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\(2 d^{2} x / d t^{2}+3 d x / d t+x=0, x(0)=-1\), \(x^{\prime}(0)=2\)

Short Answer

Expert verified
The solution to the differential equation is \( x(t) = -\frac{1}{3} e^{-\frac{1}{2} t} - \frac{2}{3} e^{-t} \).

Step by step solution

01

Identify the type of differential equation

The given equation is a second-order linear homogeneous differential equation: \[ 2 \frac{d^{2} x}{d t^{2}} + 3 \frac{d x}{d t} + x = 0 \]
02

Formulate the characteristic equation

Convert the differential equation into its characteristic (auxiliary) equation. The characteristic equation for \( a \frac{d^{2}x}{dt^{2}} + b \frac{dx}{dt} + cx = 0 \) is given by:\[ ar^{2} + br + c = 0 \]In this case: \[ 2r^{2} + 3r + 1 = 0 \]
03

Solve the characteristic equation

Solve the quadratic equation \( 2r^{2} + 3r + 1 = 0 \) using the quadratic formula \( r = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \): \[ r = \frac{-3 \pm \sqrt{3^2 - 4(2)(1)}}{2(2)} = \frac{-3 \pm 1}{4} \]So the roots are: \[ r_1 = -\frac{1}{2} \quad \text{and} \quad r_2 = -1 \]
04

Write the general solution

Since the roots of the characteristic equation are distinct and real, the general solution of the differential equation is: \[ x(t) = C_1 e^{r_1 t} + C_2 e^{r_2 t} \]Substitute \( r_1 \) and \( r_2 \): \[ x(t) = C_1 e^{-\frac{1}{2} t} + C_2 e^{-t} \]
05

Determine the constants using initial conditions

Use the initial conditions \( x(0) = -1 \) and \( x^{\prime}(0) = 2 \) to find \( C_1 \) and \( C_2 \). First, substitute \( t = 0 \) into \( x(t) \): \[ -1 = C_1 e^{0} + C_2 e^{0} \Rightarrow -1 = C_1 + C_2 \quad (1) \]Next, find \( x^{\prime}(t) \): \[ x^{\prime}(t) = -\frac{1}{2} C_1 e^{-\frac{1}{2} t} - C_2 e^{-t} \]Use the initial condition \( x^{\prime}(0) = 2 \): \[ 2 = -\frac{1}{2} C_1 e^{0} - C_2 e^{0} \Rightarrow 2 = -\frac{1}{2} C_1 - C_2 \quad (2) \]
06

Solve the system of equations for constants

Solve the equations (1) and (2) to find the values of \( C_1 \) and \( C_2 \): \( C_1 + C_2 = -1 \quad (1) \)\( -\frac{1}{2} C_1 - C_2 = 2 \quad (2) \)Multiply equation (1) by 2: \[ 2C_1 + 2C_2 = -2 \quad (3) \]Add equations (2) and (3): \[ 2C_1 + 2C_2 - \frac{1}{2}C_1 - C_2 = -2 + 2 \]\[ \frac{3}{2}C_1 + C_2 = 0 \Rightarrow \frac{3}{2}C_1 = -\frac{1}{2} \Rightarrow C_1 = -\frac{1}{3} \]Substitute \( C_1 \) back into equation (1): \[ -\frac{1}{3} + C_2 = -1 \Rightarrow C_2 = -\frac{2}{3} \]
07

Write the specific solution

Substitute \( C_1 \) and \( C_2 \) back into the general solution: \[ x(t) = -\frac{1}{3} e^{-\frac{1}{2} t} - \frac{2}{3} e^{-t} \]

