XiXiDu comments on Edward Nelson claims proof of inconsistency in Peano Arithmetic - Less Wrong
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FTL neutrinos and now a proof of inconsistency in Peano Arithmetic? What next?
I have devised a little proof of inconsistency of the Newtonian mechanics, years ago.
http://critticall.com/alog/Antinomy_inside_mechanics.pdf
Can you spot the error?
Vg vf pbeerpg gung ng g=0, rnpu cnegvpyr unf n yrsgjneqf irybpvgl. Ohg vg vf abg pbeerpg gung gur prager bs tenivgl ng g=0 unf n yrsgjneqf irybpvgl. Guvf vf orpnhfr gur flfgrz orunirf qvfpbagvahbhfyl ng g=0, naq fb gur irybpvgl bs gur prager bs tenivgl pnaabg or qrgrezvarq ol gnxvat n jrvtugrq nirentr bs gur vavgvny irybpvgvrf bs gur pbzcbaragf.
Va zber qrgnvy:
Yrg P(g) or gur cbfvgvba bs gur prager bs tenivgl ng gvzr g.
Gur irybpvgl bs gur prager bs tenivgl ng g=0 vf gur yvzvg nf g -> 0 bs (P(g)-P(0))/g.
Ng nal gvzr g, P(g) vf gur fhz bire a bs Z(a)C(a,g), jurer Z(a) vf gur znff bs gur agu cbvag naq C(a,g) vgf cbfvgvba.
Gur nethzrag eryvrf ba pbzchgvat qP/qg nf gur fhz bire a bs Z(a)qC(a,g)/qg. Guvf fjncf gur beqre bs gjb yvzvgvat cebprffrf, fhzzngvba naq qvssreragvngvba, juvpu vf inyvq sbe jryy-orunirq fhzf, ohg abg sbe guvf bar.
For intuition, imagine that there were just the first three particles in the sequence, and that the number 10 is replaced by something much larger. The two leftmost particles will rapidly oscillate about one another, while drifting slowly towards the rightmost. Now imagine the first four particles are present. The two leftmost will oscillate madly about each other, while that system as a whole oscillates rapidly about the third from the left (I'm conveniently ignoring what happens at the instants when particles meet and pass through each other), and the ensemble of the three leftmost drifts towards the rightmost. Repeat.
It's acceleration that matters, not velocity (the initial velocity of all points is zero, or at least that's how I thought of it). However, your argument does generalize nicely to acceleration, and could possibly be the correct resolution.
Yes, stupid mistake of mine. Replace velocity by acceleration and position by velocity and the same argument works. The fallacy is in the vagrepunatr bs yvzvgf.
Similar, for those who enjoyed discussing this problem: Did you know that Newtonian mechanics is indeterministic?
These equations don't make sense dimensionally. Are there supposed to be constants of proportionality that aren't being mentioned? Are they using the convention c=1? Well, I doubt it's relevant (scaling things shouldn't change the result), but...
Edit: Also, perhaps I just don't know enough differential equations, but it's not obvious to me that a curve such as he describes exists. I expect it does; it's easy enough to write down a differential equation for the height, which will give you a curve that makes sense when r>0, but it's not obvious to me that everything still works when we allow x=0.
That is my guess. The simplest way IMO would be replace the g in eq. 1 by a constant c with units of distance^(-1/2). The differential equation becomes r'' = g c r^1/2, which works dimensionally. The nontrivial solution (eq. 4) is correct with an added (c g)^2 in front.
I'm not sure what you mean here. What could be wrong in principle with a curve h = c r^3/2 describing the shape of a dome, even at r = 0?
Notice "r" here does not mean the usual radial distance but rather the radial distance along the curve itself. I don't see any obvious barrier to such a thing and I expect it exists, but that it actually does isn't obvious to me; the resulting differential equation seems to have a problem at h=0, and not knowing much about differential equations I have no idea if it's removable or not (since getting an explicit solution is not so easy).
