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Find general solutions (implicit if necessary, explicit if convenient) of the differential equations in Problems 1 through \(18 .\) Primes denote derivatives with respect to \(x.\) $$ y^{\prime}=1+x+y+x y $$

Short Answer

Expert verified
The solution is \( y = \frac{I(x) + C}{e^{x + \frac{x^2}{2}}} \), where \( I(x) \) is an integral without a simple closed form.

Step by step solution

01

Identify the type of differential equation

The given equation is \( y' = 1 + x + y + xy \). Recognize that this is a first-order differential equation because it involves the first derivative of \( y \). Moreover, observe that the equation can be rewritten as \( y' = (1 + x) + (1 + x)y \), hence it's a first-order linear differential equation in standard form \( y' = P(x)y + Q(x) \) with \( P(x) = 1 + x \) and \( Q(x) = 1 + x \).
02

Calculate the integrating factor

To solve a first-order linear differential equation, we need to find an integrating factor, \( \mu(x) \), which is defined as \( e^{\int P(x) \, dx} \). Compute the integral of \( P(x) = 1 + x \): \[ \int (1 + x) \, dx = x + \frac{x^2}{2} \]. The integrating factor is then \( \mu(x) = e^{x + \frac{x^2}{2}} \).
03

Solve the differential equation using the integrating factor

Multiply the original differential equation by the integrating factor: \( e^{x + \frac{x^2}{2}} y' = e^{x + \frac{x^2}{2}} (1 + x + y + xy) \). This simplifies to \( \frac{d}{dx} (e^{x + \frac{x^2}{2}} y) = e^{x + \frac{x^2}{2}} (1 + x) \).
04

Integrate both sides

Integrate both sides concerning \( x \): \( \int \frac{d}{dx}(e^{x + \frac{x^2}{2}} y) \, dx = \int e^{x + \frac{x^2}{2}} (1 + x) \, dx \). The left side integrates to \( e^{x + \frac{x^2}{2}} y \). For the right side, let's denote \( I = \int e^{x + \frac{x^2}{2}} (1 + x) \, dx \).
05

Evaluate the integral on the right

Although the integral \( \int e^{x + \frac{x^2}{2}} (1 + x) \, dx \) does not have a simple closed form, we express the solution in terms of an implicit function: \( e^{x + \frac{x^2}{2}} y = I + C \), where \( C \) is the constant of integration. Here, \( I \) represents the antiderivative of \( e^{x + \frac{x^2}{2}} (1 + x) \), which can be computed symbolically or numerically as needed.
06

Express the solution explicitly if possible

The explicit solution for \( y \) is given implicitly by \( y = \frac{I(x) + C}{e^{x + \frac{x^2}{2}}} \). In many cases, especially when \( I(x) \) does not simplify further nicely, it is acceptable to leave the solution in this implicit form.

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Key Concepts

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

First-order linear differential equation
A first-order linear differential equation is a type of equation that involves the first derivative of an unknown function, which we usually denote as \( y' \). In this case, the equation has the standard form:
  • \( y' = P(x)y + Q(x) \)
Here, \( P(x) \) and \( Q(x) \) are functions of \( x \) alone, or constants. In our specific example, the differential equation is given as:
  • \( y' = 1 + x + y + xy \)
When analyzed, this equation can be rearranged to fit the standard form:
  • \( y' = (1 + x)y + (1 + x) \)
When you see this form, know it is telling you there's a linear relationship between the derivative of \( y \) and the variables involved. We use techniques like finding an integrating factor to solve these equations.
Integrating factor
An integrating factor is a device we use to solve first-order linear differential equations. It simplifies the integration of such equations, allowing us to take an equation that's difficult to solve and transform it into an equation that's easier to handle.The most typical formula used for finding the integrating factor \( \mu(x) \) is:
  • \( \mu(x) = e^{\int P(x) \, dx} \)
In our solution, \( P(x) \) was identified as \( 1 + x \), leading to the integral:
  • \( \int (1 + x) \, dx = x + \frac{x^2}{2} \)
From this, we can find the integrating factor:
  • \( \mu(x) = e^{x + \frac{x^2}{2}} \)
Multiplying through the original equation by this integrating factor effectively allows us to convert the equation into an exact differential equation.
Implicit solution
An implicit solution of a differential equation is one where the dependent variable (usually \( y \)) is not isolated on one side of the equation. Instead, both \( y \) and \( x \) appear on both sides of the equation, making it implicit.In our step-by-step solution, after finding the integrating factor, we ended up with this form:
  • \( e^{x + \frac{x^2}{2}} y = I + C \)
Here, \( I \) is an expression for the integral of \( e^{x + \frac{x^2}{2}} (1 + x) \), which can't be expressed nicely in simple terms. Consequently, it remains implicit.This method of expressing the solution works well since it circumvents the need for exact expressions when they are infeasible to obtain. Plus, this format allows for numerical methods to approximate solutions as needed.
Explicit solution
In contrast to implicit solutions, an explicit solution is one where the dependent variable \( y \) is expressed solely in terms of the independent variable \( x \) and a constant \( C \).The explicit form is usually preferred when possible because it provides a clear, direct relationship between \( y \) and \( x \). For our problem, even though we started with a complex equation, the solution process led to:
  • \( y = \frac{I(x) + C}{e^{x + \frac{x^2}{2}}} \)
This is very close to an explicit solution. However, because \( I(x) \) itself doesn't have a simple form, it's common to maintain the solution in an implicit format.In fields requiring practical application (like engineering or physics), this form allows employing computational methods to compute precise values for \( y \) based on \( x \) and \( C \). This highlights the flexibility between seeking explicit and settling for implicit solutions depending on the context.

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Most popular questions from this chapter

Suppose a uniform flexible cable is suspended between two points \((\pm L, H)\) at equal heights located symmetrically on either side of the \(x\) -axis (Fig. 1.4.12). Principles of physics can be used to show that the shape \(y=y(x)\) of the hanging cable satisfies the differential equation $$a \frac{d^{2} y}{d x^{2}}=\sqrt{1+\left(\frac{d y}{d x}\right)^{2}}$$ where the constant \(a=T / \rho\) is the ratio of the cable's tension \(T\) at its lowest point \(x=0\) (where \(y^{\prime}(0)=0\) ) and its (constant) linear density \(\rho\). If we substitute \(v=d y / d x\), \(d v / d x=d^{2} y / d x^{2}\) in this second-order differential equation, we get the first-order equation $$ a \frac{d v}{d x}=\sqrt{1+v^{2}} $$ Solve this differential equation for \(y^{\prime}(x)=v(x)=\) \(\sinh (x / a)\). Then integrate to get the shape function $$y(x)=a \cosh \left(\frac{x}{a}\right)+C$$ of the hanging cable. This curve is called a catenary, from the Latin word for chain.

According to one cosmological theory, there were equal amounts of the two uranium isotopes \({ }^{235} \mathrm{U}\) and \({ }^{238} \mathrm{U}\) at the creation of the universe in the "big bang." At present there are \(137.7\) atoms of \({ }^{238} \mathrm{U}\) for each atom of \({ }^{235} \mathrm{U}\). Using the half-lives \(4.51 \times 10^{9}\) years for \({ }^{238} \mathrm{U}\) and \(7.10 \times 10^{8}\) years for \({ }^{235} \mathrm{U}\), calculate the age of the universe.

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