/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 35 Solve the given initial-value pr... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Solve the given initial-value problem. \(y^{\prime \prime \prime}-2 y^{\prime \prime}+y^{\prime}=2-24 e^{x}+40 e^{5 x}, y(0)=\frac{1}{2}, y^{\prime}(0)=\frac{5}{2}\), \(y^{\prime \prime}(0)=-\frac{9}{2}\)

Short Answer

Expert verified
The solution is \( y(x) = \frac{1}{2} + 801 e^{x} - \frac{1601}{2} xe^{x} + 40e^{5x} \).

Step by step solution

01

Write the Form of the General Solution

The given equation is a non-homogeneous linear differential equation with constant coefficients:\[ y''' - 2y'' + y' = 2 - 24e^{x} + 40e^{5x} \]First, solve the homogeneous equation:\[ y''' - 2y'' + y' = 0 \] Find the complementary solution (\(y_c\)) by solving the characteristic equation.
02

Solve the Characteristic Equation

The characteristic equation for the homogeneous equation is:\[ r^3 - 2r^2 + r = 0 \]Factoring out an \(r\), gives:\[ r(r^2 - 2r + 1) = 0 \]This simplifies to \(r=0\) and \( (r-1)^2 = 0 \), giving roots \(r = 0, 1, 1\). The solution to the homogeneous equation is:\[ y_c = C_1 + C_2 e^{x} + C_3 xe^{x} \]
03

Determine the Particular Solution

Next, assume a particular solution, \(y_p\), due to the non-homogeneous part.We try solutions of the form:\[ y_p = A + Be^{x} + Ce^{5x} \]Derive \(y_p', y_p''\), and \(y_p'''\) and substitute into:\[ y''' - 2y'' + y' = 2 - 24e^{x} + 40e^{5x} \] and solve for the coefficients \(A, B, C\).
04

Solve for Coefficients in Particular Solution

The derivatives of \(y_p\) are:- \(y_p' = Be^{x} + 5Ce^{5x}\)- \(y_p'' = Be^{x} + 25Ce^{5x}\)- \(y_p''' = Be^{x} + 125Ce^{5x}\)Substitute these into the original equation:\[ Be^{x} + 125Ce^{5x} - 2(Be^{x} + 25Ce^{5x}) + (Be^{x} + 5Ce^{5x}) = 2 - 24e^{x} + 40e^{5x} \]Simplifying gives:\[ -24e^{x} + 40e^{5x} = 2 - 24e^{x} + 40e^{5x} \]Thus, \(A = 2, B = 0, C = 40\) so:\[ y_p = 2 + 40e^{5x} \]
05

Combine Solutions

The general solution is:\[ y = y_c + y_p = C_1 + C_2 e^{x} + C_3 xe^{x} + 2 + 40e^{5x} \]
06

Apply Initial Conditions

Apply the initial conditions to solve for the constants:1. \(y(0)=\frac{1}{2}\): \[ C_1 + 2 = \frac{1}{2} \rightarrow C_1 = -\frac{3}{2} \]2. \(y'(0)=\frac{5}{2}\): \[ y'(x) = C_2 e^{x} + C_3 e^{x} + C_3 xe^{x} + 200e^{5x} \] \[ \text{At } x=0, y'(0) = C_2 + C_3 + 200 = \frac{5}{2} \]3. \(y''(0)=-\frac{9}{2}\): \[ y''(x) = C_2 e^{x} + 2C_3 e^{x} + C_3 xe^{x} + 1000e^{5x} \] \[ \text{At } x=0, y''(0) = C_2 + 2C_3 + 1000 = -\frac{9}{2} \]Solve these equations to find \(C_2\) and \(C_3\).
07

Solve for Constants

From the equation system:- \(C_1 = -\frac{3}{2}\)- \(C_2 + C_3 + 200 = \frac{5}{2} \) implies \(C_2 + C_3 = \frac{5}{2} - 200 = -\frac{395}{2}\)- \(C_2 + 2C_3 + 1000 = -\frac{9}{2} \) implies \(C_2 + 2C_3 = -\frac{9}{2} - 1000 = -\frac{2009}{2}\)Solving these gives \(C_2 = 801\) and \(C_3 = -\frac{1601}{2}\).
08

Write the Final Solution

Substitute the constants back into the general solution:\[ y(x) = -\frac{3}{2} + 801 e^{x} - \frac{1601}{2} xe^{x} + 2 + 40e^{5x} \]Thus, the final solution to the initial-value problem is:\[ y(x) = \frac{1}{2} + 801 e^{x} - \frac{1601}{2} xe^{x} + 40e^{5x} \]

