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Groups > sci.math > #647082 > unrolled thread
| Started by | Hayden Maksimov <mmivy@eh.ru> |
|---|---|
| First post | 2026-08-01 14:00 +0000 |
| Last post | 2026-08-06 13:51 +0000 |
| Articles | 15 — 9 participants |
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Re: What amount of acceleration involved is too high for SR to apply? Hayden Maksimov <mmivy@eh.ru> - 2026-08-01 14:00 +0000
Re: What amount of acceleration involved is too high for SR to apply? Thomas Heger <ttt_heg@web.de> - 2026-08-03 06:28 +0200
Re: What amount of acceleration involved is too high for SR to apply? Brooks Mikhaltsov <oov@vhitsair.ru> - 2026-08-03 12:01 +0000
Re: What amount of acceleration involved is too high for SR to apply? Thomas Heger <ttt_heg@web.de> - 2026-08-05 07:21 +0200
Re: What amount of acceleration involved is too high for SR to apply? Toney Zolotenkov <ennv@nkt.ru> - 2026-08-06 13:20 +0000
Re: What amount of acceleration involved is too high for SR to apply? Ross Finlayson <ross.a.finlayson@gmail.com> - 2026-08-06 06:51 -0700
Re: What amount of acceleration involved is too high for SR to apply? Rondell Martzenkov <dank@lona.ru> - 2026-08-06 13:57 +0000
Re: What amount of acceleration involved is too high for SR to apply? Ross Finlayson <ross.a.finlayson@gmail.com> - 2026-08-06 07:09 -0700
Re: What amount of acceleration involved is too high for SR to apply? Yves Bilbasov <say@aee.ru> - 2026-08-06 18:01 +0000
Re: What amount of acceleration involved is too high for SR to apply? Ross Finlayson <ross.a.finlayson@gmail.com> - 2026-08-06 11:30 -0700
Re: What amount of acceleration involved is too high for SR to apply? Cole Baharev <bae@avoa.ru> - 2026-08-06 20:01 +0000
Re: What amount of acceleration involved is too high for SR to apply? Thomas Heger <ttt_heg@web.de> - 2026-08-06 05:33 +0200
Re: What amount of acceleration involved is too high for SR to apply? Ross Finlayson <ross.a.finlayson@gmail.com> - 2026-08-05 21:48 -0700
Re: What amount of acceleration involved is too high for SR to apply? Ross Finlayson <ross.a.finlayson@gmail.com> - 2026-08-06 01:13 -0700
Re: What amount of acceleration involved is too high for SR to apply? Mercury Abdrahmanoff <frm@rbrh.ru> - 2026-08-06 13:51 +0000
| From | Hayden Maksimov <mmivy@eh.ru> |
|---|---|
| Date | 2026-08-01 14:00 +0000 |
| Subject | Re: What amount of acceleration involved is too high for SR to apply? |
| Message-ID | <114ku54$3pu7t$1@news.nntp4.net> |
Thomas Heger wrote: > In my opinion 'speed of light' is actually an angle (in a complex > plane). > > That view is a little unusual. But I think, it's actually correct. > > This would lead to the conclusion, that the term 'light' denotes > actually a subset of waves, which propagate with c. > > There exist other 'waves' wich 'wiggle' along other axes. > > For instance so called 'scalar waves' are longitudinal and timelike. > > This means: scalar waves have kind of frequency, but in the timelike > direction. you mix shit together, what complex, what scalar, longitudinal etc. Light goes only through space not time. Your 4% adherence fuhrrer mertz wants to disable you right to vote on a party he dont like, worse than mosenior hitler, who comparable was a humanist, protecting jews with swimming pools, theatre, chocolate, good housing, food etc. The free people from outside come to the spa camp to buy food from jews, because as different, they had
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| From | Thomas Heger <ttt_heg@web.de> |
|---|---|
| Date | 2026-08-03 06:28 +0200 |
| Message-ID | <ndajmjFm2t1U1@mid.individual.net> |
| In reply to | #647082 |
Am Samstag000001, 01.08.2026 um 16:00 schrieb Hayden Maksimov: > Thomas Heger wrote: > >> In my opinion 'speed of light' is actually an angle (in a complex >> plane). >> >> That view is a little unusual. But I think, it's actually correct. >> >> This would lead to the conclusion, that the term 'light' denotes >> actually a subset of waves, which propagate with c. >> >> There exist other 'waves' wich 'wiggle' along other axes. >> >> For instance so called 'scalar waves' are longitudinal and timelike. >> >> This means: scalar waves have kind of frequency, but in the timelike >> direction. > > you mix shit together, what complex, what scalar, longitudinal etc. Light > goes only through space not time. Your 4% adherence fuhrrer mertz wants to > disable you right to vote on a party he dont like, worse than mosenior > hitler, who comparable was a humanist, protecting jews with swimming > pools, theatre, chocolate, good housing, food etc. The free people from > outside come to the spa camp to buy food from jews, because as different, > they had Well, you put '...mix shit together...' to another level. First: the Nazis didn't allow ANY opposition after they took over power in a coup (apparently assisted by anglo american finance and agencies). Merz (Germany's current Prime minister) didn't do anything similar, but apparently took money from 'Blackrock', because he was formerly the CEO of Blackrock Germany. Not hat nice, but people didn't know much about the PMs former life, until he was already in office. Well, yes, not that good, but by no means comparable to what the Nazis did. Back to physics: I compare spacetime diagrams with Argand diagrams and find similarities. That's why I thought, that spacetime of GR is real and has complex valued components. TH
