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

Short Answer

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The differential equation is a linear second-order equation. The solution is \(y(x) = C + x^2\).

Step by step solution

01

Identify the Type of Differential Equation

First, consider the given differential equation: \(x y^{\backprime \backprime}+y^{\backprime}=4 x\). Notice that it involves the second derivative of \(y\) and the first derivative of \(y\), making it a second-order differential equation. It can be recast in standard linear form.
02

Rewrite the Equation in Standard Linear Form

The differential equation can be rewritten as: \[xy^{\backprime \backprime} + y^{\backprime} = 4x\]. This can be simplified to \[y^{\backprime \backprime} + \frac{1}{x} y^{\backprime} = 4\] by dividing both sides by \(x\). This is a linear non-homogeneous second-order differential equation.
03

Solve the Homogeneous Equation

Solve the homogeneous part of the equation: \[y^{\backprime \backprime} + \frac{1}{x} y^{\backprime} = 0\]. To do this, assume a solution of the form \(y = x^m\). Then, \(y^{\backprime} = mx^{m-1}\) and \(y^{\backprime \backprime} = m(m-1)x^{m-2}\). Substituting these into the homogeneous equation gives: \[m(m-1)x^{m-2} + \frac{m}{x}x^{m-1} = 0\]. Simplifying this, we get: \[m(m-1) + m = 0 \Rightarrow m^2 = 0 \Rightarrow m = 0\]. Thus, the homogeneous solution is \(y_h = C\) where \(C\) is a constant.
04

Solve the Non-Homogeneous Equation

For the non-homogeneous equation, we can use the method of undetermined coefficients. Assume a particular solution of the form \(y_p = Ax^2\). Then, \(y_p\backprime = 2Ax\) and \(y_p\backprime \backprime = 2A\). Substitute these into the non-homogeneous equation: \[2A + \frac{2Ax}{x} = 4\]. Simplifying, we get: \[2A + 2A = 4 \Rightarrow 4A = 4 \Rightarrow A = 1\]. So, the particular solution is \(y_p = x^2\).
05

Write the General Solution

Combine the homogeneous solution \(y_h\) with the particular solution \(y_p\) to form the general solution: \[y(x) = y_h + y_p = C + x^2\].

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Key Concepts

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

Linear Differential Equations
A linear differential equation is an equation involving derivatives of a function where each term is linear in the unknown function and its derivatives. In simpler terms, the dependent variable (like y) and its derivatives appear to the power of one and are not multiplied or divided by each other.
In our example, the differential equation \( x y^{\prime \prime} + y^{\prime} = 4x \) can be recast into standard linear form: \[ y^{\prime \prime} + \frac{1}{x} y^{\prime} = 4 \]. This makes it a second-order linear differential equation because it involves a second derivative, a first derivative, and powers of the variable x. Linear differential equations can be solved using various methods, like the method of undetermined coefficients.
Homogeneous Equations
Homogeneous differential equations are a type of differential equation where all terms involve derivatives of the same function, and the equation is set to zero. In essence, there is no external forcing function or non-homogeneous term.
For instance, consider the homogeneous part of our given equation: \( y^{\prime \prime} + \frac{1}{x} y^{\prime} = 0 \). The right-hand side is zero, indicating that it’s homogeneous. Solving a homogeneous differential equation usually results in finding the complementary function or the general solution to the homogeneous part. Here, we solved it by assuming a solution of the form \( y = x^m \), which led to the homogeneous solution \( y_h = C \), where C is a constant.
Method of Undetermined Coefficients
The method of undetermined coefficients is a technique used to find the particular solution of a non-homogeneous linear differential equation. It involves guessing a form of the particular solution based on the non-homogeneous term and determining the coefficients by substitution.
For our equation \( y^{\prime \prime} + \frac{1}{x} y^{\prime} = 4 \), we guessed that the particular solution might be of the form \( y_p = Ax^2 \), because the right-hand side is a polynomial. Substituting this guess into the differential equation, we solved for A, finding that \( A=1 \). Therefore, our particular solution is \( y_p = x^2 \).
The method of undetermined coefficients works well for cases where the non-homogeneous term is a polynomial, exponential, sine, or cosine function.
Particular Solution
The particular solution to a differential equation is a specific solution that satisfies the non-homogeneous equation. It incorporates the non-homogeneous term of the equation and complements the general solution obtained from the homogeneous equation.
Combining the solutions we obtained: the homogeneous solution \( y_h = C \) and the particular solution \( y_p = x^2 \), gives the general solution to the original non-homogeneous equation. Therefore, the final answer is \( y(x) = C + x^2 \). This general solution includes all possible solutions to the differential equation and satisfies the initial or boundary conditions provided in specific problems.

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Most popular questions from this chapter

(a) Show that $$ \begin{aligned} D\left(e^{a x} y\right) &=e^{a x}(D+a) y \\ D^{2}\left(e^{a x} y\right) &=e^{a x}(D+a)^{2} y \end{aligned} $$ and so on, that is, for any positive integral \(n_{y}\) $$ D^{n}\left(e^{a x} y\right)=e^{a x}(D+a)^{n} y $$ Thus show that if \(L(D)\) is any polynomial in the operator \(D\), then $$L(D)\left(e^{a x} y\right)=e^{\alpha x} L(D+a) y$$ This is called the exponential shift.

(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 of each of the following differential equations. \(d y+\left(2 x y-x e^{-x^{2}}\right) d x=0\)

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

Solve the following differential equations. \(y^{\prime \prime}-4 y^{\prime}+4 y=0\)

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