Are there closed curve solutions for these ODE constraints?

In summary, there is a proposition that states acceleration is orthogonal to position. This may not necessarily imply that \frac{d^2}{dt^2}\mathbf{v}(t) = 0, but there are non-trivial solutions that satisfy this constraint. These solutions can be found by solving a 4th order ODE.
  • #1
MisterX
764
71
Are there closed curve solutions for ##\mathbf{v}(t) \in \mathbb{R}^3## satisfying this constraint?
$$\mathbf{v}(t) \cdot \frac{d^2}{dt^2}\mathbf{v} = 0 $$
 
Last edited:
Physics news on Phys.org
  • #2
I do not understand your question. All velocities of type v(t) = a⋅t + v0 are trivial solutions.
 
  • #3
Unless v(t) is identically 0, so there is no motion at all, you equation just says that the acceleration is 0 so, as Svein says, the only solutions are straight line trajectories.
 
  • #4
Thanks for your replies. To be clear I meant

$$\sum_{i=1}^3 v_i \frac{d^2 v_i}{d t^2} = 0 $$

In other words acceleration is orthogonal to position. So ##\mathbf{v}(t) \neq 0## does not obviously (to me) imply ##\frac{d^2}{dt^2}\mathbf{v}(t) = 0##. I may still be that the trivial solutions mentioned above are the only ones, but I'm not sure at the moment.
 
  • #5
MisterX said:
In other words acceleration is orthogonal to position.
Ah. That is a different proposition. Of course, the trivial solutions are still solutions, but...

If an object rotates in a circle around a point, the acceleration is orthogonal to velocity, but I do not know offhand any solution to acceleration orthogonal to position. A logarithmic spiral springs to mind, but there acceleration is never quite orthogonal to position (http://en.wikipedia.org/wiki/Logarithmic_spiral ).
 
  • #6
Yes non-trivial solutions exist.

Consider the case where [itex]\frac{d^2}{dt^2} v_x = v_z [/itex] ,[itex] \frac{d^2}{dt^2}v_z = - v_x[/itex], and [itex] v_y=0 [/itex].

Here [itex]\vec V \cdot \frac{d^2}{dt^2}\vec V =0 [/itex].

You can solve for [itex] v_x [/itex] and [itex] v_z [/itex]. This amounts to solving the 4-th order ODE [itex]\frac{d^4}{dt^4} v_x + v_x =0 [/itex]. Real solutions to this equation exist. The resulting expression for [itex] v_z [/itex] is also real.
 
  • Like
Likes MisterX

FAQ: Are there closed curve solutions for these ODE constraints?

1. What are ODE constraints?

ODE constraints refer to the conditions or restrictions that are imposed on a system of Ordinary Differential Equations (ODEs). These constraints can include initial or boundary conditions, as well as any other limitations on the variables or parameters in the ODE system.

2. What are closed curve solutions?

A closed curve solution is a solution to an ODE system that forms a closed loop or curve. This means that the solution returns to its starting point after completing a full cycle. Closed curve solutions are often used to model periodic or cyclical phenomena.

3. Are there closed curve solutions for all ODE constraints?

No, not all ODE constraints have closed curve solutions. The existence of closed curve solutions depends on the specific ODE system and its constraints. In some cases, it may not be possible to find a closed curve solution, while in others, multiple closed curve solutions may exist.

4. How do closed curve solutions differ from other types of solutions?

Closed curve solutions differ from other types of solutions, such as open curve solutions or singular solutions, in that they form a closed loop or curve. This means that the solution repeats itself after a certain period or interval, whereas other types of solutions may not have this repetition.

5. What are some real-world applications of closed curve solutions?

Closed curve solutions have various real-world applications, including in physics, engineering, and biology. They can be used to model and understand periodic phenomena such as the motion of a pendulum, the behavior of electrical circuits, and the population dynamics of species. Closed curve solutions are also useful for predicting and analyzing cyclic processes in economics, finance, and other fields.

Back
Top