The trajectories of the system are concentric circles centered at the critical point (0,0).
The given second-order differential equation is x′′ +x+x=0, which can be written in the form x′′ +2x=0. This is a simple harmonic oscillator equation with a natural frequency of ω= √2
To find the implicit equations of the trajectories, we can first write the system as a set of first-order differential equations. Let v=x′ , then the system becomes:
x′ =v
v′=−x
Now, we have a system of first-order differential equations:
dx/dt= =v
dv/ dt =−x
This system can be written in vector form as u′ =f(u), where
u=
and f(u)=
![\left[\begin{array}{ccc}v\\-x\end{array}\right]](https://img.qammunity.org/2024/formulas/mathematics/high-school/3vjgwgmiyt0jiqex7ljdbq9q0v0f3d6llt.png)
Now, to find the critical points, we set f(u) equal to the zero vector:
v=0
−x=0
This gives us two critical points:
(x,v)=(0,0).
To classify the critical points, we can consider the linearization of the system around each critical point. The Jacobian matrix J is given by:
J=
![\left[\begin{array}{ccc}0&1\\-1&0\end{array}\right]](https://img.qammunity.org/2024/formulas/mathematics/high-school/55y8qpvz8dh92zefd21wz0rba0qna5am1g.png)
Evaluating this matrix at the critical point (0,0), we get:
J(0,0)=
![\left[\begin{array}{ccc}0&1\\-1&0\end{array}\right]](https://img.qammunity.org/2024/formulas/mathematics/high-school/55y8qpvz8dh92zefd21wz0rba0qna5am1g.png)
The eigenvalues of this matrix are λ=±i, which indicates that the critical point is a center. Therefore, the trajectories of the system are concentric circles centered at the critical point (0,0).