You piqued my curiosity, so I sat to play a little with the equation. If R is the usual radial coordinate, I got:
dh/dR = c y^(1/3) / [(1 - c^2 y^(2/3))^(1/2)]
with y = 3h/(2c), using the definition of c in my previous comment. (I got this by switching from dh/dr to dh/dR with the relation between sin and tan, and replaciong r by r(h). Feel free to check my math, I might have made a mistake.) This was easily integrated by Mathematica, giving a result that is too long to write here, but has no particular problem at h = 0, other than dR/Dh being infinite there. That is expected, it just means dh/dR = 0 so the peak of the dome is a smooth maximum.
Vf vg gung gur vavgvny irybpvgl bs gur znggre vf mreb, gur vavgvny naq riraghny nppryrengvba bs gur pragre bs tenivgl vf mreb, ohg gur pragre bs tenivgl vgfrys ortvaf jvgu n yrsgjneq irybpvgl?
This is a good one, but I won't try doing the math to figure out the specific error with it (other than the obvious problem of (rot13) gur arrq gb pnyphyngr gur rssrpg bs nyy gur znffrf, abg whfg gur vzzrqvngryl ba gur evtug naq gur vzzrqvngryl ba gur yrsg.)
Here's what my intuition is telling me: Gung jung jvyy npghnyyl unccra vf gung gur znffrf jvyy pbairetr fbzrjurer va gur pragre, jvgu fbzr bs gur znffrf nsgre gur zvqqyr cbvag zbivat evtugjneqf vafgrnq. V vzntvar gung V'q unir gb hfr vagrtengvba bire gur ahzore bs vasvavgr znffrf ba gur yrsg, gb frr gung gur zngu sbepr gur jubyr guvat gb onynape.
Gur prager bs znff vf ng gur bevtva naq fgnlf gurer?
Clever! It took me a couple of minutes to get it: Gur yrsgzbfg cbvag (gur 1 xt znff) jvyy zbir gb gur evtug, xrrcvat gur pragre bs tenivgl jurer vg vf. Fb vg'f abg gehr gung "jr pna cebir guvf sbe rirel cbvag.
You are misreading which one's the rightmost mass. The rightmost mass is the one with 1kg.
Whoops, you're right. I assumed +1/10 meant +1/10th from +1. I had the whole thing backwards.
Gurer vf ab reebe. Gur cevapvcyr gung gur pragre bs znff pnaabg nppryrengr pbzrf sebz gur snpg gung, sbe nal cbvag znff, gur sbepr vg rkregf ba bgure znffrf vf rknpgyl bccbfvgr gb gur sbepr bgure znffrf rkreg ba vg. Guvf qbrf abg nccyl gb vasvavgr pbyyrpgvbaf bs znffrf sbe gur fbzr ernfba gung na vasvavgr frevrf bs barf qbrf abg nqq gb mreb, rira gubhtu vg vf gur qvssrerapr orgjrra gjb vqragvpny frevrf, rnpu gur fhz bs nyy cbfvgvir vagrtref.
Vs lbh guvax gurer vf n fcrpvsvp qviretrag frevrf, anzr vg.
Gur fhz bs gur gbgny sbeprf ba nyy cnegvpyrf.
vf yrff guna 0 sbe rirel grez va gur bhgre fhz, rira gubhtu lbh pna pnapry bhg nyy gur grezf ol ernpuvat vagb gur vaare fhzf.
To put code blocks in mark down put four spaces before the lines you want to be code. I assume that is what you intended?
Edited, although I'm not sure it's all that much more readable now.
I was thinking of including a line break or two. ;)
Good idea.
bx, gung vf n ceboyrzngvp erneenatrzrag. Ohg juvpu fvqr vf pbeerpg? Lbh znqr n pynvz nobhg guvf va lbhe bevtvany pbzzrag, ohg V guvax lbh tbg vg onpxjneqf.
My previous attempt at a reply didn't make much sense. And this is deep enough into the thread that I won't bother with rot13.
Let's try again: The description given by Thomas accurately models how each individual particle accelerates (towards the origin). It thus also accurately models how the center of mass accelerates in the non-limiting case.
