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Identify each of the differential equations as to type (for example, separable, linear first order, linear second order, etc.), and then solve it. \((2 x-y \sin 2 x) d x+\left(2 y-\sin ^{2} x\right) d y=0\)

Short Answer

Expert verified
The equation is exact. The solution is given by \[x^2 + y \cos 2x + y^2 = C.\]

Step by step solution

01

Identify the Type of Differential Equation

Rewrite the given differential equation as \[(2 x - y \sin 2 x) \, dx + (2 y - \sin^2 x) \, dy = 0.\]To classify the type, compare it to standard forms. Here, it doesn't fit separable, linear first-order, or linear second-order forms. Notice it's approach to a potential exact differential equation.
02

Check Exactness

To check for an exact differential equation, we need\[M(x, y) = 2x - y \sin 2x\]and\[N(x, y) = 2y - \sin^2 x.\]Calculate partial derivatives \[\frac{\partial M}{\partial y} = -\sin 2x\]and\[\frac{\partial N}{\partial x} = -2 \sin x \cos x = -\sin 2x.\]Since \frac{\partial M}{\partial y} = \frac{\partial N}{\partial x}, the equation is exact.
03

Solve the Exact Differential Equation

Find the function \Psi(x, y) such that \frac{\partial \Psi}{\partial x} = M and \frac{\partial \Psi}{\partial y} = N. Integrate \frac{\partial \Psi}{\partial x} w.r.t x,\[\Psi(x, y) = \int (2x - y \sin 2x) \, dx\]\[\Psi(x, y) = x^2 + y \cos 2x + g(y)\]Compute \frac{\partial \Psi}{\partial y}:\[\Psi_y = \cos 2x + \frac{d g(y)}{d y} = 2y - \sin^2 x.\]So \frac{d g(y)}{d y} = 2y. Integrate w.r.t y,\[g(y) = y^2 + C.\]
04

Form the General Solution

Combine everything to \[\Psi(x, y) = x^2 + y \cos 2x + y^2 = C.\]This is the implicit solution.

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Key Concepts

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

differential equations
Differential equations are equations that involve an unknown function and its derivatives. They can model many physical systems and processes, such as motion, heat, or waves. There are different types of differential equations:
  • Separable: Can be rewritten as a product of two functions, each depending on a single variable.
  • Linear First Order: In the form \(a(x) y' + b(x) y = c(x)\).
  • Linear Second Order: In the form \(a(x) y'' + b(x) y' + c(x) y = d(x)\).
This particular problem involves identifying the type first, and determining if it fits an exact differential equation by checking if the exactness condition holds.
exactness condition
The exactness condition is essential for identifying exact differential equations. If a differential equation is in the form
\[ M(x, y) \, dx + N(x, y) \, dy = 0, \]
it is exact if the mixed partial derivatives of \(M\) and \(N\) are equal. Specifically, this means:
\[ \frac{\partial M}{\partial y} = \frac{\partial N}{\partial x}. \]
In our exercise:
\( M(x, y) = 2x - y \sin 2x \)
\( N(x, y) = 2y - \sin^2 x \)
we compute:
\( \frac{\partial M}{\partial y} = -\sin 2x \)
\( \frac{\partial N}{\partial x} = -2 \sin x \cos x = -\sin 2x \)
The derivatives are equal, confirming the equation is exact.
partial derivatives
Partial derivatives are derivatives of functions with more than one variable. They measure how the function changes as each variable changes while the others are held constant. For a function \(f(x, y)\):
  • \( \frac{\partial f}{\partial x} \): Keeps \(y\) constant and differentiates with respect to \(x\).
  • \( \frac{\partial f}{\partial y} \): Keeps \(x\) constant and differentiates with respect to \(y\).
In our problem, we used partial derivatives to check the exactness condition:
\( \frac{\partial M}{\partial y} = -\sin 2x \)
\( \frac{\partial N}{\partial x} = -\sin 2x \)
Both matched, allowing us to confirm the exactness of the equation.
integration
Integration is the process of finding the integral of a function, which is the reverse operation of differentiation. In the context of exact differential equations, solving involves finding a potential function \(\Psi(x, y)\) such that:
\(\frac{\partial \Psi}{\partial x} = M \)
\(\frac{\partial \Psi}{\partial y} = N \)
In our solution:
\(\frac{\partial \Psi}{\partial x} = 2x - y \sin 2x \)
Integrating w.r.t \(x\):
\(\Psi(x, y) = \int (2x - y \sin 2x) \, dx = x^2 + y \cos 2x + g(y) \)
Next, matching \(\frac{d g(y)}{\partial y}\) with \(N\):
\(\Psi_y = \cos 2x + \frac{d g(y)}{d y} = 2y - \sin^2 x \)
We solve for \(g(y)\):
\(\frac{d g(y)}{d y} = 2y \Rightarrow g(y) = y^2 \)
Thus the general solution is:
\(\Psi(x, y) = x^2 + y \cos 2x + y^2 = C \).

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Most popular questions from this chapter

Solve the following differential equations. \(y^{\prime}+\frac{1}{x} y=2 x^{3 / 2} y^{1 / 2}\)

Solve the following differential equations. \(y^{\prime \prime}-2 y^{\prime}=0\)

(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 \(T\).

Find a particular solution satisfying the given conditions. \(x y^{\prime}-y=x^{2}, \quad y=6\) when \(x=2\)

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. \(x y=k\).

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