Chapter 2: Problem 28
Find the value of \(y_{0}\) for which the solution of the initial value problem $$ y^{\prime}-y=1+3 \sin t, \quad y(0)=y_{0} $$ remains finite as \(t \rightarrow \infty\).
Short Answer
Expert verified
Answer: The value of \(y_0\) is \(-4\).
Step by step solution
01
Solve the differential equation using integrating factor
First, rewrite the given differential equation:
$$
y^{\prime}-y=1+3 \sin t
$$
This is a first-order linear ordinary differential equation in the form of:
$$
y^{\prime} + P(t)y = Q(t)
$$
Here, we have \(P(t)=-1\) and \(Q(t)=1+3\sin t\). Now, we will find the integrating factor (IF) which is given by \(e^{\int P(t) \, dt}\).
Calculate the integrating factor:
$$
IF = e^{\int -1 dt} = e^{-t}
$$
Now, multiply both sides of the differential equation with the integrating factor:
$$
e^{-t}y^{\prime} - e^{-t}y = e^{-t}(1+3\sin t)
$$
Now, observe that the left-hand side of the equation is the derivative of the product \(y(t)e^{-t}\):
$$
\frac{d}{dt}(y(t)e^{-t}) = e^{-t}(1+3\sin t)
$$
Now, we integrate both sides with respect to t:
$$
\int \frac{d}{dt}(y(t)e^{-t}) dt = \int e^{-t}(1+3\sin t) dt
$$
02
Find the function \(y(t)\) and its limit as \(t \rightarrow \infty\)
Using integration by parts (twice) on the right-hand side of the equation and remembering that the integral of the derivative of a function is the function itself, we have:
$$
y(t)e^{-t} = -e^{-t} - 3e^{-t}\cos t + C
$$
To find the general solution, multiply both sides by \(e^t\) to clear out the exponential term:
$$
y(t) = -1 - 3\cos t + Ce^t
$$
The problem asks for the solution to remain finite as \(t \rightarrow \infty\). To satisfy this condition, we need \(Ce^t\) to go to zero as \(t \rightarrow \infty\). Therefore, we must have \(C=0\). Thus, we get the specific solution:
$$
y(t) = -1 - 3\cos t
$$
03
Use the initial condition to find the value of \(y_0\)
Use the initial condition \(y(0) = y_0\):
$$
y_0 = -1 - 3\cos (0)
$$
Since \(\cos (0) = 1\), we get:
$$
y_0 = -1 - 3 \cdot 1 = -4
$$
So the value of \(y_0\) for which the solution remains finite as \(t \rightarrow \infty\) is \(y_0 = -4\).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
First-Order Linear Ordinary Differential Equation
First-order linear ordinary differential equations are a specific type of differential equation. They have the general form:
- \( y' + P(t)y = Q(t) \)
- \( y' \) is the derivative of \( y \) with respect to \( t \).
- \( P(t) \) and \( Q(t) \) are given functions of \( t \). They can be constant or vary with \( t \).
- \( y' - y = 1 + 3 \sin t \)
Integrating Factor
The integrating factor is a key tool in solving first-order linear differential equations. Think of it as a magic multiplier that helps simplify the equation. To find it, use the formula:
- \( IF = e^{\int P(t) \ dt} \)
- \( IF = e^{-t} \)
- \( \frac{d}{dt}(y(t)e^{-t}) = e^{-t}(1+3\sin t) \)
Integration by Parts
Integration by parts is a technique used when integrating the product of two functions. In this exercise, we employed integration by parts twice. This was necessary because the expression \( e^{-t} (1+3\sin t) \) required it for a complete solution. The integration by parts formula is:
- \( \int u \, dv = uv - \int v \, du \)
- First integration yields a simpler form after applying the formula.
- The second round of integration by parts further simplifies the expression.
- \( y(t)e^{-t} = -e^{-t} - 3e^{-t} \cos t + C \)
Bounded Solutions
When looking at differential equations, especially initial value problems, one important aspect is whether solutions remain bounded. A bounded solution is one that does not go to infinity as time \( t \) approaches infinity.
This ensures predictability and stability of the solution over time.In our problem, when \( y(t) = -1 - 3\cos t + Ce^t \), for the solution to be bounded, \( Ce^t \) must approach zero as \( t \to \infty \).
This shows how elements such as initial conditions affect the nature of solutions.
This ensures predictability and stability of the solution over time.In our problem, when \( y(t) = -1 - 3\cos t + Ce^t \), for the solution to be bounded, \( Ce^t \) must approach zero as \( t \to \infty \).
- Therefore, \( C \) must be zero.
- If \( C eq 0 \), \( Ce^t \) becomes unbounded because \( e^t \) grows exponentially.
This shows how elements such as initial conditions affect the nature of solutions.