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find the general solution of the given differential equation. $$ y^{\prime \prime}+y^{\prime}+1.25 y=0 $$

Short Answer

Expert verified
Answer: The general solution is \(y(x) = e^{-\frac{1}{2}x}(A \cos(\frac{\sqrt{3}}{2}x) + B \sin (\frac{\sqrt{3}}{2}x))\), where A and B are arbitrary constants.

Step by step solution

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01

Identify the coefficients

Identify the coefficients of the given differential equation, which are: a = 1, b = 1, and c = 1.25. The equation is: $$ y^{\prime \prime} + y^{\prime} + 1.25 y=0 $$
02

Find the characteristic equation

Form the characteristic equation by replacing the derivatives with their corresponding powers of the variable r: $$ r^2 + r + 1.25 = 0 $$
03

Solve the characteristic equation

Now, solve for r to find the roots. We can use the quadratic formula: $$ r = \frac{-b\pm \sqrt{b^2-4ac}}{2a} $$ Substitute the known coefficients into the formula: $$ r = \frac{-1 \pm \sqrt{1^2-4(1)(1.25)}}{2(1)} $$
04

Simplify and determine roots

Upon simplification, we find that the discriminant, \(1-5 = -4\) is negative. Thus, we have complex roots: $$ r = \frac{-1 \pm \sqrt{-4}}{2} $$ Which simplifies to: $$ r_1 = -\frac{1}{2} + \frac{\sqrt{3}}{2}i, \quad r_2 = -\frac{1}{2} - \frac{\sqrt{3}}{2}i $$
05

Form the general solution based on roots

Since we have two distinct complex roots, \(r_1\) and \(r_2\), we can express the general solution of the given second-order differential equation as: $$ y(x) = e^{\alpha x}(A \cos(\beta x) + B \sin (\beta x)) $$ Using the real and imaginary parts of \(r_1\) and \(r_2\), \(\alpha = -\frac{1}{2}\) and \(\beta = \frac{\sqrt{3}}{2}\): $$ y(x) = e^{-\frac{1}{2}x}(A \cos(\frac{\sqrt{3}}{2}x) + B \sin (\frac{\sqrt{3}}{2}x)) $$
06

Write down the general solution

The general solution of the given second-order linear homogeneous differential equation is: $$ y(x) = e^{-\frac{1}{2}x}(A \cos(\frac{\sqrt{3}}{2}x) + B \sin (\frac{\sqrt{3}}{2}x)) $$ Here, A and B are arbitrary constants.

Key Concepts

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

Characteristic Equation
The characteristic equation is a vital tool when solving differential equations, especially second-order linear homogeneous ones. When given a differential equation like \( y'' + y' + 1.25y = 0 \), the characteristic equation helps us determine the roots that dictate the behavior of the solution.
The characteristic equation is created by replacing each derivative in the differential equation with a power of \( r \), a variable often used for this purpose. Therefore, for our example:
- Replace \( y' \) with \( r \)- Replace \( y'' \) with \( r^2 \)
This gives us the characteristic equation \( r^2 + r + 1.25 = 0 \). Assessing these roots enables us to analyze if they are real or complex, which then affects the form of the general solution.
Complex Roots
Complex roots occur when the discriminant of the characteristic equation is negative. In our example, the discriminant \((b^2 - 4ac)\) equals \(-4\) because \(1^2 - 4(1)(1.25) = -4\). This negative result indicates complex roots.
To actually find these roots, we apply the quadratic formula \( r = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \). Inserting the coefficients from our characteristic equation, we get:
- \( r = \frac{-1 \pm \sqrt{-4}}{2} \)
Which simplifies to:
- \( r_1 = -\frac{1}{2} + \frac{\sqrt{3}}{2}i \)- \( r_2 = -\frac{1}{2} - \frac{\sqrt{3}}{2}i \)
Complex roots involve both real and imaginary parts, which we use in forming the general solution.
General Solution
For differential equations with complex roots, like \( r_1 \) and \( r_2 \) found earlier, the general solution takes on a specific form. This form accommodates the oscillatory nature of complex solutions, combining exponential decay or growth with sine and cosine functions.
The general solution for complex roots \( \alpha \pm \beta i \) is expressed as:
- \( y(x) = e^{\alpha x}(A \cos(\beta x) + B \sin(\beta x)) \)
Where:- \( \alpha \) is the real part of the roots- \( \beta \) is the imaginary part
For our specific equation, with \( \alpha = -\frac{1}{2} \) and \( \beta = \frac{\sqrt{3}}{2} \), the solution follows:
- \( y(x) = e^{-\frac{1}{2}x}(A \cos(\frac{\sqrt{3}}{2}x) + B \sin(\frac{\sqrt{3}}{2}x)) \)
Here, \( A \) and \( B \) represent constants determined by initial conditions.
Second-Order Linear Homogeneous Differential Equation
Second-order linear homogeneous differential equations are a fundamental class of differential equations. They typically look like \( a y'' + b y' + c y = 0 \), where:- \( y'' \) is the second derivative of \( y \)- \( y' \) is the first derivative- \( y \) is the function itself- \( a, b, \) and \( c \) are constants
These equations are homogeneous, meaning that every term includes the function \( y \) or its derivatives directly, without any standalone functions or constants.
To solve these equations, one derives a characteristic equation from which the roots are calculated. The nature of these roots—whether real or complex—guides the formulation of the general solution. This forms the basis for understanding and solving higher-order differential equations comprehensively.