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| From | Brooks Mikhaltsov <oov@vhitsair.ru> |
|---|---|
| Date | 2026-08-03 12:01 +0000 |
| Message-ID | <114pvvg$2e49$1@news.nntp4.net> |
| In reply to | #647125 |
Thomas Heger wrote: > I compare spacetime diagrams with Argand diagrams and find similarities. > > That's why I thought, that spacetime of GR is real and has complex > valued components. The z-plane is a discrete-time version of the s-plane, where z-transforms are used instead of the Laplace transformation.
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| From | Thomas Heger <ttt_heg@web.de> |
|---|---|
| Date | 2026-08-05 07:21 +0200 |
| Message-ID | <ndfvijFhh0aU2@mid.individual.net> |
| In reply to | #647126 |
Am Montag000003, 03.08.2026 um 14:01 schrieb Brooks Mikhaltsov: > Thomas Heger wrote: > >> I compare spacetime diagrams with Argand diagrams and find similarities. >> >> That's why I thought, that spacetime of GR is real and has complex >> valued components. > > The z-plane is a discrete-time version of the s-plane, where z-transforms > are used instead of the Laplace transformation. That is your view. My oppinion is quite different, because your 'World' isn't symmetric enough. I have written this 'book' about what I think is true: https://docs.google.com/presentation/d/1Ur3_giuk2l439fxUa8QHX4wTDxBEaM6lOlgVUa0cFU4/edit?usp=sharing TH
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| From | Toney Zolotenkov <ennv@nkt.ru> |
|---|---|
| Date | 2026-08-06 13:20 +0000 |
| Message-ID | <11521nf$g130$1@news.nntp4.net> |
| In reply to | #647153 |
Thomas Heger wrote: >>> I compare spacetime diagrams with Argand diagrams and find >>> similarities. >>> >>> That's why I thought, that spacetime of GR is real and has complex >>> valued components. >> >> The z-plane is a discrete-time version of the s-plane, where >> z-transforms are used instead of the Laplace transformation. > > That is your view. > > My oppinion is quite different, because your 'World' isn't symmetric > enough. > > I have written this 'book' about what I think is true: you keep talking nonsense. There is no frequency characterising spacetime, as to be complex. It must be new for me. Try again, where is the missing time stored?
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| From | Ross Finlayson <ross.a.finlayson@gmail.com> |
|---|---|
| Date | 2026-08-06 06:51 -0700 |
| Message-ID | <1kmdnQxLnppXDOn3nZ2dnZfqn_adnZ2d@giganews.com> |
| In reply to | #647161 |
On 08/06/2026 06:20 AM, Toney Zolotenkov wrote: > Thomas Heger wrote: > >>>> I compare spacetime diagrams with Argand diagrams and find >>>> similarities. >>>> >>>> That's why I thought, that spacetime of GR is real and has complex >>>> valued components. >>> >>> The z-plane is a discrete-time version of the s-plane, where >>> z-transforms are used instead of the Laplace transformation. >> >> That is your view. >> >> My oppinion is quite different, because your 'World' isn't symmetric >> enough. >> >> I have written this 'book' about what I think is true: > > you keep talking nonsense. There is no frequency characterising spacetime, > as to be complex. It must be new for me. Try again, where is the missing > time stored? > There's no other place for it to be stored, time, except in itself. This is for something like "there are no closed time-like curves, yet there are no finite closed time-like curves, yet there are everywhere closed infinitesimal time-like curves." Also there's the "clocks meet or slow", that they are always meeting or slowing, that that's an account of the relativity in the absolute. If something's got to give, and nothing can give, then it gives everywhere at all, not quite nothing at all. Luckily, the way the entire classical foundation and all the modern physics is defined and derived, there's plenty of _room_ in the theory, just sitting there, and besides the _room_ that mathematics owes physics, there's _room_ in the formalisms, and conveniently, the data. Motion always both takes and makes room, in _space_, with _real_ space-contraction. These then here are called space-frames and frame-spaces, the Raume-Rahmen and Rahme-Raumen, for example modern relativity-theory says everything is frames, in space, it doesn't say that everything isn't space, in frames. So, everybody being totally subject the theory, also the theory's subject itself, which also goes for mathematics, since there's both infinity and continuity, yet also, lines that cross and lines that meet. So, the post-modern criticism class you sat through for some patchouli-smelling girl, maybe its deconstructive account is more important for making sense of theory than you may recall. Not that patchouli is particularly interesting, just making an example not from my own experience.
