Identify each of the differential equations as type (for example, separable, linear first order, linear second order, etc.), and then solve it. $$\left(x \cos y-e^{-\sin y}\right) d y+d x=0$$

Short Answer

Expert verified
Integrate to: (dy/dx) adjusting constants deriving trigonometric solution to match simpler form.

Step by step solution

01

Identify the type of differential equation

Rewrite the given differential equation in the form \(M(x,y)dx + N(x,y)dy = 0\), where\(M(x,y) = 1\) and \(N(x,y) = x \, \text{cos} \, y - e^{-\sin y}\).Notice that this equation has the potential of being an exact differential equation.
02

Check if the Differential Equation is Exact

To check if the differential equation is exact, we need to verify if the partial derivatives satisfy \( \frac{\partial M}{\partial y} = \frac{\partial N}{\partial x} \).Compute \( \frac{\partial M}{\partial y} = 0 \ \frac{\partial N}{\partial x} = \text{cos} \, y \).Since the equation \( \frac{\partial M}{\partial y} \) is not equal to \( \frac{\partial N}{\partial x} \), it is not an exact differential equation.
03

Transform the Equation to Solve

Use the standard approach of finding an integrating factor to transform it into an exact equation. The integrating factor depends on whether the equation depends on x or y only. Suppose it's a function of y: \( \mu(y) = e^{-\int P(y) dy} \), where \( P(y) = \frac{\partial M}{\partial y} - \frac{\partial N}{\partial x} \).However, since X is the variable of integration, rearrange to solve for y: \( dx + \frac{x \, cos y - e^{- \sin y}}{1} dy = 0 \). Integrate with respect to x to isolate.
04

Solution to Differential Equation

The simplest way is rearranging and integrating with x on left in non-linear form. This flow achieves linear integrating factor of combining trigonometric to achieve fundamental solution: Integrate both sides respectively: \( dy = - \int \frac{1}{x \cos y} dx \) to edge fundamental form to further establish arbitrary integral function solution.

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Key Concepts

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

Partial Derivatives
To understand partial derivatives, we must first grasp what a derivative is. In simple terms, a derivative measures how a function changes as its input changes. When dealing with functions of multiple variables, we take partial derivatives. A partial derivative focuses on the change with respect to one variable, keeping the others constant.
Here's an example: For a function of two variables, say \( z = f(x,y) \), the partial derivatives are \( \frac{\text{∂}z}{\text{∂}x} \) and \( \frac{\text{∂}z}{\text{∂}y} \).
These derivatives show how \( z \) changes with \( x \) and \( y \) respectively.

Let's use the given differential equation: \( (x \text{cos} \, y - e^{-\text{sin} \, y}) dy + dx = 0 \). We rewrite this in standard form: \( M(x, y) dx + N(x, y) dy = 0 \). Here, \( M(x,y) = 1 \) and \( N(x, y) = x \text{cos} \, y - e^{-\text{sin} \, y} \).
To check for exactness, we compute the partial derivatives: \( \frac{\text{∂} M}{\text{∂} y} = 0 \) and \( \frac{\text{∂} N}{\text{∂} x} = \text{cos} \, y \). Since these are not equal, the equation isn't exact.
Understanding and calculating partial derivatives is essential in verifying whether a differential equation is exact or not.
Integrating Factor
When facing a non-exact differential equation, we can often use an integrating factor to transform it into an exact one. An integrating factor is typically a function of \( x \) or \( y \). Applying it multiplies both sides of the differential equation, potentially converting it into an exact equation.

Consider a function \( \text{μ}(y) \):\[ \text{μ}(y) = e^{\text{−∫ P(y) dy}} \]
Where \( P(y) \) represents terms derived from the partial derivatives of the original non-exact equation. In our example, the integrating factor will depend on \( y \), as shown in step 3: \( \text{μ}(y) = e^{\text{−∫ (cos \, y) dy}} \).
This approach ensures that once we apply the integrating factor, the new equation can be easily integrated, providing a clear path to the solution. Understanding the concept and application of an integrating factor helps simplify seemingly complex differential equations.
Non-Exact Differential Equations
Non-exact differential equations do not meet the criteria where \( \frac{\text{∂}M}{\text{∂}y} = \frac{\text{∂}N}{\text{∂}x} \). This means we can't immediately integrate them. However, with techniques such as using an integrating factor, they can be converted to an exact form.

The given differential equation \( (x \text{cos} \, y - e^{-\text{sin} \, y}) dy + dx = 0 \) was identified as non-exact due to the mismatch between \( \frac{\text{∂} M}{\text{∂} y} \) and \( \frac{\text{∂} N}{\text{∂} x} \). Thus, we must find an integrating factor.
The process may involve trial and error or insight into the structure of the equation. Once identified and applied, the differential equation transforms into exact form, making it easier to solve.
Understanding how to work with non-exact differential equations enhances problem-solving skills and mathematical intuition. This knowledge is particularly valuable for advanced studies in differential equations and their applications.

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Most popular questions from this chapter

(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 which 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 \(I=I_{0} e^{-\mu s} .\) 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 ft, 500 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 1, 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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The curvature of a curve in the \((x, y)\) plane is $$K=y^{\prime \prime}\left(1+y^{\prime 2}\right)^{-3 / 2}$$. With \(K=\) const., solve this differential equation to show that curves of constant curvature are circles (or straight lines).

Suppose that the rate at which you work on a hot day is inversely proportional to the excess temperature above \(75^{\circ} .\) One day the temperature is rising steadily, and you start studying at 2 p.m. You cover 20 pages the first hour and 10 pages the second hour. At what time was the temperature \(75^{\circ} ?\)

By using Laplace transforms, solve the following differential equations subject to the given initial conditions. $$y^{\prime \prime}+16 y=8 \cos 4 t, \quad y_{0}=0, y_{0}^{\prime}=8$$

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