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Key Concepts

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

characteristic equation
In solving second-order linear homogeneous differential equations, the characteristic equation is essential. It's derived from the given differential equation. For example, consider the equation:
\[2 \frac{d^{2} x}{d t^{2}} + 3 \frac{d x}{d t} + x = 0 \]
To find the characteristic equation, we replace \( \frac{d^2x}{dt^2} \) with \( r^2 \), \( \frac{dx}{dt} \) with \( r \), and \( x \) with 1. This transformation simplifies the differential equation into an algebraic quadratic equation:
\[2r^{2} + 3r + 1 = 0 \]
Solving this quadratic equation gives us the characteristic roots, which are pivotal for finding the general solution. The roots provide insight into the nature of the solution, whether it involves real or complex exponentials.
initial conditions
Initial conditions are crucial for determining the specific solution of a differential equation. They allow us to find the exact values of the constants in the general solution. Let's say we have the initial conditions as follows:
\( x(0) = -1 \) and \( x^{\rightarrow}(0) = 2 \).
First, we substitute these conditions into the general solution obtained from the characteristic equation. For example, if our general solution is:
\[x(t) = C_1 e^{-\frac{1}{2} t} + C_2 e^{-t} \],
we use \( t = 0 \) to form an equation and then solve a system of equations to find the constants \( C_1 \) and \( C_2 \). These constants adjust the general pattern of the solution to fit the specific problem's requirements.
homogeneous differential equation
A differential equation is homogeneous if all terms are related to the function and its derivatives. There are no standalone terms or functions of other variables. For example:
\[2 \frac{d^{2} x}{d t^{2}} + 3 \frac{d x}{d t} + x = 0 \]
This is homogeneous because each term involves either \( x \), \( \frac{dx}{dt} \), or \( \frac{d^2x}{dt^2} \). Homogeneous equations are a subset of linear differential equations and are solvable using specific techniques like forming and solving characteristic equations. The absence of non-zero constant or non-homogenous terms (terms that are functions of \( t \), but not multiplying \( x \) or its derivatives) makes these equations simpler to solve.
quadratic formula
The quadratic formula is a mathematical tool used to find the roots of a quadratic equation. Given a standard form quadratic equation \( ar^{2} + br + c = 0 \), the quadratic formula is:
\[r = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a} \]
This formula provides two solutions, one for the plus and one for the minus. For example, in the equation:
\[2r^2 + 3r + 1 = 0 \],
we identify \( a = 2 \), \( b = 3 \), and \( c = 1 \). Plugging these into the quadratic formula, we get:
\[r = \frac{-3 \pm \sqrt{3^2 - 4(2)(1)}}{2(2)} = \frac{-3 \pm 1}{4} \]
This results in roots \( r_1 = -\frac{1}{2} \) and \( r_2 = -1 \), which are then used to form the general solution of the differential equation. The quadratic formula is a fundamental method in finding these roots easily and accurately.

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Most popular questions from this chapter

\(x^{\prime \prime}+4 x=0, x(0)=1, x^{\prime}(0)=1\)

An object of mass \(m=2 \mathrm{~kg}\) is attached to a spring with spring constant \(k=1 \mathrm{~kg} / \mathrm{m}\). If the resistive force is \(F_{R}=3 d x / d t\) and the external force is \(f(t)=2 \cos \omega t\), find the displacement of the object if \(x(0)=0\) and \(x^{\prime}(0)=0\). Will resonance occur for any values of \(\omega\) ?

A 4-lb weight stretches a spring \(1 \mathrm{ft}\). A 16 - \(\mathrm{lb}\) weight is then attached to the spring, and it comes to rest in its equilibrium position. If it is then put into motion with a downward velocity of \(2 \mathrm{ft} / \mathrm{s}\), determine the displacement of the mass. What is the maximum displacement of the object? When does it occur?

An object of mass \(m=70 \mathrm{~kg}\) is attached to the end of a spring and stretches the spring \(0.25 \mathrm{~m}\) beyond its natural length. If the restrictive force is \(F_{R}=280 d x / d t\), find the displacement of the object if it is released from a position \(3 \mathrm{~m}\) above its equilibrium position with no initial velocity. Does the object pass through its equilibrium position at any time?

A \(32 \mathrm{lb}\) weight is attached to the end of a spring with spring constant \(k=24 \mathrm{lb} / \mathrm{ft}\). If the resistive force is \(F_{R}=10 d x / d t\), determine the displacement of the mass if it is released with no initial velocity from a position 6 in above the equilibrium position. Determine if the mass passes through its equilibrium position and, if so, when. Determine the maximum displacement of the object from the equilibrium position.

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