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Most popular questions from this chapter

Consider the vibrating system described by the initial value problem $$ u^{\prime \prime}+u=3 \cos \omega t, \quad u(0)=1, \quad u^{\prime}(0)=1 $$ (a) Find the solution for \(\omega \neq 1\). (b) Plot the solution \(u(t)\) versus \(t\) for \(\omega=0.7, \omega=0.8,\) and \(\omega=0.9 .\) Compare the results with those of Problem \(18,\) that is, describe the effect of the nonzero initial conditions.

The method of Problem 20 can be extended to second order equations with variable coefficients. If \(y_{1}\) is a known nonvanishing solution of \(y^{\prime \prime}+p(t) y^{\prime}+q(t) y=0,\) show that a second solution \(y_{2}\) satisfies \(\left(y_{2} / y_{1}\right)^{\prime}=W\left(y_{1}, y_{2}\right) / y_{1}^{2},\) where \(W\left(y_{1}, y_{2}\right)\) is the Wronskian \(\left. \text { of }\left.y_{1} \text { and } y_{2} \text { . Then use Abel's formula [Eq. ( } 8\right) \text { of Section } 3.3\right]\) to determine \(y_{2}\).

(a) Determine a suitable form for \(Y(t)\) if the method of undetermined coefficients is to be used. (b) Use a computer algebra system to find a particular solution of the given equation. $$ y^{\prime \prime}+y=t(1+\sin t) $$

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In the spring-mass system of Problem \(31,\) suppose that the spring force is not given by Hooke's law but instead satisfies the relation $$ F_{s}=-\left(k u+\epsilon u^{3}\right) $$ where \(k>0\) and \(\epsilon\) is small but may be of either sign. The spring is called a hardening spring if \(\epsilon>0\) and a softening spring if \(\epsilon<0 .\) Why are these terms appropriate? (a) Show that the displacement \(u(t)\) of the mass from its equilibrium position satisfies the differential equation $$ m u^{\prime \prime}+\gamma u^{\prime}+k u+\epsilon u^{3}=0 $$ Suppose that the initial conditions are $$ u(0)=0, \quad u^{\prime}(0)=1 $$ In the remainder of this problem assume that \(m=1, k=1,\) and \(\gamma=0\). (b) Find \(u(t)\) when \(\epsilon=0\) and also determine the amplitude and period of the motion. (c) Let \(\epsilon=0.1 .\) Plot (a numerical approximation to) the solution. Does the motion appear to be periodic? Estimate the amplitude and period. (d) Repeat part (c) for \(\epsilon=0.2\) and \(\epsilon=0.3\) (e) Plot your estimated values of the amplitude \(A\) and the period \(T\) versus \(\epsilon\). Describe the way in which \(A\) and \(T\), respectively, depend on \(\epsilon\). (f) Repeat parts (c), (d), and (e) for negative values of \(\epsilon .\)

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