Find the general solution of each of the following differential equations. \(y^{\prime}+y \tanh x=2 e^{x}\)

Short Answer

Expert verified
The general solution is \( y = 2e^x \tanh x + C \cdot \text{sech} x \).

Step by step solution

01

Identify the Form of the Differential Equation

The given differential equation is: \(y' + y \tanh x = 2 e^x\). This is a first-order linear differential equation in the form \(y' + P(x)y = Q(x)\), where \(P(x) = \tanh x\) and \(Q(x) = 2 e^x\).
02

Determine the Integrating Factor

The integrating factor \(\mu(x)\) is given by \(e^{\int P(x) \, dx}\). Here, \(P(x) = \tanh x\), so we compute:\[ \mu(x) = e^{\int \tanh x \, dx} \]Since \(\int \tanh x \, dx = \ln |\cosh x|\), we have:\[ \mu(x) = e^{\ln |\cosh x|} = \cosh x \]
03

Multiply the Differential Equation by the Integrating Factor

Multiply both sides of the given differential equation by the integrating factor \(\cosh x\):\[ \cosh x \cdot y' + \cosh x \cdot y \tanh x = 2 e^x \cdot \cosh x \]Since \(\cosh x \cdot \tanh x = \sinh x\), the equation simplifies to:\[ \cosh x \cdot y' + \sinh x \cdot y = 2 e^x \cosh x \]
04

Rewrite the Left Side as a Derivative

The left side of the equation can be written as the derivative of the product of \(y\) and the integrating factor \(\cosh x\):\[ \frac{d}{dx}(y \cosh x) = 2 e^x \cosh x \]
05

Integrate Both Sides

Integrate both sides with respect to \(x\):\[ \int \frac{d}{dx}(y \cosh x) \, dx = \int 2 e^x \cosh x \, dx \]The left side simplifies to \(y \cosh x\):\[ y \cosh x = \int 2 e^x \cosh x \, dx \]
06

Solve the Integral on the Right Side

To solve the integral on the right side, notice that:\(\int 2 e^x \cosh x \, dx\) can be solved by using integration by parts or recognizing it as a standard integral. We get:\[ \int 2 e^x \cosh x \, dx = 2 e^x \sinh x\]Thus,\[ y \cosh x = 2 e^x \sinh x + C \]
07

Solve for \(y\)

Finally, solve for \(y\) by dividing both sides by \( \cosh x \):\[ y = \frac{2 e^x \sinh x + C}{\cosh x} \]This can be simplified noting that \(\frac{\sinh x}{\cosh x} = \tanh x\):\[ y = 2 e^x \tanh x + C \cdot \text{sech}x \]

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Key Concepts

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

Integrating Factor
First-order linear differential equations can often be solved using an integrating factor. The integrating factor is a function that, when multiplied by the original differential equation, transforms it into an equation that is easier to solve. For a differential equation of the form \(y' + P(x)y = Q(x)\), the integrating factor \(\mu(x)\) is given by:

\[ \mu(x) = e^{\int P(x) \, dx} \]

In the specific exercise we are considering, \(P(x) = \tanh x\). The integral of \(\tanh x\) is \(\ln |\cosh x|\), so the integrating factor \(\mu(x)\) is \(e^{\ln |\cosh x|} = \cosh x\). Multiplying through by this integrating factor allows us to rewrite the differential equation in a way that simplifies the process of finding its solution.
Hyperbolic Functions
Understanding hyperbolic functions is essential for solving some differential equations. Hyperbolic functions, similar to trigonometric functions, have essential properties and are defined as follows:
  • \( \sinh x = \frac{e^x - e^{-x}}{2} \)
  • \( \cosh x = \frac{e^x + e^{-x}}{2} \)
  • \( \tanh x = \frac{\sinh x}{\cosh x} \)
  • \( \sech x = \frac{1}{\cosh x} \)
  • \( \csch x = \frac{1}{\sinh x} \)
  • \( \coth x = \frac{1}{\tanh x} \)


In our equation, the term \( \tanh x \) on the left-hand side and terms \( \cosh x \), \( \sinh x \) on both sides are hyperbolic functions. Simplifying hyperbolic expressions is crucial to reaching the general solution.
General Solution of Differential Equations
Finding the general solution to a differential equation involves several steps, with the aim of expressing the dependent variable, typically \(y\), explicitly in terms of the independent variable, typically \(x\), plus an arbitrary constant (reflecting the general nature of the solution).

For the differential equation \(y' + y \tanh x = 2 e^x\) discussed in the exercise, we first identify the integrating factor and proceed through several transformations, utilizing hyperbolic functions and integrating both sides accordingly. The simplified version of the final general solution is:

\[ y = 2 e^x \tanh x + C \cdot \sech x \]

Here, \(C\) represents the integration constant, and it is crucial in describing the family of solutions for the differential equation. Each specific value of \(C\) corresponds to a specific solution path for the given differential equation.

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Most popular questions from this chapter

Find the general solution of each of the following differential equations. \(d x+\left(x-e^{y}\right) d y=0\)

Solve the following differential equations. \(y^{\prime \prime}+9 y=0\)

(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 \(T\).

Show that the thickness of the ice on a lake increases with the square root of the time in cold weather, making the following simplifying assumptions. Let the water temperature be a constant \(10^{\circ} \mathrm{C}\), the air temperature a constant \(-10^{\circ} \mathrm{C}_{7}\) and assume that at any given time the ice forms a slab of uniform thickness \(x\). The rate of formation of ice is proportional to the rate at which heat is transferred from the water to the air. Let \(t=0\) when \(x=0\).

Consider an equation for damped forced vibrations (mechanical or electrical) in which the right-hand side is a sum of several forces or emfs of different frequencies. For example, in (6.32) let the right-hand side be $$ F_{1} e^{i \omega_{1}^{\prime} t}+F_{2} e^{\operatorname{ior}_{2} l}+F_{3} e^{i \operatorname{cog} T} $$ Write the solution by the principle of superposition. Suppose, for given \(\omega_{1}^{\prime}, \omega_{2}^{\prime}, \omega_{3}^{\prime}\), that we adjust the system so that \(\omega=\omega_{1}^{\prime}\); show that the principal term in the solution is then the first one. Thus the system acts as a "filter" to select vibrations of one frequency from a given set (for example, a radio tuned to one station selects principally the vibrations of the frequency of that station).

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