Chapter 3: Problem 42
The differential equation \(d P / d t=(k \cos t) P,\) where \(k\) is a positive constant, is a mathematical model for a population \(P(t)\) that undergoes yearly seasonal fluctuations. Solve the equation subject to \(P(0)=P_{0}\) Use a graphing utility to graph the solution for different choices of \(P_{0}\)
Short Answer
Step by step solution
Identify the Type of Differential Equation
Use Separation of Variables
Integrate Both Sides
Solve for the Integration Constant
Express the Solution in Terms of P(t)
Graph the Solution for Different Values of P_0
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Separation of Variables
This process effectively isolates all terms involving \( P \) on one side and all terms involving \( t \) on the other. By doing this, we create an opportunity to integrate each side with respect to its own variable.
The main benefit of separation of variables is that it simplifies the integration process and can be used in various other types of first-order differential equations as well.
Integration
On the right side, the integral of \( k \cos t \) with respect to \( t \) is \( k \sin t + C \), where \( C \) is the constant of integration. This constant is added because indefinite integration does not specify the bounds, so any number could potentially be added to the function.
- Left side integral: \( \int \frac{dP}{P} = \ln |P| \)
- Right side integral: \( \int k \cos t \, dt = k \sin t + C \)
Mathematical Modeling
Here, the model suggests that the rate of population change is influenced by a constant \( k \) and a sinusoidal function \( \cos t \). This implies that the population experiences periodic fluctuations over time, similar to seasonal changes.
- \( k \) is a positive constant affecting the amplitude of fluctuations.
- \( \cos t \) indicates the periodic nature of the changes.
Initial Conditions
Substituting \( t = 0 \) and \( P = P_0 \) into the integrated equation \( \ln |P| = k \sin t + C \), gives us \( \ln |P_0| = C \). Thus, \( C = \ln P_0 \).
Applying initial conditions is critical as it allows us to solve for unknown constants and arrive at a unique solution that fits the specific circumstances of the problem. With \( C \) known, the particular solution becomes \( P(t) = P_0 e^{k \sin t} \), which can now be used to predict future behavior under the initial conditions specified.