Chapter 3: Problem 10
First find the general solution (involving a constant \(C\) ) for the given differential equation. Then find the particular solution that satisfies the indicated condition. (See Example 2.) $$\frac{d y}{d t}=y^{4} ; y=1\( at \)t=0$$
Short Answer
Expert verified
The particular solution is \( y = (-3t + 1)^{-1/3} \).
Step by step solution
01
Separate Variables
To solve the differential equation \( \frac{d y}{d t} = y^4 \), we begin by separating the variables. This involves rearranging the equation to have all terms involving \( y \) on one side and all terms involving \( t \) on the other side. Divide both sides by \( y^4 \) and multiply both sides by \( dt \): \[ y^{-4} dy = dt \]
02
Integrate Both Sides
Now that we have separated the variables, we integrate both sides of the equation with respect to their respective variables. Integrate \( \int y^{-4} \, dy \) and \( \int dt \):\[ \int y^{-4} \, dy = \int dt \]The left integral gives \(-\frac{1}{3}y^{-3}\) and the right integral gives \(t + C\). Therefore, we obtain:\[-\frac{1}{3}y^{-3} = t + C\]
03
Solve for the General Solution
To express \( y \) in terms of \( t \), solve the equation for \( y \). Multiply both sides by \(-3\):\[ y^{-3} = -3(t + C) \]Taking the cube root of both sides gives:\[ y = (-3(t + C))^{-1/3} \]
04
Find the Particular Solution
Use the initial condition \( y = 1 \) when \( t = 0 \) to determine the constant \( C \). Substitute \( t = 0 \) and \( y = 1 \) into the general solution:\[ 1 = (-3(0 + C))^{-1/3} \]Cube both sides to get rid of the cube root:\[ 1 = -3C \]Solve for \( C \):\[ C = -\frac{1}{3} \]
05
Write the Particular Solution
Substitute \( C = -\frac{1}{3} \) back into the general solution to obtain the particular solution:\[ y = \left(-3\left(t - \frac{1}{3}\right)\right)^{-1/3} \]This simplifies to:\[ y = \left(-3t + 1\right)^{-1/3} \]
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Separation of Variables
Separation of variables is a crucial technique used to solve differential equations. It involves rearranging the equation so that each variable appears on a different side of the equation. This process simplifies solving, as each variable can be integrated independently.
For example, consider the given differential equation \( \frac{dy}{dt} = y^4 \). By separating variables, we rewrite it as \( y^{-4} \, dy = dt \).
This separation allows us to deal with the equation using integration. Here, the equation is arranged such that all terms involving \( y \) are on one side and those involving \( t \) are on the other. This is a necessary step in making these equations more manageable to solve.
For example, consider the given differential equation \( \frac{dy}{dt} = y^4 \). By separating variables, we rewrite it as \( y^{-4} \, dy = dt \).
This separation allows us to deal with the equation using integration. Here, the equation is arranged such that all terms involving \( y \) are on one side and those involving \( t \) are on the other. This is a necessary step in making these equations more manageable to solve.
Integration
Integration is a mathematical operation that is used to find a function, known as the antiderivative, from its derivative. After separating variables in a differential equation, integration is the next logical step to determine the general solution.
Each side of our separated equation, \( \int y^{-4} \, dy = \int dt \), is integrated with respect to its own variable. For \( \int y^{-4} \, dy \), the antiderivative is \(-\frac{1}{3}y^{-3} \). For \( \int dt \), it results in \( t + C \), where \( C \) represents the constant of integration.
Through integration, we find the general form of the solution to the differential equation, which in this case is \(-\frac{1}{3}y^{-3} = t + C \). Integration is vital as it transforms a rate of change into a comprehensible function.
Each side of our separated equation, \( \int y^{-4} \, dy = \int dt \), is integrated with respect to its own variable. For \( \int y^{-4} \, dy \), the antiderivative is \(-\frac{1}{3}y^{-3} \). For \( \int dt \), it results in \( t + C \), where \( C \) represents the constant of integration.
Through integration, we find the general form of the solution to the differential equation, which in this case is \(-\frac{1}{3}y^{-3} = t + C \). Integration is vital as it transforms a rate of change into a comprehensible function.
Initial Conditions
Initial conditions are specific values provided in a problem that allow us to solve for any constants in the general solution. They personalize the solution to match the context of a given situation.
In our exercise, the initial condition given is \( y = 1 \) when \( t = 0 \). By substituting these values into the general solution, \(-\frac{1}{3}(1)^{-3} = 0 + C \), we obtain \( 1 = -3C \). Solving this yields \( C = -\frac{1}{3} \).
These initial conditions are crucial in converting a general solution into a particular solution, which precisely aligns with real-world scenarios.
In our exercise, the initial condition given is \( y = 1 \) when \( t = 0 \). By substituting these values into the general solution, \(-\frac{1}{3}(1)^{-3} = 0 + C \), we obtain \( 1 = -3C \). Solving this yields \( C = -\frac{1}{3} \).
These initial conditions are crucial in converting a general solution into a particular solution, which precisely aligns with real-world scenarios.
Particular Solution
The particular solution of a differential equation is the specific solution obtained after satisfying the initial conditions. Once we determine the constant \( C \), we substitute it back into the general solution.
For the given problem, by substituting \( C = -\frac{1}{3} \) into the general solution, we attain the particular solution \( y = \left(-3t + 1\right)^{-1/3} \).
This provides a definitive answer that uniquely meets the initial condition \( y = 1 \) when \( t = 0 \). The role of the particular solution is to ensure the solution's applicability to the specific scenario described.
For the given problem, by substituting \( C = -\frac{1}{3} \) into the general solution, we attain the particular solution \( y = \left(-3t + 1\right)^{-1/3} \).
This provides a definitive answer that uniquely meets the initial condition \( y = 1 \) when \( t = 0 \). The role of the particular solution is to ensure the solution's applicability to the specific scenario described.