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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. $$ y^{\prime \prime}+y^{\prime}=e^{-t} $$

Short Answer

Expert verified
To solve the given second-order differential equation, we first transformed it into a first-order differential equation by substituting v for y' and v' for y''. We then solved the first-order differential equation to find v and integrated v with respect to t to find y. The final solution is: $$ y(t) = -(t+C_1)e^{-t} - e^{-t} + C_2 $$ where \(C_1\) and \(C_2\) are arbitrary constants.

Step by step solution

01

Substituting v and v' for y' and y'' respectively

Given the second order differential equation: $$ y^{\prime\prime} + y^{\prime} = e^{-t} $$ Let's make the substitution \(v = y^{\prime}\), and \(v^{\prime} = y^{\prime\prime}\). The given equation becomes: $$ v^{\prime} + v = e^{-t} $$ Now we have a first-order differential equation in terms of \(v\) and \(t\).
02

Solve the first-order differential equation for v

The first-order differential equation in terms of \(v\) and \(t\) is: $$ v^{\prime} + v = e^{-t} $$ This is a first-order linear differential equation. To solve it, we need to find an integrating factor. The integrating factor \(I(t)\) for this equation is given by: $$ I(t) = \exp\left(\int 1 \, dt \right) = e^{t} $$ Now, multiply the equation by the integrating factor: $$ e^t v^{\prime} + e^t v = e^{-t} e^t $$ $$ \frac{d}{dt}\left(e^t v\right) = 1 $$ Now, integrate both sides with respect to t: $$ \int\frac{d}{dt}\left( e^t v\right) dt = \int 1 dt $$ $$ e^t v = t + C_1 $$ Now, isolate \(v\): $$ v = e^{-t}(t + C_1) $$
03

Integrate v to find y

Recall that \(v = y^{\prime}\). So now we need to integrate \(v\) with respect to \(t\) to find \(y\): $$ y^{\prime} = e^{-t}(t + C_1) $$ $$ y(t) = \int e^{-t}(t + C_1) dt $$ To integrate this expression, we can use integration by parts, let: $$ u = t + C_1,\ dv = e^{-t} dt \\ du = dt,\ v = -e^{-t} $$ Applying integration by parts formula (\(\int u dv = uv - \int v du\)), we get $$ y(t) = -(t+C_1)e^{-t} + \int e^{-t} dt $$ $$ y(t) = -(t+C_1)e^{-t} - e^{-t} + C_2 $$ Therefore, the solution to the original second-order differential equation is: $$ y(t) = -(t+C_1)e^{-t} - e^{-t} + C_2 $$ where \(C_1\) and \(C_2\) are arbitrary constants.

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Most popular questions from this chapter

In the absence of damping the motion of a spring-mass system satisfies the initial value problem $$ m u^{\prime \prime}+k u=0, \quad u(0)=a, \quad u^{\prime}(0)=b $$ (a) Show that the kinetic energy initially imparted to the mass is \(m b^{2} / 2\) and that the potential energy initially stored in the spring is \(k a^{2} / 2,\) so that initially the total energy in the system is \(\left(k a^{2}+m b^{2}\right) / 2\). (b) Solve the given initial value problem. (c) Using the solution in part (b), determine the total energy in the system at any time \(t .\) Your result should confirm the principle of conservation of energy for this system.

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