I think Richard Kennaway's answer is correct and it seems to me to be opposite to your original answer. The non-limiting case is not interesting. The question is whether there is a coherent extension of Newtonian mechanics to infinitely many particles. It does cover this case and the center of mass still works.
I think this paradox shows that the answer is no.
I can't figure out what this sentence was intended to mean.
Richard Kennaway's answer
V guvax gung va gur aba-yvzvgvat pnfr, gur neenatrzrag fubjvat rirelguvat qevsgvat gbjneqf gur bevtva vf pbeerpg naq gur neenatrzrag fubjvat gur pragre bs znff fgnlvat fgvyy vf va reebe. Bs pbhefr, va gur yvzvg nf gur ahzore bs cbvag znffrf vapyhqrq tbrf gb vasvavgl, vg'f gur bgure jnl nebhaq.
An elegant puzzle.
Gur fbyhgvba vf rnfvrfg gb frr vs jr pbafvqre n svavgr ahzore bs vgrengvbaf bs gur cebprqher bs fcyvggvat bss n fznyyre znff. Va rnpu vgrengvba, gur yrsgzbfg znff onynaprf gur obbxf ol haqretbvat irel encvq nppryrengvba gb gur evtug. Va gur yvzvg nf gur ahzore bs vgrengvbaf tbrf gb vasvavgl, jr unir na vasvavgrfvzny znff onynapvat gur obbxf jvgu vasvavgryl ynetr nppryrengvba.
I think the solution I came up with is, in spirit, the same as this one.
Pbafvqre gur nzbhag bs nppryrengvba rnpu cnegvpyr haqretbrf. Gur snegure lbh tb gb gur yrsg, gur terngre gur nppryrengvbaf naq gur fznyyre gur qvfgnaprf, naq, guhf, gur yrff gvzr vg gnxrf orsber n pbyyvfvba unccraf. (V pbhyq or zvfgnxra gurer.) Sbe rirel cbfvgvir nzbhag bs gvzr, pbyyvfvbaf unccra orsber gung nzbhag bs gvzr. Gurersber, gur orunivbe bs gur flfgrz nsgre nal nzbhag bs gvzr vf haqrsvarq.
Jung vs jr fhccbfr gung gur obqvrf pna cnff guebhtu rnpu bgure? Ubj qbrf gur flfgrz orunir nf gvzr cebterffrf?
Vg'f rnfl rabhtu gb rkgraq arjgbavna zrpunavpf gb unaqyr gjb-cnegvpyr pbyyvfvbaf. Whfg cvpx bar bs "rynfgvp pbyyvfvba" be "cnff guebhtu rnpu bgure", naq nccyl gur pbafreingvba ynjf naq flzzrgevrf. Ohg V'z abg njner bs nal cebcbfnyf gb unaqyr guerr-be-zber-cnegvpyr pbyyvfvbaf: va gung pnfr, pbafreingvba bs raretl naq zbzraghz vfa'g rabhtu gb qrgrezvar gur bhgchg fgngr, lbh'q arrq fbzr npghny qlanzvpf gung ner qrsvarq ba gur vafgnag bs pbyyvfvba.
Do you have a reference for how to extend Newtonian mechanics to collisions or passing-through of point particles subject to gravity? how about people complaining about 3 body collisions?
Bringing in energy and momentum doesn't sound helpful to me because they are both infinite at the point of collision.
My understanding is that both of the choices has a unique analytic extension to the complex plane away from the point of collision. Most limiting approaches will agree with this one. In particular, Richard Kennaway's approach (to non-collision) is perturb the particles into another dimension, so that the particles don't collide. The limit of small perturbation is the passing-through model.
For elastic collisions, I would take the limit of small radius collisions. I think this is fine for two body collisions. In dimension one, I can see a couple ways to do three body collisions, including this one. The other, once you can do two body collisions, is to perturb one of bodies, to get a bunch of two body collisions; in the limit of small perturbation, you get a three body collision. But if you extend this to higher dimension, it results in the third body passing through the collision (which is a bad sign for my claim that most limiting approaches agree). When I started writing, I thought the small radius approach had the same problem, but I'm not sure anymore.
Yes, I think so too.