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Equations with the Dependent Variable Missing. For a scond order differential equation of the form \(y^{\prime \prime}=f\left(t, y^{\prime}\right),\) the substitution \(v=y^{\prime}, v^{\prime}=y^{\prime \prime}\) leads to a first order equation of the form \(v^{\prime}=f(t, v)\). If this equation can be solved for \(v\), then \(y\) can be obtained by integrating \(d y / d t=v .\) Note that one arbitrary constant is obtained in solving the first order equation for \(v,\) and a second is introduced in the integration for \(y\). In each of Problems 28 through 33 use this substitution to solve the given equation. $$ t^{2} y^{\prime \prime}+2 t y^{\prime}-1=0, \quad t>0 $$

Short Answer

Expert verified
Answer: The general solution of the given second-order differential equation is \(y(t) = \ln{t} - \frac{1}{3}t^3 + C_1t + C_2\), where \(C_1\) and \(C_2\) are constants of integration.

Step by step solution

01

Perform the substitution

Substitute \(v=y'\) and \(v'=y''\) into the given equation. $$ t^{2}v'+2tv-1=0 $$
02

Solve for \(v'\)

Isolate \(v'\) in the equation: $$ v' = \frac{1-2tv}{t^2} $$
03

Integrate the equation to find \(v\)

Integrate the equation for \(v'\) with respect to \(t\): $$ v(t) = \int \frac{1-2tv}{t^2} dt $$ Using the power rule for integration, we find: $$ v(t) = \int \frac{1}{t^2} dt - 2\int t dt = -\frac{1}{t} - t^2 + C_1 $$ where \(C_1\) is the constant of integration.
04

Substitute back for \(y'\)

Now that we have found \(v(t)\), substitute back \(y'\) for \(v\). Recall that \(v=y'\): $$ y' = -\frac{1}{t} - t^2 + C_1 $$
05

Integrate to find \(y\)

Integrate the equation for \(y'\) with respect to \(t\) to find \(y(t)\): $$ y(t) = \int (-\frac{1}{t} - t^2 + C_1) dt $$ Using the power rule and factoring out the constant, we find: $$ y(t) = \ln{t} - \frac{1}{3}t^3 + C_1t + C_2 $$ where \(C_2\) is another constant of integration. So, the solution to the given second-order differential equation is: $$ y(t) = \ln{t} - \frac{1}{3}t^3 + C_1t + C_2 $$

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Most popular questions from this chapter

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. $$ x^{2} y^{\prime \prime}-3 x y^{\prime}+4 y=x^{2} \ln x, \quad x>0 ; \quad y_{1}(x)=x^{2}, \quad y_{2}(x)=x^{2} \ln x $$

A spring-mass system has a spring constant of \(3 \mathrm{N} / \mathrm{m}\). A mass of \(2 \mathrm{kg}\) is attached to the spring and the motion takes place in a viscous fluid that offers a resistance numerically equal to the magnitude of the instantaneous velocity. If the system is driven by an external force of \(3 \cos 3 t-2 \sin 3 t \mathrm{N},\) determine the steady-state response. Express your answer in the form \(R \cos (\omega t-\delta)\)

Show that the solution of the initial value problem $$ L[y]=y^{\prime \prime}+p(t) y^{\prime}+q(t) y=g(t), \quad y\left(t_{0}\right)=y_{0}, \quad y^{\prime}\left(t_{0}\right)=y_{0}^{\prime} $$ can be written as \(y=u(t)+v(t)+v(t),\) where \(u\) and \(v\) are solutions of the two initial value problems $$ \begin{aligned} L[u] &=0, & u\left(t_{0}\right)=y_{0}, & u^{\prime}\left(t_{0}\right)=y_{0}^{\prime} \\ L[v] &=g(t), & v\left(t_{0}\right)=0, & v^{\prime}\left(t_{0}\right) &=0 \end{aligned} $$ respectively. In other words, the nonhomogeneities in the differential equation and in the initial conditions can be dealt with separately. Observe that \(u\) is easy to find if a fundamental set of solutions of \(L[u]=0\) is known.

Consider the vibrating system described by the initial value problem $$ u^{\prime \prime}+u=3 \cos \omega t, \quad u(0)=1, \quad u^{\prime}(0)=1 $$ (a) Find the solution for \(\omega \neq 1\). (b) Plot the solution \(u(t)\) versus \(t\) for \(\omega=0.7, \omega=0.8,\) and \(\omega=0.9 .\) Compare the results with those of Problem \(18,\) that is, describe the effect of the nonzero initial conditions.

Use the substitution introduced in Problem 38 in Section 3.4 to solve each of the equations \(t^{2} y^{\prime \prime}-3 t y^{\prime}+4 y=0, \quad t>0\)

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