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find the solution of the given initial value problem. $$ y^{\prime}-y=2 t e^{2 t}, \quad y(0)=1 $$

Short Answer

Expert verified
Question: Given the differential equation \(y' - y = 2te^{2t}\) with initial condition \(y(0) = 1\), find the solution y(t). Answer: The solution to the initial value problem is \(y(t) = (2t-2)e^{2t} + 3e^{t}\).

Step by step solution

01

Rewrite as a first-order linear equation in standard form

We can notice that the given differential equation is already in standard form: $$ y^{\prime}-y=2 t e^{2 t} $$ Here, the function p(t) is -1, and the function g(t) is 2te^{2t}.
02

Determine the integrating factor

We'll now find the integrating factor \(μ(t)\) by calculating the exponential of the integral of p(t) with respect to t: $$ μ(t) = e^{\int -1 dt} = e^{-t} $$
03

Multiply by the integrating factor

Next, multiply both sides of the equation by the integrating factor, \(e^{-t}\): $$ e^{-t} (y^{\prime}-y)=2 t e^{t} $$
04

Integrate both sides with respect to t

Now, we'll find that the left side of the equation is the derivative of the product \(y(t)e^{-t}\). Let's integrate both sides with respect to t: $$ \int y(t) e^{-t} dt = \int 2 t e^{t} dt $$
05

Solve the integral on the right side

To solve the integral on the right side, we will use integration by parts: $$ \int 2 t e^{t} dt = (2t-2)e^{t} + C $$
06

Integrate left side and solve for y(t)

Now the equation looks like: $$ y(t) e^{-t} = (2t-2)e^{t} + C $$ Let's multiply both sides by \(e^{t}\) to solve for y(t): $$ y(t) = (2t-2)e^{2t} + Ce^{t} $$
07

Apply the initial condition and find C

Lastly, we'll apply the initial condition y(0) = 1 to find C: $$ 1 = (2(0)-2)e^{2(0)} + Ce^{(0)} $$ This simplifies to: $$ 1 = -2 + C $$ So, C = 3.
08

Write the final solution

Now, we have found the solution to the initial value problem: $$ y(t) = (2t-2)e^{2t} + 3e^{t} $$

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Most popular questions from this chapter

Show that the equations are not exact, but become exact when multiplied by the given integrating factor. Then solve the equations. $$ \left(\frac{\sin y}{y}-2 e^{-x} \sin x\right) d x+\left(\frac{\cos y+2 e^{-x} \cos x}{y}\right) d y=0, \quad \mu(x, y)=y e^{x} $$

Sometimes it is possible to solve a nonlinear equation by making a change of the dependent variable that converts it into a linear equation. The most important such equation has the form $$ y^{\prime}+p(t) y=q(t) y^{n} $$ and is called a Bernoulli equation after Jakob Bernoulli. deal with equations of this type. (a) Solve Bemoulli's equation when \(n=0\); when \(n=1\). (b) Show that if \(n \neq 0,1\), then the substitution \(v=y^{1-n}\) reduces Bernoulli's equation to a linear equation. This method of solution was found by Leibniz in 1696 .

let \(\phi_{0}(t)=0\) and use the method of successive approximations to approximate the solution of the given initial value problem. (a) Calculate \(\phi_{1}(t), \ldots, \phi_{3}(t)\) (b) \(\mathrm{Plot} \phi_{1}(t), \ldots, \phi_{3}(t)\) and observe whether the iterates appear to be converging. $$ y^{\prime}=1-y^{3}, \quad y(0)=0 $$

Determine whether or not each of the equations is exact. If it is exact, find the solution. $$ \left(2 x y^{2}+2 y\right)+\left(2 x^{2} y+2 x\right) y^{\prime}=0 $$

A body of constant mass \(m\) is projected vertically upward with an initial velocity \(v_{0}\) in a medium offering a resistance \(k|v|,\) where \(k\) is a constant. Neglect changes in the gravitational force. $$ \begin{array}{l}{\text { (a) Find the maximum height } x_{m} \text { attained by the body and the time } t_{m} \text { at which this }} \\ {\text { maximum height is reached. }} \\ {\text { (b) Show that if } k v_{0} / m g<1, \text { then } t_{m} \text { and } x_{m} \text { can be expressed as }}\end{array} $$ $$ \begin{array}{l}{t_{m}=\frac{v_{0}}{g}\left[1-\frac{1}{2} \frac{k v_{0}}{m g}+\frac{1}{3}\left(\frac{k v_{0}}{m g}\right)^{2}-\cdots\right]} \\\ {x_{m}=\frac{v_{0}^{2}}{2 g}\left[1-\frac{2}{3} \frac{k r_{0}}{m g}+\frac{1}{2}\left(\frac{k v_{0}}{m g}\right)^{2}-\cdots\right]}\end{array} $$ $$ \text { (c) Show that the quantity } k v_{0} / m g \text { is dimensionless. } $$

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