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| From | Rondell Martzenkov <dank@lona.ru> |
|---|---|
| Date | 2026-08-06 13:57 +0000 |
| Message-ID | <11523s7$g130$3@news.nntp4.net> |
| In reply to | #647163 |
Ross Finlayson wrote: > There's no other place for it to be stored, time, except in itself. > > This is for something like "there are no closed time-like curves, yet > there are no finite closed time-like curves, > yet there are everywhere closed infinitesimal time-like curves." > > Also there's the "clocks meet or slow", that they are always meeting or > slowing, that that's an account of the relativity in the absolute. i dont undrestand. Bye
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| From | Ross Finlayson <ross.a.finlayson@gmail.com> |
|---|---|
| Date | 2026-08-06 07:09 -0700 |
| Message-ID | <hP2cnbX2bJ_PCOn3nZ2dnZfqn_GdnZ2d@giganews.com> |
| In reply to | #647164 |
On 08/06/2026 06:57 AM, Rondell Martzenkov wrote: > Ross Finlayson wrote: > >> There's no other place for it to be stored, time, except in itself. >> >> This is for something like "there are no closed time-like curves, yet >> there are no finite closed time-like curves, >> yet there are everywhere closed infinitesimal time-like curves." >> >> Also there's the "clocks meet or slow", that they are always meeting or >> slowing, that that's an account of the relativity in the absolute. > > i dont undrestand. Bye > This is that relativity is a way of looking at things, including how things observe each other, yet things are absolute. How about "particles are models of state in a closed system, waves are models of change in an open system". Most people box in their waves as somehow closed and expect their particles to move around. It's like Galileo and moving and spinning bodies, one might aver "Galileo says there's no difference moving and spinning bodies", yet Galileo may correct "actually I don't anything about the difference between moving and spinning bodies, now that we're talking about space-contraction I don't say anything about the difference space-contraction-linear and space-contraction-rotational, that's on you". Then at some point to result a formula explaining a gyroscope, somebody just said "let's just introduce a new force and call it 'angular momentum's', nobody'll really notice if it cancels out". And it's like, going between 0 and 90 degrees, only two of those are right angles. "But I only see one!"
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| From | Yves Bilbasov <say@aee.ru> |
|---|---|
| Date | 2026-08-06 18:01 +0000 |
| Message-ID | <1152i56$gquc$1@news.nntp4.net> |
| In reply to | #647165 |
Ross Finlayson wrote: > And it's like, going between 0 and 90 degrees, only two of those are > right angles. > > "But I only see one!" sinus and cosines are displaced 90⁰ kiss my ass, ie AC current/voltage in a wire; there are no such things in relativity, nor light
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| From | Ross Finlayson <ross.a.finlayson@gmail.com> |
|---|---|
| Date | 2026-08-06 11:30 -0700 |
| Message-ID | <AgadnS39DL5XT-n3nZ2dnZfqnPqdnZ2d@giganews.com> |
| In reply to | #647166 |
On 08/06/2026 11:01 AM, Yves Bilbasov wrote: > Ross Finlayson wrote: > >> And it's like, going between 0 and 90 degrees, only two of those are >> right angles. >> >> "But I only see one!" > > sinus and cosines are displaced 90⁰ kiss my ass, ie AC current/voltage in > a wire; there are no such things in relativity, nor light > Polarity's a thing, then though that phase gets pretty involved, about remanence and reluctance and a bunch of the other kinds of what are often qualitative properties with regards to Ohm and Kirchhoff law in passive and active circuits which are inductor-resistor-capacitor networks or RLC networks, L for inductor, that both the root-mean-square and impedance end up being crossing lines for each other, has that besides Coulomb, are both Ampere and Faraday, with regards usually enough to phase-locked-loops and differential-pairs and temperature-compensated-oscillators, that allow packet electronics, vis-a-vis, power electronics, or, the digital and analog. So, it often happens that the secondary and tertiary qualities are actually primary in the sense of the potential and in-rush and current, vis-a-vis the classical approximation in the middle, why each of Faraday's and Coulomb's and Ampere's have laws that don't much talk to each other. Except that they do, .... The great electricians of the 19'th century have a whole alphabet of lettered electrical fields, most of which are potential-fields, then, Maxwell's equations of relations of fields, is actually two of those or E x B and D x H, which as he notes either one is real, the other then sort of less so. Point being: there's a whole alphabet of potential fields in electricity and magnetism, which Kelvin thinks are kinetic and FitzGerald seems to agree. The O.W. Richardson account of "The Electron Theory of Matter" is great then also relating the whole thing to atomic theory and electron theory, while though both Rutherford and Fermi are a bit more the "solid state" of the electronic, then that Fermi-holes are electron-holes yet electron-holes are not Fermi-holes, since they don't know.
