Identify each of the differential equations as to type (for example, separable, linear first order, linear second order, etc.), and then solve it. \(y^{\prime \prime}+4 y^{\prime}+5 y=26 e^{3 x}\)

Short Answer

Expert verified
Linear second-order non-homogeneous; \[ y = e^{-2x}( C_1 \cos x + C_2 \sin x ) + e^{3x} \]

Step by step solution

01

Identify the Type of Differential Equation

Examine the provided differential equation: \[ y^{abla abla} + 4y^{abla} + 5y = 26e^{3x} \] This equation is a second-order linear non-homogeneous differential equation since it contains the second derivative of y, and the non-homogeneous term is 26e^{3x}.
02

Find the Complementary Function (C.F.)

Solve the corresponding homogeneous equation: \[ y^{abla abla} + 4y^{abla} + 5y = 0 \] Assume a solution of the form \( y = e^{rx} \). Plug this into the homogeneous equation to obtain the characteristic equation: \[ r^2 + 4r + 5 = 0 \] Solve for r using the quadratic formula: \[ r = \frac{-4 \pm \sqrt{16 - 20}}{2} = \frac{-4 \pm i \sqrt{4}}{2} = -2 \pm i \] Thus, the complementary function is: \[ y_c = e^{-2x}( C_1 \cos x + C_2 \sin x ) \]
03

Determine the Particular Solution (P.S.)

Assume a particular solution of the form: \[ y_p = Ae^{3x} \] Find the first and second derivatives: \[ y_p^{abla} = 3Ae^{3x} \] \[ y_p^{abla abla} = 9Ae^{3x} \] Substitute these into the non-homogeneous differential equation: \[ 9Ae^{3x} + 12Ae^{3x} + 5Ae^{3x} = 26e^{3x} \] Combine and solve for A: \[ 26Ae^{3x} = 26e^{3x} \] \[ A =1 \] Thus, the particular solution is: \[ y_p = e^{3x} \]
04

Form the General Solution

Combine the complementary function and the particular solution to obtain the general solution: \[ y = y_c + y_p \] Therefore, the general solution is: \[ y = e^{-2x}( C_1 \cos x + C_2 \sin x ) + e^{3x} \]

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Key Concepts

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

characteristic equation
To solve a second-order linear non-homogeneous differential equation, we start with the corresponding homogeneous equation.
We assume that the solution to this homogeneous equation has the form of an exponential function: \( y = e^{rx} \).
Substituting this assumption into the homogeneous differential equation converts it to a polynomial equation in terms of \(r\), known as the *characteristic equation*.
In this exercise, the homogeneous equation is:
y'' + 4y' + 5y = 0. Replacing \(y = e^{rx}\), the characteristic equation becomes:
\[ r^2 + 4r + 5 = 0 \]
This quadratic equation allows us to solve for the roots (\(r\)) using the quadratic formula. The solutions to this polynomial will help us construct the complementary function.
complementary function
The complementary function (C.F.) is the general solution to the homogeneous part of the differential equation.
The roots of the characteristic equation we found were complex:
\[ r = -2 \text{±} i \]
For complex roots of the form \(r = \text{α} \text{±}βi\), the complementary function is:
\[ y_c = e^{ \text{α} x} (C_1 \text{cos} (\text{β}x) + C_2 \text{sin}(\text{β}x)) \].
Substituting \( \text{α} = -2 \) and \( \text{β} = 1 \) into this form gives:

\[ y_c = e^{ -2x} (C_1 \text{cos}(x) + C_2 \text{sin}(x)) \]
Here, \(C_1\) and \(C_2\) are arbitrary constants that we can determine if initial conditions are provided.
particular solution
The particular solution (P.S.) is a specific solution that satisfies the non-homogeneous differential equation.
For this equation, we assume a particular solution based on the form of the non-homogeneous term \(26e^{3x}\).
Assume a solution of the form:
\( y_p = Ae^{3x} \).
To find \(A\), we differentiate:
\( y_p' = 3Ae^{3x} \) \( y_p'' = 9Ae^{3x} \)
Substitute these into the original non-homogeneous equation:
\( 9Ae^{3x} + 12Ae^{3x} + 5Ae^{3x} = 26e^{3x} \)
Combining coefficients, we get:
\( 26Ae^{3x} = 26e^{3x} \).
Thus, \(A = 1\), giving the particular solution:
\( y_p = e^{3x} \)
homogeneous differential equation
A homogeneous differential equation is one where all terms depend only on the function and its derivatives.
There is no term that is a standalone function of the independent variable. The equation is set to zero.
For our given problem, the homogeneous form is:
\( y'' + 4y' + 5y = 0 \).
This is derived by removing the non-homogeneous term \(26e^{3x}\). By solving this, we find the complementary function, which combined with the particular solution, forms the general solution.
The general solution of the given second-order linear non-homogeneous differential equation
is then given by:
\( y = y_c + y_p \)
where \( y_c = e^{-2x}(C_1 \text{cos}x + C_2 \text{sin}x) \) and \( y_p = e^{3x} \).

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Most popular questions from this chapter

Find the "general solution" (that is, a solution containing an arbitrary constant) of each of the following differential equations, by separation of variables. Then find a particular solution of each equation satisfying the given boundary conditions. \(\cos x \cos y d x-\sin x \sin y d y=0, \quad y=\pi\) when \(x=\pi / 2\)

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

Find the general solution of each of the following differential equations. \(\left(1+e^{x}\right) y^{\prime}+2 e^{x} y=\left(1+e^{x}\right) e^{x}\)

(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 the "general solution" (that is, a solution containing an arbitrary constant) of each of the following differential equations, by separation of variables. Then find a particular solution of each equation satisfying the given boundary conditions. \(y^{\prime}+2 x y^{2}=0\) \(y=1\) when \(x=2\)

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