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Initial-Value Problems
An initial-value problem involves a differential equation along with specified values at the initial point of the variables involved. These particular values, known as initial conditions, allow us to find a unique solution to a differential equation.
The given problem involves the third-order differential equation:
\( y''' - 2y'' + y' = 2 - 24e^{x} + 40e^{5x} \), with initial conditions \( y(0)=\frac{1}{2} \), \( y'(0)=\frac{5}{2} \), and \( y''(0)=-\frac{9}{2} \).
The goal is to find the function \( y(x) \) that satisfies both this differential equation and the initial conditions.
  • Initial conditions provide specific values of the function and its derivatives at a starting point.
  • They are essential to distinguish between multiple possible solutions.
Understanding and applying initial-value problems is vital in predicting and modeling physical phenomena, where specific conditions are always present at the start.
Particular Solution
The particular solution of a differential equation deals with finding a specific solution to the non-homogeneous equation, differentiating it from the general solution.
In this equation, \( y''' - 2y'' + y' = 2 - 24e^{x} + 40e^{5x} \), we aim to find \( y_p \):
  • The particular solution is influenced by the non-homogeneous part (\(2 - 24e^{x} + 40e^{5x}\)).
  • We assume a form for \( y_p \), usually involving constants and functions matching those in the problem.
For this exercise:
Suppose \( y_p = A + Be^{x} + Ce^{5x} \).
By substituting and matching coefficients:
- The derivatives are substituted back into the equation, leading us to solve for the coefficients \(A, B, C\).
Thus, \( y_p = 2 + 40e^{5x} \) based on the particularities here.
Complementary Solution
The complementary solution is the part of the general solution to a homogeneous differential equation.
For the homogeneous counterpart of our differential equation:
\( y''' - 2y'' + y' = 0 \)
We found the complementary solution, \( y_c \), by solving the characteristic equation.
  • The roots of the characteristic equation provide us the basis for \( y_c \).
The characteristic equation:
\( r^3 - 2r^2 + r = 0 \), factored to get:\( r(r-1)^2 = 0 \), yields roots \( r = 0, 1, 1 \).
This gives:
\( y_c = C_1 + C_2 e^{x} + C_3 xe^{x} \).
The complementary solution represents all the possible solutions to the homogeneous equation and forms a foundation for the overall solution.
Characteristic Equation
A characteristic equation is essential for solving linear homogeneous differential equations with constant coefficients.
For the differential equation \( y''' - 2y'' + y' = 0 \), the associated characteristic equation is derived by replacing each derivative with powers of \( r \):
  • The characteristic equation reflects the algebraic form: \( r^3 - 2r^2 + r = 0 \).
  • Solving it gives us the vital roots \( r \) which inform on the nature of the complementary solution.
Through factoring \( r \) out, it becomes:
\( r(r^2 - 2r + 1) = 0 \), which further simplifies to \( r(r-1)^2 = 0 \) with roots \( r = 0, 1, 1 \).
Each root corresponds to a component in the complementary solution:
- Different roots give distinct solutions.
These steps are crucial as they determine how the general solution is structured and how specific solutions to these differential equations can be articulated.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Use the substitution \(x=e^{t}\) to transform the given Cauchy-Euler equation to a differential equation with constant coefficients. Solve the original equation by solving the new equation using the procedures in Sections 3.3-3.5. $$ x^{2} y^{\prime \prime}-9 x y^{\prime}+25 y=0 $$

Consider a pendulum that is released from rest from an initial displacement of \(\theta_{0}\) radians. Solving the linear model (7) subject to the initial conditions \(\theta(0)=\theta_{0}, \theta^{\prime}(0)=0\) gives \(\theta(t)=\theta_{0} \cos \sqrt{g} \| t .\) Theperiod of oscillations predicted by this modelisgivenbythefamiliarformula \(T=2 \pi / \sqrt{g l l}=2 \pi \sqrt{U g}\). The interesting thing about this formula for \(T\) is that it does not depend on the magnitude of the initial displacement \(\theta_{0}\). In other words, the linear model predicts that the time that it would take the pendulum to swing from an initial displacement of, say, \(\theta_{0}=\pi / 2\left(=90^{\circ}\right)\) to \(-\pi / 2\) and back again would be exactly the same time to cycle from, say, \(\theta_{0}=\pi / 360\left(=0.5^{\circ}\right)\) to \(-\pi / 360\). This is intuitively unreasonable; the actual period must depend on \(\theta_{0}\). If we assume that \(g=32 \mathrm{ft} / \mathrm{s}^{2}\) and \(l=32 \mathrm{ft}\), then the period of oscillation of the linear model is \(T=2 \pi \mathrm{s}\). Let us compare this last number with the period predicted by the nonlinear model when \(\theta_{0}=\pi / 4\). Using a numerical solver that is capable of generating hard data, approximate the solution of $$\frac{d^{2} \theta}{d t^{2}}+\sin \theta=0, \quad \theta(0)=\frac{\pi}{4}, \quad \theta^{\prime}(0)=0$$ for \(0 \leq t \leq 2\). As in Problem 24 , if \(t_{1}\) denotes the first time the pendulum reaches the position \(O P\) in Figure 3.11.3, then the period of the nonlinear pendulum is \(4 t_{1} .\) Here is another way of solving the equation \(\theta(t)=0\). Expeniment with small step sizes and advance the time staning at \(t=0\) and ending at \(t=2\). From your hard data, observe the time \(t_{1}\) when \(\theta(t)\) changes, for the first time, from positive to negative. Use the value \(t_{1}\) to determine the true value of the period of the nonlinear pendulum. Compute the percentage relative error in the period estimated by \(T=2 \pi\).

$$ y^{(4)}+2 y^{\prime \prime}-y^{\prime}+2 y=0 $$

Use the substitution \(y=\left(x-x_{0}\right)^{m}\) to solve the given equation. $$ (x-4)^{2} y^{\prime \prime}-5(x-4) y^{\prime}+9 y=0 $$

Solve the given system of differential equations by systematic elimination. $$ \begin{aligned} &\frac{d x}{d t}=-x+z \\ &\frac{d y}{d t}=-y+z \\ &\frac{d z}{d t}=-x+y \end{aligned} $$

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.