(C_{\infty}\) (you may assume \(C_{\infty}\) is a constant). One model for the diffusion of molecules across the cell membrane is that the rate at which molecules travel through the membrane is proportional to the difference in concentration between the cell and its surroundings. That is: Rate at which $$ \text { molecules flow out }=k\left(C-C_{\infty}\right) $$ of cell The constant \(k\) is known as the permeability of the membrane: \(k>0\), and \(k\) depends on the surface area of the cell and the chemistry of the membrane, as well as the type of molecule. (a) Starting with a word equation for the amount of small molecules in the cell, show, if the cell volume is \(V\), then: $$ \frac{d C}{d t}=-\frac{k}{V}\left(C-C_{\infty}\right) $$ (b) Find the equilibrium of \((8.53)\) and use a graphical analysis to determine whether it is stable or unstable. (c) Suppose that the molecule we are studying is produced within the cell. The cell produces the molecule at a rate \(r\); that is, a quantity \(r\) is produced (added to the cell) in unit time. Explain why the differential equation for the concentration of molecules in the cell should be modified to: $$ \frac{d C}{d t}=-\frac{k}{V}\left(C-C_{\infty}\right)+\frac{r}{V} $$ (d) Analyze Equation (8.54) to find the equilibrium value of the cell concentration. Is this equilibrium stable or unstable? You may use a graphical argument or calculate the eigenvalue to determine the equilibrium's stability.

In our compartment model we assumed that inflows and outflows are matched at \(q\) to keep the volume of water in the tank constant. It's often useful when modeling, for example, the flow of pollutant into a pristine environment, to consider what can occur if the inflows and outflows do not match. Let's assume that the tank initially contains a volume \(V_{0}\) of water. Water flows into the tank at rate \(q_{\mathrm{in}}\), and out of the tank at rate \(q_{\text {out. }}\) (You may assume \(q_{\text {in }}>q_{\text {out } .}\) ) Suppose that the water flowing into the tank contains a concentration \(C_{I}\) of solute. As usual we write \(C(t)\) for the concentration in the tank. (a) Show that the concentration in the tank can be modeled using a differential equation: $$ \frac{d}{d t}(C V)=q_{\text {in }} C_{I}-q_{\text {out }} C $$ (b) Previously we were able to treat \(V\) as a constant. Now \(V\) changes with time. Derive a formula for \(V(t)\). (c) By substituting your formula for \(V(t)\) into (a), derive a differential equation for \(C(t)\). (d) In general we cannot analyze the behavior of the solution \(C(t)\) using techniques from Section \(8.2 .\) Why not? (e) Let's assume \(C_{l}=0\). Then show that your equation from (c) can be written as: $$ \frac{d C}{d t}=\frac{-q_{\mathrm{in}} C}{V_{0}+\left(q_{\mathrm{in}}-q_{\mathrm{out}}\right) t} $$ (f) Assume some definite values for the constants in \((8.57):\) \(q_{\mathrm{in}}=2, q_{\text {out }}=1\), and \(V_{0}=20 .\) Assuming \(C(0)=1\), solve \((8.57)\) to find \(C(t) .\) Show that \(\lim _{t \rightarrow \infty} C(t)=0\).

Find the equilibria of the following differential equations. $$ \frac{d y}{d t}=y\left(y^{2}-1\right) $$

Find all equilibria, and, by calculating the eigenvalue of the differential equation, determine which equilibria are stable and which are unstable. $$ \frac{d N}{d t}=N \ln \left(\frac{2}{N}\right) \quad N>0 $$

Determine whether the equilibrium at \(x=0\) is stable, unstable, or semi- stable. $$ \frac{d x}{d t}=x^{3}+x^{4} $$

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