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

find the fundamental set of solutions specified by Theorem 3.2.5 for the given differential equation and initial point. $$ y^{\prime \prime}+4 y^{\prime}+3 y=0, \quad t_{0}=1 $$

Short Answer

Expert verified
Based on the given differential equation and the step-by-step solution provided, the fundamental set of solutions for the differential equation is: $$ \{e^{-3t}, e^{-t}\} $$

Step by step solution

01

Write down the characteristic equation

The characteristic equation of the given differential equation is: $$ r^2 + 4r + 3 = 0 $$
02

Find the roots of the characteristic equation

We can solve the quadratic equation by factoring or using the quadratic formula, but in this case, the characteristic equation can be factored as: $$ (r + 3)(r + 1) = 0 $$ Hence, the roots are \(r_1 = -3\) and \(r_2 = -1\).
03

Write down the general solution

Since we have found two distinct real roots, the general solution of the differential equation is given by: $$ y(t) = C_1 e^{-3t} + C_2 e^{-t} $$ Now, we have the general solution, and we can find the fundamental set of solutions by applying the initial condition.
04

Apply the initial condition

The given initial point is \((t_0, y_0) = (1, 0)\). Substitute \(t_0=1\) into the general solution: $$ 0 = C_1 e^{-3(1)} + C_2 e^{-1(1)} $$ However, finding the constants \(C_1\) and \(C_2\) in this case is not necessary, because we only need the fundamental set of solutions. Notice that we do not have a value for \(y_0\) which would allow us to find a unique solution by solving for \(C_1\) and \(C_2\).
05

Write down the fundamental set of solutions

Since we have a second-order homogeneous linear differential equation, the fundamental set of solutions consists of the two linearly independent solutions given by the general solution. Hence, the fundamental set of solutions can be written as: $$ \{e^{-3t}, e^{-t}\} $$

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.

Second-Order Differential Equation
A second-order differential equation involves the second derivative of a function. The equation we are examining is in the form:\[y'' + 4y' + 3y = 0\]Here, \(y\) is a function of \(t\), \(y'\) is the first derivative, and \(y''\) is the second derivative.
  • "Second-order" indicates that the highest derivative is the second derivative \(y''\).
  • Such equations often describe systems where the rate of change of the rate of change (like acceleration) is considered.
These equations are crucial in expressing real-world phenomena such as the motion of mechanical systems, electrical circuits, and more.
The second-order linear differential equation can additionally be categorized based on other properties, such as homogeneity and linearity.
Linear Homogeneous Differential Equations
A linear homogeneous differential equation can be recognized by its structure and the condition that all terms involve either the function or its derivatives.
In the equation \(y'' + 4y' + 3y = 0\), neither standalone constants nor functions of \(t\) appear.
  • "Linear" here means that the function \(y(t)\) and its derivatives appear to the power of 1.
  • "Homogeneous" indicates that the entire equation equals zero, without any external function term on the right-hand side.
Linear homogeneous equations are significant in various studies because they allow for the superposition principle. This means that if \(y_1(t)\) and \(y_2(t)\) are solutions, then any linear combination \(C_1y_1(t) + C_2y_2(t)\) is also a solution. This makes finding solutions systematic and applicable to complex scenarios like vibrations and waves.
Characteristic Equation
The characteristic equation is vital to solving second-order linear differential equations. It helps find the solution by converting a differential equation into an algebraic one.
To derive it, replace the derivatives in the differential equation with powers of a variable (commonly \(r\)). For \(y'' + 4y' + 3y = 0\), the characteristic equation becomes:\[r^2 + 4r + 3 = 0\]
  • Solving this quadratic equation provides the roots \(r_1\) and \(r_2\).
  • The roots inform us about the general solution of the differential equation.
In this context, the equation allows us to factor it into: \[(r + 3)(r + 1) = 0\]yielding \(r_1 = -3\) and \(r_2 = -1\). These roots describe the exponents in the general solution's terms, guiding us to the fundamental set of solutions.
Initial Value Problem
An initial value problem (IVP) involves not only finding a general solution to a differential equation but also determining a specific solution that meets given conditions.
For the given differential equation, the initial condition is typically specified at a particular point \((t_0, y_0)\). Even though in our problem, \((t_0 = 1, y_0)\) lacks enough information to determine specific constants for a unique solution, it provides direction in certain contexts.
  • The condition \(y(t_0) = y_0\) helps identify particular solutions in other scenarios.
  • Solving an IVP ensures that solutions accurately fit physical or real-life initial conditions.
While the fundamental set of solutions \( \{e^{-3t}, e^{-t}\} \) provides the basis, in many cases, specific initial conditions are necessary to pin down unique solutions.

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

If \(a, b,\) and \(c\) are positive constants, show that all solutions of \(a y^{\prime \prime}+b y^{\prime}+c y=0\) approach zero as \(t \rightarrow \infty\).

try to transform the given equation into one with constant coefficients by the method of Problem 34. If this is possible, find the general solution of the given equation. $$ y^{\prime \prime}+t y^{\prime}+e^{-t^{2}} y=0, \quad-\infty

determine \(\omega_{0}, R,\) and \(\delta\) so as to write the given expression in the form \(u=R \cos \left(\omega_{0} t-\delta\right)\) $$ u=3 \cos 2 t+4 \sin 2 t $$

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 \(\epsilon .\)

Assume that the system described by the equation \(m u^{\prime \prime}+\gamma u^{\prime}+k u=0\) is critically damped and the initial conditions are \(u(0)=u_{0}, u^{\prime}(0)=v_{0}\), If \(v_{0}=0,\) show that \(u \rightarrow 0\) as \(t \rightarrow \infty\) but that \(u\) is never zero. If \(u_{0}\) is positive, determine a condition on \(v_{0}\) that will assure that the mass passes through its equilibrium position after it is released.

See all solutions

Recommended explanations on Math 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