No, in the heuristic approximation you are using here, the strong interaction does not weaken with distance; it strengthens with distance, so it takes more and more energy to try to pull two quarks apart, for example, as they get further apart (whereas the energy it takes to pull, say, an electron and a proton apart gets less and less as they get further apart).
So, for example, if you try to pull apart the quark and antiquark inside a pion, at a distance scale of roughly a femtometer, the energy required to pull the two quarks apart is large enough to create another quark-antiquark pair, and so you end up with two pions. You never get free quarks.
Similar remarks would apply to trying to pull a gluon out of, say, a glueball; you just end up making more gluons and making the glueball larger; you never get free gluons.
That sort of makes intuitive sense, right? If the force were weaker so that it "snapped" at 10 femtometers, you'd expect protons themselves to be somewhere in that size range as well.
(Or am I totally wrong?)
I _think_ I expect it to be quite high. My understanding is it's "weak" because it falls off quickly, past a certain distance, due to the force carrier having mass.
This is the explanation for why when we collide beams of protons at near c they don’t produce a new higher energy particle, but a massive shower of secondary and tertiary particles like pions and kaons as a result of the decay chain from initial pair production.
But then when the energy becomes great enough and it snaps into a new pair of gluons, do those new gluons go anywhere or do they stay in between the original pair of particles. Do the original particles shoot off into the distance because the force holding them together got converted into some new particles?
Is there a link where I could read more? At these super small scales all my intuitions break down so I'd like something more mathematical to get a grasp on things :)
Just like photons arise from the curvature of the electric charge field.
This is extremely complicated, it's called gauge theory.
> Is there a link where I could read more?
Ask your favourite LLM, it will explain much better.
Or 5 hour video on the subject, but with all the math:
So in the model of two proton beams near c intersecting you essentially have the protons go through a phase change- they almost melt into a quark-gluon plasma that's stupendously hot- followed by a rapid condensation into a showers of kaons, pions, new protons... all of it adds up to the original mass of the protons in the collision. If you surround the area of that collision with EXTREMELY sensitive calorimeters and devices designed to monitor this process you can do some incredible accounting to find out what if anything is missing. That missing bit would be a possible new particle, some new physics, or as is often the case a chance to learn more about possible errors in measurement.
https://modern-physics.org/hadronization/
https://profmattstrassler.com/articles-and-posts/particle-ph...