Chapter 10: Problem 23
Solve the following differential equations with the given initial conditions. $$ 3 y^{2} y^{\prime}=-\sin t, y\left(\frac{\pi}{2}\right)=1 $$
Short Answer
Expert verified
The solution is \(y = \frac{1}{1 - 3 \text{cos}(t)}\).
Step by step solution
01
- Write the differential equation
Given the differential equation: \[3 y^{2} y^{\text{prime}}=-\text{sin}(t), \, y\left(\frac{\pi}{2}\right)=1\]We need to solve this for the function \(y(t)\).
02
- Separate the variables
Design the equation to separate variables: \[3 y^{2} \frac{dy}{dt}=-\text{sin}(t)\]Now divide both sides by \(3 y^{2}\) and multiply by \(dt\): \[\frac{1}{3 y^{2}} dy = -\text{sin}(t) dt\]
03
- Integrate both sides
Integrate both sides with respect to their variables: \[\int \frac{1}{3 y^{2}} dy = \int -\text{sin}(t) dt\]For the left side: \[\int \frac{1}{3 y^{2}} dy = \int \frac{1}{3} y^{-2} dy = \frac{1}{3} \left( \frac{-1}{y} \right) = -\frac{1}{3y}\]For the right side: \[\int -\text{sin}(t) dt = \text{cos}(t) + C\]
04
- Solve for C using the initial condition
Apply the initial condition to solve for the constant C: \[y\left(\frac{\pi}{2}\right) = 1\]Substitute \(t = \frac{\pi}{2}\) and \(y = 1\) into the integrated result: \[-\frac{1}{3 \cdot 1} = \text{cos}\left(\frac{\pi}{2}\right) + C\]This simplifies to: \[-\frac{1}{3} = 0 + C\]Hence, \(C = -\frac{1}{3}\)
05
- Write the general solution
The general solution, including the constant found, is: \[-\frac{1}{3y} = \text{cos}(t) - \frac{1}{3}\]Solving for \(y\): \[-\frac{1}{3y} + \frac{1}{3} = \text{cos}(t)\]Multiply through by 3y to isolate y: \[ -1 + y = 3y \cdot \text{cos}(t) \]Thus, the solution simplifies to: \[ y(1 - 3 \text{cos}(t)) = 1 \]Solving for y completely: \[ y = \frac{1}{1 - 3 \text{cos}(t)} \]
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Variable Separation
The method of variable separation is a foundational technique in solving differential equations. It involves rearranging the differential equation so that each variable appears on a different side of the equation. This method enables us to integrate each side with respect to its own variable. In our example, the equation starts as: \[3 y^{2} \frac{dy}{dt}=-\text{sin}(t)\]To achieve separation, we multiply both sides by \(dt\) and divide by \(3 y^{2}\). This results in:\[\frac{1}{3 y^{2}} dy = -\text{sin}(t) dt\]Here, we successfully separated variables: \(y\) terms on the left, \(t\) terms on the right. This separation allows for the next step: integration of each side separately. Ensuring variables are correctly separated is crucial for the solving process to work.
Initial Conditions
Initial conditions are given values that a solution must satisfy, often used to determine unknown constants after integration. In our example, the initial condition is:\[ y\left(\frac{\pi}{2}\right)=1 \]This means when \(t = \frac{\pi}{2}\), \(y = 1\). Once we separate the variables and integrate both sides, we get:\[-\frac{1}{3y} = \text{cos}(t) + C \]Using the initial condition, substitute \(t = \frac{\pi}{2}\) and \(y = 1\):\[ -\frac{1}{3 \cdot 1} = \text{cos}\left(\frac{\pi}{2}\right) + C \]Since \(\text{cos}\left(\frac{\pi}{2}\right) = 0\), we simplify:\[ -\frac{1}{3} = 0 + C \]Thus, \(C = -\frac{1}{3}\). Initial conditions personalize the general solution to fit specific scenarios, making them essential in differential equations.
Integration
Integration is the mathematical process of finding the integral of a function, often reversing differentiation. In our context, integrating both sides of a separated differential equation provides the antiderivatives essential to solving the equation. From our separated variables:\[\int \frac{1}{3 y^{2}} dy = \int -\text{sin}(t) dt\]These integrals are computed as follows:For the left side:\[\int \frac{1}{3 y^{2}} dy = \int \frac{1}{3} y^{-2} dy = \frac{1}{3} \, \left( \frac{-1}{y} \right) = -\frac{1}{3y}\]For the right side:\[\int -\text{sin}(t) dt = \text{cos}(t) + C\]Combining these results, we obtain:\[-\frac{1}{3y} = \text{cos}(t) + C\]This step-by-step integration crucially leads us from a differential equation to an equation we can solve for the unknown function \(y(t)\). When tackling differential equations, precise integration and careful manipulation of constants are key to finding accurate solutions.