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6. Consider the differential equation \[ \frac{d y}{d t}=y(y-1)^{2}(y-2)^{3}(y-3)^{4} \] Select the equilibrium point(s) in the list below that are nodes: \[ y=0, \quad y=1, \quad y=2, \quad y=3 \]

Ask by Wilson Summers. in the United States
Jan 25,2025

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Answer

Both \( y = 1 \) and \( y = 3 \) are equilibrium points that are nodes.

Solution

In the given differential equation: \[ \frac{d y}{d t} = y(y-1)^{2}(y-2)^{3}(y-3)^{4} \] the equilibrium points occur where \(\frac{dy}{dt} = 0\), which are \(y = 0\), \(y = 1\), \(y = 2\), and \(y = 3\). ### Understanding the Nature of Each Equilibrium Point 1. **\(y = 0\) (Multiplicity 1):** - **Behavior:** - For \(y < 0\), \(\frac{dy}{dt} > 0\). - For \(y > 0\), \(\frac{dy}{dt} > 0\). - **Interpretation:** The solution does not cross \(y = 0\) and flows away from it on both sides, indicating it's a **repelling equilibrium**. 2. **\(y = 1\) (Multiplicity 2):** - **Behavior:** - For \(y < 1\), \(\frac{dy}{dt} > 0\). - For \(y > 1\), \(\frac{dy}{dt} > 0\). - **Interpretation:** The solution does not cross \(y = 1\) and flows away on both sides, making it a **non-crossing equilibrium**. Due to its even multiplicity, it behaves like a **node**. 3. **\(y = 2\) (Multiplicity 3):** - **Behavior:** - For \(y < 2\), \(\frac{dy}{dt} < 0\). - For \(y > 2\), \(\frac{dy}{dt} > 0\). - **Interpretation:** The solution crosses \(y = 2\), changing direction from decreasing to increasing. This indicates a **semi-stable equilibrium**. 4. **\(y = 3\) (Multiplicity 4):** - **Behavior:** - For \(y < 3\), \(\frac{dy}{dt} > 0\). - For \(y > 3\), \(\frac{dy}{dt} > 0\). - **Interpretation:** Similar to \(y = 1\), the solution does not cross \(y = 3\) and flows away on both sides, behaving like a **node** due to its even multiplicity. ### Conclusion **Equilibrium points with even multiplicities (i.e., \(y = 1\) and \(y = 3\)) behave as nodes** in the phase line analysis of this differential equation. **Answer:** Both y = 1 and y = 3 are equilibrium points that are nodes.

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The Deep Dive

To determine the stability of the equilibrium points, we need to analyze the behavior of the differential equation near each point. The equilibrium points are the values of \(y\) for which \(\frac{dy}{dt} = 0\). The given differential equation can be factored as follows: \[ \frac{d y}{d t} = y(y-1)^2(y-2)^3(y-3)^4. \] Setting this equal to zero, we find the equilibrium points: \(y=0\), \(y=1\), \(y=2\), and \(y=3\). Next, we will analyze each equilibrium point's stability by considering the sign of \(\frac{dy}{dt}\) around each point: 1. **At \(y=0\)**: - For \(y < 0\), \(\frac{dy}{dt} < 0\). - For \(y > 0\), \(\frac{dy}{dt} > 0\). - Thus, \(y=0\) is a stable equilibrium (attractor). 2. **At \(y=1\)**: - For \(y < 1\), \(\frac{dy}{dt} < 0\). - For \(y > 1\), \(\frac{dy}{dt} > 0\). - Therefore, \(y=1\) is also a stable equilibrium (attractor). 3. **At \(y=2\)**: - For \(y < 2\), \(\frac{dy}{dt} < 0\) (since \((y-2)^3\) is negative). - For \(y > 2\), \(\frac{dy}{dt} > 0\). - Hence, \(y=2\) is an unstable equilibrium (repeller). 4. **At \(y=3\)**: - For \(y < 3\), \(\frac{dy}{dt} < 0\) (since \((y-3)^4\) is positive). - For \(y > 3\), \(\frac{dy}{dt} > 0\). - Thus, \(y=3\) is a stable equilibrium (attractor). In conclusion, \(y=0\), \(y=1\), and \(y=3\) are nodes, while \(y=2\) is not. Specifically, the nodes are \(y=0\), \(y=1\), and \(y=3\).

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