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Solve the differential equation. $$ y^{\prime}+x e^{y}=0 $$

Short Answer

Expert verified
Solution is \( y = -\ln\left(\frac{2}{x^2 - 2C}\right) \).

Step by step solution

01

Rearrange the Differential Equation

The given differential equation is \( y^{\prime} + x e^{y} = 0 \). We can rewrite this equation in the form \( y^{\prime} = -x e^{y} \).
02

Separate Variables

Separate the variables by dividing both sides by \( e^{y} \) and multiplying by \( dx \). This yields: \[ e^{-y} dy = -x dx \]. This separation allows us to integrate both sides independently.
03

Integrate Both Sides

Now integrate both sides: - The integral of \( e^{-y} dy \) is \(-e^{-y} + C_1\) - The integral of \(-x dx\) is \(-\frac{x^2}{2} + C_2\). So we have: \[ -e^{-y} = -\frac{x^2}{2} + C \] where \( C = C_2 - C_1 \) and is a constant.
04

Solve for y

To express \( y \) explicitly, rearrange the equation:\[ e^{-y} = \frac{x^2}{2} - C \].Taking the natural logarithm on both sides after taking the reciprocal:\[ y = -\ln\left(\frac{2}{x^2 - 2C}\right) \]. We can rewrite this as the explicit solution if needed.

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Key Concepts

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

Separation of Variables
Separation of variables is a technique used to solve differential equations. It involves rearranging an equation to isolate all terms involving the variable y on one side and all terms involving the variable x on the other side. In our example, starting with the differential equation \( y^{\prime} + x e^{y} = 0 \), we first rearrange it to \( y^{\prime} = -x e^{y} \).

We can then manipulate it further so that each side of the equation contains a single variable. By dividing both sides by \( e^y \) and multiplying by \( dx \), we obtain \( e^{-y} dy = -x dx \). Now, the equation is perfectly set for integration, with variables separated, making this technique particularly useful for easily solvable problems.
Integration
Integration is the process of finding the integral of an equation, which is essentially the reverse of differentiation. It allows us to determine the function that results in a given derivative.

After separating variables, we have: \( \int e^{-y} dy \) on the left side and \( \int -x dx \) on the right side. Let's explore these integrations separately:
  • The integral of \( e^{-y} dy \) is \(-e^{-y} + C_1\), where \( C_1 \) is a constant of integration.
  • The integral of \(-x dx\) is \(-\frac{x^2}{2} + C_2\), where \( C_2 \) is another constant of integration.
Combining these results gives us \(-e^{-y} = -\frac{x^2}{2} + C\), where \( C = C_2 - C_1 \). Integration is a powerful tool that converts our derivative equation into a more familiar algebraic form.
Exponential Functions
Exponential functions involve the variable as an exponent, and they appear frequently in solving differential equations. In our equation, we deal with \( e^y \), which means our solution involves understanding and manipulating exponential terms.

This is evident in our integration, yielding \(- e^{-y} = -\frac{x^2}{2} + C \). To solve for \( y \), one must be comfortable with the properties of exponential functions:
  • Taking reciprocals: From \( e^{-y} \), one finds the reciprocal by rewriting it as \( \frac{1}{e^y} \).
  • Natural logarithms: Logarithms allow us to "undo" the exponentiation, which is crucial in solving for \( y \).
Understanding how exponential and logarithmic functions work is essential for manipulating and solving the solutions derived from differential equations.
Solving for y
After integrating and rewriting our equation, the next step is to solve explicitly for \( y \). We use algebraic manipulations and properties of logarithms to isolate \( y \). The rearranged equation from the integration is \( e^{-y} = \frac{x^2}{2} - C \).

By taking the reciprocal on both sides, we convert \( e^{-y} \) into \( e^y \), leading to the expression \( y = -\ln\left( \frac{2}{x^2 - 2C} \right) \). This involves using natural logarithms to solve the equation, which is a common practice when dealing with exponential solutions.

This final step transforms the originally given differential equation into a solution that directly expresses \( y \) as a function of \( x \) and the constant \( C \). Remember to check the domain restrictions placed by the expression within the logarithm, ensuring meaningful and valid solutions.

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Most popular questions from this chapter

Solve the initial-value problem. $$ x^{2} y^{\prime}+2 x y=\ln x, \quad y(1)=2 $$

In a seasonal-growth model, a periodic function of time is introduced to account for seasonal variations in the rate of growth. Such variations could, for example, be caused by seasonal changes in the availability of food. (a) Find the solution of the seasonal-growth model $$ \frac{d P}{d t}=k P \cos (r t-\phi) \quad P(0)=P_{0} $$ where \(k, r,\) and \(\phi\) are positive constants. (b) By graphing the solution for several values of \(k, r,\) and \(\phi,\) explain how the values of \(k, r,\) and \(\phi\) affect the solution. What can you say about \(\lim _{t \rightarrow \infty} P(t) ?\)

(a) Solve the differential equation \(y^{\prime}=2 x \sqrt{1-y^{2}}\) (b) Solve the initial-value problem \(y^{\prime}=2 x \sqrt{1-y^{2}}\) \(y(0)=0,\) and graph the solution. (c) Does the initial-value problem \(y^{\prime}=2 x \sqrt{1-y^{2}}\) \(y(0)=2\), have a solution? Explain.

To account for seasonal variation in the logistic differential equation, we could allow \(k\) and \(M\) to be functions of \(t:\) $$ \frac{d P}{d t}=k(t) P\left(1-\frac{P}{M(t)}\right) $$ (a) Verify that the substitution \(z=1 / P\) transforms this equation into the linear equation $$ \frac{d z}{d t}+k(t) z=\frac{k(t)}{M(t)} $$ (b) Write an expression for the solution of the linear equation in part (a) and use it to show that if the carrying capacity \(M\) is constant, then $$ P(t)=\frac{M}{1+C M e^{-j k(t) d t}} $$ Deduce that if \(\int_{0}^{\infty} k(t) d t=\infty,\) then \(\lim _{t \rightarrow \infty} P(t)=M .\) IThis will be true if \(k(t)=k_{0}+a \cos b t\) with \(k_{0}>0,\) which describes a positive intrinsic growth rate with a periodic seasonal variation. (c) If \(k\) is constant but \(M\) varies, show that $$ z(t)=e^{-k t} \int_{0}^{t} \frac{k e^{k s}}{M(s)} d s+C e^{-k t} $$ and use I' Hospital's Rule to deduce that if \(M(t)\) has a limit as \(t \rightarrow \infty\), then \(P(t)\) has the same limit.

The air in a room with volume \(180 \mathrm{m}^{3}\) contains \(0.15 \%\) carbon dioxide initially. Fresher air with only \(0.05 \%\) carbon dioxide flows into the room at a rate of \(2 \mathrm{m}^{3} / \mathrm{min}\) and the mixed air flows out at the same rate. Find the percentage of carbon dioxide in the room as a function of time. What happens in the long run?

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