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Find a formula involving integrals for a particular solution of the differential equation $$ y^{\prime \prime \prime}-3 y^{\prime \prime}+3 y^{\prime}-y=g(t) $$ If \(g(t)=t^{-2} e^{t},\) determine \(Y(t)\)

Short Answer

Expert verified
The purpose of using the convolution theorem in this exercise is to rewrite the Laplace transform of the product of two functions as the integral of products of their inverse Laplace transforms, which facilitates finding the particular solution Y(t) for the given differential equation.

Step by step solution

01

Rewrite the given differential equation

We are given the differential equation: $$ y^{\prime \prime \prime}-3 y^{\prime \prime}+3 y^{\prime}-y=g(t) $$ where \(g(t)=t^{-2} e^{t}\)
02

Take Laplace transform of the equation

Taking the Laplace transform on both sides of the equation, we get: $$ \Lap[ y^{\prime \prime \prime}] - 3\Lap[y^{\prime \prime}] + 3\Lap[y^{\prime}] - \Lap[y] = \Lap[g(t)] $$ Using the Laplace transform properties, we can rewrite the equation as: $$ s^3Y(s) - 3 s^2 Y(s) + 3s Y(s) - Y(s) = \lap[ t^{-2} e^{t}] $$
03

Find the Laplace transform of a particular solution using convolution theorem

Using the convolution theorem, we can rewrite the equation as: $$ ( s^3 - 3 s^2 + 3s - 1) Y(s) = \frac{ e^s \Gamma(0,s) } {s^2} $$ Now, we need to find the inverse Laplace transform to get \(Y(t)\): $$ y(t) = L^{-1}\left( \frac{ e^s \Gamma(0,s) } {s^2(s^3 - 3 s^2 + 3s - 1)}\right) $$
04

Use convolution theorem and inverse Laplace transforms to determine \(Y(t)\)

Using convolution theorem, we have: $$ y(t) = \int_0^t L^{-1}\left( \frac{ e^s \Gamma(0,s) } {s^2} \right) L^{-1}(s^3 - 3 s^2 + 3 s - 1)ds $$ For convenience, let \(u(s) = L^{-1}\left( \frac{ e^s \Gamma(0,s) } {s^2} \right)\) and \(v(s) = L^{-1}(s^3 - 3 s^2 + 3 s - 1)\). Then: $$ y(t) = \int_0^t u(s) \cdot v(t-s) ds $$ Now, we need to find the inverse Laplace transforms of \(u(s)\) and \(v(s)\) and then calculate the integral. Note that we may need to use partial fraction decomposition or other Laplace transform properties and techniques to find the inverse Laplace transforms. After finding the inverse Laplace transforms and calculating the integral, we will have our particular solution \(Y(t)\).

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Most popular questions from this chapter

Find the general solution of the given differential equation. $$ y^{\mathrm{vi}}-y^{\prime \prime}=0 $$

Use Abel’s formula (Problem 20) to find the Wronskian of a fundamental set of solutions of the given differential equation. $$ t^{2} y^{\mathrm{iv}}+t y^{\prime \prime \prime}+y^{\prime \prime}-4 y=0 $$

We consider another way of arriving at the proper form of \(Y(t)\) for use in the method of undetermined coefficients. The procedure is based on the observation that exponential, polynomial, or sinusoidal terms (or sums and products of such terms) can be viewed as solutions of certain linear homogeneous differential equations with constant coefficients. It is convenient to use the symbol \(D\) for \(d / d t\). Then, for example, \(e^{-t}\) is a solution of \((D+1) y=0 ;\) the differential operator \(D+1\) is said to annihilate, or to be an annihilator of, \(e^{-t}\). Similarly, \(D^{2}+4\) is an annihilator of \(\sin 2 t\) or \(\cos 2 t,\) \((D-3)^{2}=D^{2}-6 D+9\) is an annihilator of \(e^{3 t}\) or \(t e^{3 t},\) and so forth. Show that linear differential operators with constant coefficients obey the commutative law, that is, $$ (D-a)(D-b) f=(D-b)(D-a) f $$ for any twice differentiable function \(f\) and any constants \(a\) and \(b .\) The result extends at once to any finite number of factors.

Consider the spring-mass system, shown in Figure \(4.2 .4,\) consisting of two unit masses suspended from springs with spring constants 3 and \(2,\) respectively. Assume that there is no damping in the system. (a) Show that the displacements \(u_{1}\) and \(u_{2}\) of the masses from their respective equilibrium positions satisfy the equations $$ u_{1}^{\prime \prime}+5 u_{1}=2 u_{2}, \quad u_{2}^{\prime \prime}+2 u_{2}=2 u_{1} $$ (b) Solve the first of Eqs. (i) for \(u_{2}\) and substitute into the second equation, thereby obtaining the following fourth order equation for \(u_{1}:\) $$ u_{1}^{\mathrm{iv}}+7 u_{1}^{\prime \prime}+6 u_{1}=0 $$ Find the general solution of Eq. (ii). (c) Suppose that the initial conditions are $$ u_{1}(0)=1, \quad u_{1}^{\prime}(0)=0, \quad u_{2}(0)=2, \quad u_{2}^{\prime}(0)=0 $$ Use the first of Eqs. (i) and the initial conditions (iii) to obtain values for \(u_{1}^{\prime \prime}(0)\) and \(u_{1}^{\prime \prime \prime}(0)\) Then show that the solution of Eq. (ii) that satisfies the four initial conditions on \(u_{1}\) is \(u_{1}(t)=\cos t .\) Show that the corresponding solution \(u_{2}\) is \(u_{2}(t)=2 \cos t .\) (d) Now suppose that the initial conditions are $$ u_{1}(0)=-2, \quad u_{1}^{\prime}(0)=0, \quad u_{2}(0)=1, \quad u_{2}^{\prime}(0)=0 $$ Proceed as in part (c) to show that the corresponding solutions are \(u_{1}(t)=-2 \cos \sqrt{6} t\) and \(u_{2}(t)=\cos \sqrt{6} t\) (e) Observe that the solutions obtained in parts (c) and (d) describe two distinct modes of vibration. In the first, the frequency of the motion is \(1,\) and the two masses move in phase, both moving up or down together. The second motion has frequency \(\sqrt{6}\), and the masses move out of phase with each other, one moving down while the other is moving up and vice versa. For other initial conditions, the motion of the masses is a combination of these two modes.

Find the general solution of the given differential equation. Leave your answer in terms of one or more integrals. $$ y^{\prime \prime \prime}-y^{\prime \prime}+y^{\prime}-y=\sec t, \quad-\pi / 2

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