Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Solve the following differential equations. . (D22D+1)y=0

Short Answer

Expert verified
The solution is y(t)=(C1+C2t)et

Step by step solution

01

- Identify the characteristic equation

Rewrite the differential equation in terms of the characteristic equation. For the differential equation (D22D+1)y=0, the equivalent characteristic equation is r22r+1=0.
02

- Solve characteristic equation

Solve the characteristic equation r22r+1=0. This is a quadratic equation which can be factored as (r1)2=0. Therefore, the roots are r=1 with multiplicity 2.
03

- Write the general solution

For a characteristic equation with a repeated root (in this case, r=1 repeated), the general solution to the differential equation is given by y(t)=(C1+C2t)erty(t)=(C1+C2t)ert. Since r=1, the final general solution is y(t)=(C1+C2t)et

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 Vaia!

Key Concepts

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

characteristic equation
The characteristic equation is a fundamental concept when solving linear differential equations. It connects the differential equation to a polynomial, making it easier to find solutions. In our example, we start with the second-order differential equation: (D22D+1)y=0By substituting the operator D with r, we can rewrite it as a polynomial, called the characteristic equation:r22r+1=0This transformation allows us to solve for r using algebraic methods, such as factoring or the quadratic formula. Finding the roots r is the key to determining the general solution of the differential equation.
general solution
The general solution of a second-order differential equation depends on the roots of its characteristic equation. After solving the characteristic equation, we found the roots: r=1Since this is a repeated root (multiplicity 2), we use a specific form to represent the general solution. For repeated roots, the general solution is given by: y(t)=(C1+C2t)ertHere, C1 and C2 are constants determined by initial conditions. In our case, with r=1, the solution becomes: y(t)=(C1+C2t)etThis formula encompasses all possible solutions to the original differential equation.
repeated roots
Repeated roots occur when solving the characteristic equation yields the same root more than once. In our example, the characteristic equation r22r+1=0factors as (r1)2=0indicating a repeated root at r=1. Repeated roots require a special treatment in forming the general solution. Instead of simply using exponential functions, we introduce an extra term involving the variable t, leading to the form: y(t)=(C1+C2t)ertThis ensures the solution captures all behaviors represented by the differential equation. The additional t term is essential in accounting for the root's multiplicity.
second-order differential equation
Second-order differential equations involve derivatives up to the second order. In general, they can be written as: ay+by+cy=0where a, b, and c are constants. The specific example we solved is: (D22D+1)y=0Here, D represents differentiation with respect to t. Solving these equations typically involves:
  • Formulating the characteristic equation
  • Finding its roots
  • Using the roots to write the general solution
Second-order differential equations show up in many physical phenomena such as oscillations, circuits, and mechanical systems, making them essential in various scientific and engineering fields.

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

A block of wood is floating in water; it is depressed slightly and then released to oscillate up and down. Assume that the top and bottom of the block are parallel planes which remain horizontal during the oscillations and that the sides of the block are vertical. Show that the period of the motion (neglecting friction) is 2πh/g, where h is the vertical height of the part of the block under water when it is floating at rest. Hint: Recall that the buoyant force is equal to the weight of displaced water.

Find the orthogonal trajectories of each of the following families of curves. In each case sketch several of the given curves and several of their orthogonal trajectories. Be careful to eliminate the constant from dy/dx for the original curves; this constant takes different values for different curves of the original family and you want an expression for dy/dx which is valid for all curves of the family crossed by the orthogonal trajectory you are trying to find. xy=k.

Solve the following differential equations. . (xy)dy+(y+x+1)dx=0

Find the orthogonal trajectories of each of the following families of curves. In each case sketch several of the given curves and several of their orthogonal trajectories. Be careful to eliminate the constant from dy/dx for the original curves; this constant takes different values for different curves of the original family and you want an expression for dy/dx which is valid for all curves of the family crossed by the orthogonal trajectory you are trying to find. y=kx2

Find the "general solution" (that is, a solution containing an arbitrary constant) of each of the following differential equations, by separation of variables. Then find a particular solution of each equation satisfying the given boundary conditions. y+2xy2=0 y=1 when x=2

See all solutions

Recommended explanations on Combined Science 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.

Sign-up for free