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

Short Answer

Expert verified
Answer: The solution for the given IVP is $y(x) = e^{2x}(x + 2)$.

Step by step solution

01

Identify the given differential equation and initial condition

The given differential equation is $$ y'(x)-2y(x)=e^{2x} $$ and the initial condition is $$ y(0) = 2 $$
02

Calculate the integrating factor

In our case, the function associated with y(x) is -2. Let's call this function p(x): $$ p(x) = -2 $$ Now, the integrating factor (IF) is given by the exponential of the integral of p(x) tensorwith respect to x: $$ \text{IF} = e^{\int p(x) \, dx} $$ Plugging the value of p(x) and simplify: $$ \text{IF} = e^{\int -2 \, dx} = e^{-2x}\ $$
03

Multiply the differential equation by the integrating factor

Now, multiply the given differential equation by the computed integrating factor: $$ e^{-2x} (y'(x) - 2y(x)) = e^{-2x} e^{2x} $$ which becomes: $$ (e^{-2x}y(x))' = 1 $$
04

Integrate both sides of the equation

Now, we integrate both sides of the equation with respect to x: $$ \int (e^{-2x}y(x))' \, dx = \int 1 \, dx $$ This results in $$ e^{-2x}y(x) = x + C $$
05

Rearrange the equation to find the general solution

Now, rearrange the equation above to find y(x): $$ y(x) = e^{2x}(x + C) $$ Now we have the general solution.
06

Apply the initial condition to find the particular solution

Using the initial condition y(0) = 2, we can find the particular solution: $$ 2 = e^{2\cdot0}(0 + C) $$ which gives us $$ C = 2 $$
07

Write down the final solution

Finally, plug the value of C back into the general solution to find the particular solution: $$ y(x) = e^{2x}(x + 2) $$ That is the solution of the given initial value problem.

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Most popular questions from this chapter

Show that if \(y=\phi(t)\) is a solution of \(y^{\prime}+p(t) y=0,\) then \(y=c \phi(t)\) is also a solution for any value of the constant \(c .\)

Involve equations of the form \(d y / d t=f(y) .\) In each problem sketch the graph of \(f(y)\) versus \(y\), determine the critical (equilibrium) points, and classify each one as asymptotically stable, unstable, or semistable (see Problem 7 ). $$ d y / d t=y^{2}(1-y)^{2}, \quad-\infty

draw a direction field and plot (or sketch) several solutions of the given differential equation. Describe how solutions appear to behave as \(t\) increases, and how their behavior depends on the initial value \(y_{0}\) when \(t=0\). $$ y^{\prime}=t-1-y^{2} $$

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 .

Involve equations of the form \(d y / d t=f(y) .\) In each problem sketch the graph of \(f(y)\) versus \(y\), determine the critical (equilibrium) points, and classify each one as asymptotically stable, unstable, or semistable (see Problem 7 ). $$ d y / d t=y^{2}\left(4-y^{2}\right), \quad-\infty

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