# Circular motion when F=ma'

I apologize in advance if this question is deemed too general or too similar to this and this question.

How would mechanics be different if $F=mx'''$ instead of $F=ma$? I feel like I have intuition about what kind of place an $F=mv$ world would be like, since, after all, this is part of our everyday experience dominated by friction. Let me make my question more specific.

If I pick a ball attached to the end of a string in a $F=mv$ world, I cannot make it move in uniform circular motion by swinging it around. I can separate the ball and the end of string by pulling the two apart, but then pulling on the string simply pulls the ball towards me. $F=mv$ is like living in a very viscous liquid. I've heard that at a very small scale (like that of bacteria), water is like this and this has consequences for the propulsion of microorganisms.

In reality, it is possible to give an initial velocity to the ball and then to tug on the string to rotate the velocity vector so that it is moving in uniform circular motion.

Please correct me if any of the above is wrong.

But what happens if $F=mx'''$? I have no intuition about what would happen with the string and ball example in this case. You could give the ball a constant velocity and zero initial acceleration. But then how does it move constrained by a string that is applying a force which changes acceleration. Would it spiral? What kind of setup of forces could force a particle into circular motion? Is there any way to gain intuition about the consequences of $F=mx'''$?

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Think of force as it works in the real word as the resistance a body has against changing its velocity. In your fantasy world, then, a force is a body resisting against changing its accelleration. Newton's first law, then, would read that a body has constant acceleration unless a force acts upon it. An object in empty space would therefore accelerate constantly and thus gain speed. –  Lagerbaer Sep 12 '11 at 19:52
Yes, thank you, I already understand this. But I don't have general intuition about even slightly more complex physical scenarios, like the ball and string example I give. –  JOwen Sep 12 '11 at 20:00
Aren't questions like this closed if they speculate about what the world would be like if physics wasn't the way it is? –  John McVirgo Sep 12 '11 at 20:20
@John: that thought did occur to me. Generally the questions that we close for that reason are broad and too vaguely defined to say anything useful about them; things like "what if we could travel faster than light." But this one is much more focused; it asks about a specific consequence of altering a specific law of physics in a clearly defined way. I view this as being in the same vein as things like 10-dimensional spacetimes or supersymmetric particles, which people publish papers on all the time - it seems a little hypocritical to close this when so much of modern physics is speculative. –  David Z Sep 12 '11 at 20:43
(cont.) But feel free to open up a meta question on this if you'd like to gather more input from the community. –  David Z Sep 12 '11 at 20:44

Confine the motion to a plane, and for convenience make it the complex plane. Describe the position of a particle in uniform circular motion by $z = Re^{i\omega t}$. Then the jerk (derivative of acceleration} is $z''' = -i\omega^3 z$. Compare that to velocity $z' = i\omega z$. The jerk points opposite the velocity. Thus, to move in uniform circular motion with $F = ma'$, you must constantly feel a force pushing you backwards, opposite your current direction of motion. Additionally, you must have the correct initial conditions for $z(0)$, $z'(0)$, and $z''(0)$.
Presumably, a string could not provide this force, because the force would still act in the direction of the string. We would have $z''' \propto z$, the force in the direction of the motion, if the string followed Hooke's law. The solutions are $z = e^{\alpha t}$ with $\alpha$ some constant times a cube root of unity. The interesting solutions have both periodic and exponential behavior, so the particle would spiral out or spiral in with this force law.