Problem 3
Question
In Problems, write the given nonlinear second-order differential equation as a plane autonomous system. Find all critical points of the resulting system. $$ x^{\prime \prime}+x^{\prime}\left(1-x^{3}\right)-x^{2}=0 $$
Step-by-Step Solution
Verified Answer
The plane autonomous system is \( x'=y \), \( y'=-y(1-x^3)+x^2 \), with the critical point at \( (0,0) \).
1Step 1: Introduce New Variables
To convert the given second-order differential equation \( x'' + x'(1-x^3) - x^2 = 0 \) into a system of first-order differential equations, we start by introducing a new variable. Let \( y = x' \), which implies \( y' = x'' \). This allows us to express the equation in terms of \( x \) and \( y \).
2Step 2: Write the System of First-Order Equations
Substituting \( y = x' \) into the original equation, we get \( y' = -y(1-x^3) + x^2 \). Thus, the system of equations becomes:- \( x' = y \)- \( y' = -y(1-x^3) + x^2 \).
3Step 3: Identify the Plane Autonomous System
The plane autonomous system derived from the given nonlinear second-order differential equation is:- \( \frac{dx}{dt} = y \)- \( \frac{dy}{dt} = -y(1-x^3) + x^2 \). This is a system of two first-order equations in the variables \( x \) and \( y \).
4Step 4: Find Critical Points
The critical points of the system occur where both derivatives are zero. Set \( \frac{dx}{dt} = y = 0 \) and \( \frac{dy}{dt} = -y(1-x^3) + x^2 = 0 \). The first equation, \( y = 0 \), is immediately satisfied. The second equation reduces to \( x^2 = 0 \), resulting in \( x = 0 \). Therefore, the only critical point is \( (0, 0) \).
Key Concepts
Nonlinear Differential EquationsCritical PointsFirst-Order Differential Equations
Nonlinear Differential Equations
Nonlinear differential equations differ from linear ones because they involve terms that are not simply proportional to the unknown function or its derivatives. In other words, the equation can contain powers or products of the variable and its derivative, making them more complex and challenging to solve. For instance, the equation \( x'' + x'(1-x^3) - x^2 = 0 \) is nonlinear because it includes a term \( x'(1-x^3) \). This term is nonlinear since it involves both a multiplication and a power of the variable \( x \).
- These equations model more complex systems that linear equations cannot adequately describe, such as chaotic systems or those exhibiting large changes.
- Nonlinear equations often require numerical methods or approximations for solutions, as closed-form solutions can be elusive.
Critical Points
Critical points in a differential equation are the values of the variable and its derivative where the derivatives both equal zero. These points are crucial because they often indicate equilibrium points where the system doesn't change, making them important for understanding system stability.In the context of the provided problem, finding critical points involved solving the equations \( \frac{dx}{dt} = y = 0 \) and \( \frac{dy}{dt} = -y(1-x^3) + x^2 = 0 \). Setting \( y = 0 \) simplified the system drastically as it tells us part of the critical condition already. The remaining equation, \( x^2 = 0 \), gives us \( x = 0 \). Therefore, the only critical point is \((0, 0)\).
- Identifying critical points helps understand the stable/unstable nature of a system.
- Further analysis like linearization and eigenvalue calculations around these points can reveal more about the system's behavior.
First-Order Differential Equations
First-order differential equations involve the first derivative of the unknown function and no higher derivatives. They are essential because many complex higher-order differential equations can be converted into a system of first-order equations, facilitating easier analysis and computational solving.In our exercise, the second-order equation \( x'' + x'(1-x^3) - x^2 = 0 \) was converted into a system of first-order differential equations by introducing a new variable \( y = x' \). This resulted in:- \( x' = y \)- \( y' = -y(1-x^3) + x^2 \)
- Each equation describes the rate of change of one variable in terms of others, forming a "plane autonomous system".
- This transformation to first-order systems is a standard technique for solving and visualizing differential equations.
Other exercises in this chapter
Problem 3
The general solution of the linear system \(\mathbf{X}^{\prime}=\mathbf{A} \mathbf{X}\) is given. (a) In each case discuss the nature of the solution in a neigh
View solution Problem 3
In Problems \(3-10\), without solving explicitly, classify the critical points of the given first-order autonomous differential equation as either asymptoticall
View solution Problem 3
Show that the given plane autonomous system (or second-order differential equation) has no periodic solutions. $$ \begin{aligned} &x^{\prime}=-x+y^{2} \\ &y^{\p
View solution Problem 3
Without solving explicitly, classify the critical points of the given first- order autonomous differential equation as either asymptotically stable or unstable.
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