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In each of Problems 1 through 10 find the general solution of the given differential equation. \(4 y^{\prime \prime}+17 y^{\prime}+4 y=0\)

Short Answer

Expert verified
Answer: The general solution of the given differential equation is \(y(x) = C_1 e^{-1x} + C_2 e^{-4x}\), where \(C_1\) and \(C_2\) are arbitrary constants.

Step by step solution

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01

Write down the given differential equation

The given second-order linear homogeneous differential equation is: \(4 y^{\prime \prime}+17 y^{\prime}+4 y=0\)
02

Formulate the characteristic equation

Replace \(y^{\prime \prime}\) with \(r^2\), \(y^{\prime}\) with \(r\), and \(y\) with 1: \(4r^2 + 17r + 4 = 0\)
03

Solve the characteristic equation

Now solve for r in the quadratic equation \(4r^2 + 17r + 4 = 0\). We may factor the quadratic as \((r+1)(4r+4)=0\), or simply use the quadratic formula: \(r = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\), where \(a=4\), \(b=17\), and \(c=4\). \(r_1 = \frac{-17 + \sqrt{17^2 - 4\cdot4\cdot4}}{2\cdot4} = -1\) \(r_2 = \frac{-17 - \sqrt{17^2 - 4\cdot4\cdot4}}{2\cdot4} = -4\)
04

Write the general solution of the differential equation

Since we have two distinct real roots, the general solution of the given differential equation is: \(y(x) = C_1 e^{r_1 x} + C_2 e^{r_2 x}\) Substitute the values of \(r_1\) and \(r_2\) we found in Step 3: \(y(x) = C_1 e^{-1x} + C_2 e^{-4x}\) Here, \(C_1\) and \(C_2\) are arbitrary constants. This is the general solution to the given differential equation.

Key Concepts

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

Characteristic Equation
Understanding the characteristic equation is fundamental to solving second-order linear homogeneous differential equations. The characteristic equation is derived from the original differential equation by replacing the derivative terms with powers of a variable (typically denoted as 'r'). For example, for a second derivative \( y^{\prime \prime} \) you would use \( r^2 \), and similarly \( y^{\prime} \) would be represented by \( r \). This transformation results in a polynomial equation that reflects the structure of the differential equation.

To illustrate, consider the exercise where the differential equation is \( 4y^{\prime \prime} + 17y^{\prime} + 4y = 0 \). By replacing the derivatives, we obtain the characteristic equation \( 4r^2 + 17r + 4 = 0 \) which is a quadratic equation in terms of 'r'. This equation can be solved by factoring, as shown in the steps provided, or by using the quadratic formula \( r = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \) as an alternative method if factoring is not straightforward.
Second-Order Linear Homogeneous Differential Equation
A second-order linear homogeneous differential equation has the form \( a y^{\prime \prime} + b y^{\prime} + c y = 0 \), where \( a \), \( b \) and \( c \) are constants. In the context of this exercise, we are looking at a differential equation in which the right-hand side is zero, denoting it 'homogeneous'.

To solve this type of equation, we rely on the characteristic equation as previously discussed. The roots of the characteristic equation, which can be real or complex, dictate the form of the general solution. If the roots are real and distinct, as with \( r_1 \) and \( r_2 \) found in our example problem, the general solution is a linear combination of exponential functions: \( y(x) = C_1 e^{r_1 x} + C_2 e^{r_2 x} \). On the other hand, if the roots are real and repeated or complex, the form of the solution will differ, involving repeated exponential terms or sinusoids and cosines, respectively.
General Solution of Differential Equation
The general solution of a differential equation incorporates the entire family of solutions that satisfy the equation. It includes arbitrary constants, \( C_1 \) and \( C_2 \) in our case, because the second-order differential equation results in a solution space spanned by two linearly independent functions. These constants represent the initial conditions or specifics of a particular solution within the general family.

In the given exercise, after finding the roots of the characteristic equation, we construct the general solution by combining the exponential terms involving the roots and the arbitrary constants: \( y(x) = C_1 e^{-1x} + C_2 e^{-4x} \). This expression can fit infinite scenarios depending on the values assigned to \( C_1 \) and \( C_2 \), which are typically determined from initial value conditions or boundary conditions given in a specific problem. It's crucial for students to understand that these constants are essential in tailoring the general solution to the particular problem at hand.

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Most popular questions from this chapter

try to transform the given equation into one with constant coefficients by the method of Problem 34. If this is possible, find the general solution of the given equation. $$ t y^{\prime \prime}+\left(t^{2}-1\right) y^{\prime}+t^{3} y=0, \quad 0

In each of Problems 1 through 12 find the general solution of the given differential equation. $$ y^{\prime \prime}-2 y^{\prime}-3 y=3 e^{2 x} $$

A mass of \(5 \mathrm{kg}\) stretches a spring \(10 \mathrm{cm} .\) The mass is acted on by an external force of \(10 \mathrm{sin}(t / 2) \mathrm{N}\) (newtons) and moves in a medium that imparts a viscous force of \(2 \mathrm{N}\) when the speed of the mass is \(4 \mathrm{cm} / \mathrm{sec} .\) If the mass is set in motion from its equilibrium position with an initial velocity of \(3 \mathrm{cm} / \mathrm{sec}\), formulate the initial value problem describing the motion of the mass.

By combining the results of Problems 24 through \(26,\) show that the solution of the initial value problem $$ L[y]=\left(a D^{2}+b D+c\right) y=g(t), \quad y\left(t_{0}\right)=0, \quad y^{\prime}\left(t_{0}\right)=0 $$ where \(a, b,\) and \(c\) are constants, has the form $$ y=\phi(t)=\int_{t_{0}}^{t} K(t-s) g(s) d s $$ The function \(K\) depends only on the solutions \(y_{1}\) and \(y_{2}\) of the corresponding homogeneous equation and is independent of the nonhomogeneous term. Once \(K\) is determined, all nonhomogeneous problems involving the same differential operator \(L\) are reduced to the evaluation of an integral. Note also that although \(K\) depends on both \(t\) and \(s,\) only the combination \(t-s\) appears, so \(K\) is actually a function of a single variable. Thinking of \(g(t)\) as the input to the problem and \(\phi(t)\) as the output, it follows from Eq. (i) that the output depends on the input over the entire interval from the initial point \(t_{0}\) to the current value \(t .\) The integral in Eq. (i) is called the convolution of \(K\) and \(g,\) and \(K\) is referred to as the kernel.

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