Chapter 4: Problem 10
\(y^{\prime}-y / t=-t \sin t\), with \(y(\pi)=-\pi\), on \([0,2 \pi]\).
Short Answer
Expert verified
The solution is \( y = t \cos t \).
Step by step solution
01
Identify Equation Type
Notice that the given equation is a first-order linear differential equation of the form \( y' + P(t) y = Q(t) \). Here, \( P(t) = -1/t \) and \( Q(t) = -t \sin t \).
02
Determine Integrating Factor
The integrating factor \( \mu(t) \) is given by \( e^{\int P(t) \, dt} \). So, we compute \( \int -1/t \, dt = -\ln |t| \), and therefore, \( \mu(t) = e^{-\ln |t|} = \frac{1}{t} \).
03
Multiply Equation by Integrating Factor
Multiply the entire differential equation by the integrating factor \(\frac{1}{t}\) to obtain \( \frac{1}{t}y' - \frac{y}{t^2} = -\sin t \).
04
Rewrite as Total Derivative
Recognize that the left side of the equation can be expressed as a derivative: \( \frac{d}{dt}\left(\frac{y}{t}\right) = -\sin t \).
05
Integrate Both Sides
Integrate both sides with respect to \( t \): \( \int \frac{d}{dt}\left(\frac{y}{t}\right) \, dt = \int -\sin t \, dt \). This gives \( \frac{y}{t} = \cos t + C \), where \( C \) is the constant of integration.
06
Solve for y(t)
Solve the equation \( \frac{y}{t} = \cos t + C \) for \( y \), giving \( y = t(\cos t + C) \).
07
Apply Initial Condition
Use the initial condition \( y(\pi) = -\pi \) to find \( C \). Substitute \( t = \pi \) and \( y = -\pi \) into \( y = t(\cos t + C) \): \(-\pi = \pi (\cos \pi + C) \). Knowing \( \cos \pi = -1 \), we have \(-\pi = \pi(-1 + C) \). Solve for \( C \): \(-\pi = -\pi + \pi C \), so \( \pi C = 0 \) which implies \( C = 0 \).
08
Write Final Solution
Substituting \( C = 0 \) into \( y = t(\cos t + C) \), the solution is \( y = t \cos t \).
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
First-Order Linear Differential Equation
Differential equations describe various phenomena such as physics, biology, and finance. A significant category of these is the first-order linear differential equation. This type of equation appears in the form \( y' + P(t) y = Q(t) \).
In the given example, we identify the equation \( y' - \frac{y}{t} = -t \sin t \) as a first-order linear differential equation with \( P(t) = -\frac{1}{t} \) and \( Q(t) = -t \sin t \).
Recognizing the terms \( P(t) \) and \( Q(t) \) is crucial for applying the method of integrating factors to find solutions.
In the given example, we identify the equation \( y' - \frac{y}{t} = -t \sin t \) as a first-order linear differential equation with \( P(t) = -\frac{1}{t} \) and \( Q(t) = -t \sin t \).
Recognizing the terms \( P(t) \) and \( Q(t) \) is crucial for applying the method of integrating factors to find solutions.
Integrating Factor
To solve a first-order linear differential equation, we often utilize an integrating factor. The purpose of this factor is to transform the differential equation into a form that is easier to integrate.
The integrating factor is denoted as \( \mu(t) \), given by the formula \( e^{\int P(t) \, dt} \). In our example, we compute \( \int -\frac{1}{t} \, dt = -\ln |t| \). This results in the integrating factor \( \mu(t) = e^{-\ln |t|} = \frac{1}{t} \).
Multiplying the differential equation by this integrating factor helps us to reformulate the equation into a total derivative, facilitating straightforward integration.
The integrating factor is denoted as \( \mu(t) \), given by the formula \( e^{\int P(t) \, dt} \). In our example, we compute \( \int -\frac{1}{t} \, dt = -\ln |t| \). This results in the integrating factor \( \mu(t) = e^{-\ln |t|} = \frac{1}{t} \).
Multiplying the differential equation by this integrating factor helps us to reformulate the equation into a total derivative, facilitating straightforward integration.
Initial Condition
An initial condition provides specific data to uniquely determine the solution of a differential equation from a family of possible solutions.
In our case, we have the initial condition \( y(\pi) = -\pi \). This means that when \( t = \pi \), the value of \( y(t) \) is \(-\pi\).
Initial conditions are essential because they allow us to compute the constant of integration, completing our solution. Here, we found that substituting \( t = \pi \) and \( y = -\pi \) in the solution equation provides us with \( C = 0 \).
Thus, applying the initial condition gives the particular solution applicable to the specific scenario described in the problem.
In our case, we have the initial condition \( y(\pi) = -\pi \). This means that when \( t = \pi \), the value of \( y(t) \) is \(-\pi\).
Initial conditions are essential because they allow us to compute the constant of integration, completing our solution. Here, we found that substituting \( t = \pi \) and \( y = -\pi \) in the solution equation provides us with \( C = 0 \).
Thus, applying the initial condition gives the particular solution applicable to the specific scenario described in the problem.
Solution to Differential Equation
Finding the solution to a differential equation involves several steps: identifying the type of equation, using an integrating factor, and applying initial conditions.
The original problem yields the differential equation \( \frac{y}{t} = \cos t + C \). Solving for \( y \) gives \( y = t(\cos t + C) \).
By using the initial condition \( y(\pi) = -\pi \), we calculated the constant \( C \) as 0.
This allows us to determine the final solution, which is \( y = t \cos t \). This solution represents the full behavior of \( y \) in the interval \([0, 2\pi]\) as described by the problem, providing an equation that respects all given conditions.
The original problem yields the differential equation \( \frac{y}{t} = \cos t + C \). Solving for \( y \) gives \( y = t(\cos t + C) \).
By using the initial condition \( y(\pi) = -\pi \), we calculated the constant \( C \) as 0.
This allows us to determine the final solution, which is \( y = t \cos t \). This solution represents the full behavior of \( y \) in the interval \([0, 2\pi]\) as described by the problem, providing an equation that respects all given conditions.