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

If the Wronskian \(W\) of \(f\) and \(g\) is \(3 e^{4 t}\), and if \(f(t)=e^{2 t},\) find \(g(t)\)

Short Answer

Expert verified
Question: Determine the function g(t) given that the Wronskian W of the functions f(t) and g(t) is 3e^(4t) and the function f(t) is e^(2t). Answer: g(t) = 3te^(2t) + Ce^(2t), where C is an arbitrary constant.

Step by step solution

01

Write down the given information

We are given the following: - Wronskian, \(W = 3e^{4t}\) - Function \(f(t) = e^{2t}\) Our task is to find the function \(g(t)\).
02

Compute the derivative of \(f(t)\)

In order to use the Wronskian formula, we need to find the derivative of \(f(t)\). Differentiating \(f(t) = e^{2t}\) with respect to \(t\), we get: \(f'(t) = 2e^{2t}\)
03

Write down the Wronskian formula and substitute the given information

We know that the Wronskian is given by the formula: \(W(f,g) = fg' - f'g\) Substitute the given information into the formula: \(3e^{4t} = (e^{2t})(g'(t)) - (2e^{2t})(g(t))\)
04

Solve the differential equation for \(g(t)\)

Now, we need to solve the differential equation for \(g(t)\). This is a first-order linear inhomogeneous differential equation. Let's first divide through by \(e^{2t}\): \(\frac{3e^{4t}}{e^{2t}}=g'(t)-2g(t)\) Simplify the equation: \(3e^{2t}=g'(t)-2g(t)\) Let's write it in the form of a first-order linear differential equation: \(g'(t) - 2g(t) = 3e^{2t}\)
05

Use the integrating factor method to solve the differential equation

We can solve this differential equation using the integrating factor method. First, we calculate the integrating factor (\(IF\)): \(IF = e^{\int -2dt} = e^{-2t}\) Now, multiply both sides of the differential equation by the integrating factor: \(e^{-2t}g'(t) - 2e^{-2t}g(t) = 3e^{2t}e^{-2t}\) This simplifies to: \((e^{-2t}g(t))' = 3\) Now, integrate both sides with respect to \(t\): \(\int(e^{-2t}g(t))' dt = \int 3 dt\) This gives: \(e^{-2t}g(t) = 3t + C\) Now, multiply both sides by the integrating factor's inverse, which is \(e^{2t}\): \(g(t) = 3te^{2t} + Ce^{2t}\) Here, \(g(t)\) is the function we were looking for, and \(C\) is an arbitrary constant.

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!

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 spring-mass system with a hardening spring (Problem 32 of Section 3.8 ) is acted on by a periodic external force. In the absence of damping, suppose that the displacement of the mass satisfies the initial value problem $$ u^{\prime \prime}+u+\frac{1}{5} u^{3}=\cos \omega t, \quad u(0)=0, \quad u^{\prime}(0)=0 $$ (a) Let \(\omega=1\) and plot a computer-generated solution of the given problem. Does the system exhibit a beat? (b) Plot the solution for several values of \(\omega\) between \(1 / 2\) and \(2 .\) Describe how the solution changes as \(\omega\) increases.

Show that \(A \cos \omega_{0} t+B \sin \omega_{0} t\) can be written in the form \(r \sin \left(\omega_{0} t-\theta\right) .\) Determine \(r\) and \(\theta\) in terms of \(A\) and \(B\). If \(R \cos \left(\omega_{0} t-\delta\right)=r \sin \left(\omega_{0} t-\theta\right),\) determine the relationship among \(R, r, \delta,\) and \(\theta .\)

Verify that the given functions \(y_{1}\) and \(y_{2}\) satisfy the corresponding homogeneous equation; then find a particular solution of the given nonhomogeneous equation. In Problems 19 and \(20 g\) is an arbitrary continuous function. $$ (1-t) y^{\prime \prime}+t y^{\prime}-y=2(t-1)^{2} e^{-t}, \quad 0

A spring is stretched \(10 \mathrm{cm}\) by a force of 3 newtons. A mass of \(2 \mathrm{kg}\) is hung from the spring and is also attached to a viscous damper that exerts a force of 3 newtons when the velocity of the mass is \(5 \mathrm{m} / \mathrm{sec}\). If the mass is pulled down \(5 \mathrm{cm}\) below its equilibrium position and given an initial downward velocity of \(10 \mathrm{cm} / \mathrm{sec},\) determine its position \(u\) at any time \(t\) Find the quasi frequency \(\mu\) and the ratio of \(\mu\) to the natural frequency of the corresponding undamped motion.

(a) Determine a suitable form for \(Y(t)\) if the method of undetermined coefficients is to be used. (b) Use a computer algebra system to find a particular solution of the given equation. $$ y^{\prime \prime}+3 y^{\prime}+2 y=e^{f}\left(t^{2}+1\right) \sin 2 t+3 e^{-t} \cos t+4 e^{t} $$

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