ï + x + ex = 0, with x(0) = 1, ¿(0) = 1.

Advanced Engineering Mathematics
10th Edition
ISBN:9780470458365
Author:Erwin Kreyszig
Publisher:Erwin Kreyszig
Chapter2: Second-order Linear Odes
Section: Chapter Questions
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Using pertubation theory, find x0, x1, and x2 in the series expansion x(t,epsilon)=x0(t)+epsilon x1(t) + epsilon^2  x2(t) + O(epsilon^3).

This differential equation is given by:

\[
\ddot{x} + x + \epsilon x = 0,
\]

with initial conditions:

\[
x(0) = 1, \quad \dot{x}(0) = 1.
\]

### Explanation:

This is a second-order linear differential equation with a small parameter \(\epsilon\). The function \(x(t)\) represents the unknown solution, with its second derivative given by \(\ddot{x}\) and first derivative by \(\dot{x}\).

### Initial Conditions:

- \(x(0) = 1\): the initial position at time \(t = 0\) is 1.
- \(\dot{x}(0) = 1\): the initial velocity at time \(t = 0\) is 1.

This equation might be used to model different physical phenomena, like oscillations in mechanical or electrical systems, depending on the value of \(\epsilon\).
Transcribed Image Text:This differential equation is given by: \[ \ddot{x} + x + \epsilon x = 0, \] with initial conditions: \[ x(0) = 1, \quad \dot{x}(0) = 1. \] ### Explanation: This is a second-order linear differential equation with a small parameter \(\epsilon\). The function \(x(t)\) represents the unknown solution, with its second derivative given by \(\ddot{x}\) and first derivative by \(\dot{x}\). ### Initial Conditions: - \(x(0) = 1\): the initial position at time \(t = 0\) is 1. - \(\dot{x}(0) = 1\): the initial velocity at time \(t = 0\) is 1. This equation might be used to model different physical phenomena, like oscillations in mechanical or electrical systems, depending on the value of \(\epsilon\).
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