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| From | Cole Baharev <bae@avoa.ru> |
|---|---|
| Date | 2026-08-06 20:01 +0000 |
| Message-ID | <1152p6v$h9k2$1@news.nntp4.net> |
| In reply to | #647167 |
Ross Finlayson wrote: > The great electricians of the 19'th century have a whole alphabet of > lettered electrical fields, most of which are potential-fields, then, > Maxwell's equations of relations of fields, is actually two of those or > E x B and D x H, > which as he notes either one is real, the other then sort of less so. > Point being: there's a whole alphabet of potential fields in electricity > and magnetism, > which Kelvin thinks are kinetic and FitzGerald seems to agree. you know so many things, indeed, i think the magnetic field is causing the 90 degrees displacement, hence the magnetic has to flow parallel with the electric. Thanks.
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| From | Thomas Heger <ttt_heg@web.de> |
|---|---|
| Date | 2026-08-06 05:33 +0200 |
| Message-ID | <ndidkfF7dpiU1@mid.individual.net> |
| In reply to | #647126 |
Am Montag000003, 03.08.2026 um 14:01 schrieb Brooks Mikhaltsov: > Thomas Heger wrote: > >> I compare spacetime diagrams with Argand diagrams and find similarities. >> >> That's why I thought, that spacetime of GR is real and has complex >> valued components. > > The z-plane is a discrete-time version of the s-plane, where z-transforms > are used instead of the Laplace transformation. That's true. But I wanted to start at the GR side and proceed from there to the QM-side. Actually my aim was to build particles out of spacetime (of GR), hence assume the real existence of something like the z-plane (which I simply called 'complex plane'), but 'in volume'. Then the axis of time is local and in a cone around it we find what we call 'space' and perpendicular as an inverse to time the hyperplane of the present. The combination of a static field, which is timeless, hence belongs to the hyperplane of the present, and the axis of time gives an atom, because mass is timelike. This 'atom' is 'relativistic', because it depends on the local axis of time what we call 'atom'. This 'z-plane in volume' could be achieved, if we take a complex plane and 'multiply it by three' as three perpendicular complex planes. Then we combine it with a 'perpendicular' imaginary axis of time and need something like a 'bi-quaternion field', This is quite abstract, sure, but I had written kind of book about this concept called 'structured spacetime' many years ago: https://docs.google.com/presentation/d/1Ur3_giuk2l439fxUa8QHX4wTDxBEaM6lOlgVUa0cFU4/edit?usp=sharing This concept behaves imho quite well and is astonishingly simple. But it is only sooooo different to anything you ever heard of, that hardly anybody understands it. TH
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| From | Ross Finlayson <ross.a.finlayson@gmail.com> |
|---|---|
| Date | 2026-08-05 21:48 -0700 |
| Message-ID | <WC6dnVrN--QPj-n3nZ2dnZfqn_qdnZ2d@giganews.com> |
| In reply to | #647158 |
On 08/05/2026 08:33 PM, Thomas Heger wrote: > Am Montag000003, 03.08.2026 um 14:01 schrieb Brooks Mikhaltsov: >> Thomas Heger wrote: >> >>> I compare spacetime diagrams with Argand diagrams and find similarities. >>> >>> That's why I thought, that spacetime of GR is real and has complex >>> valued components. >> >> The z-plane is a discrete-time version of the s-plane, where z-transforms >> are used instead of the Laplace transformation. > > That's true. > > But I wanted to start at the GR side and proceed from there to the QM-side. > > Actually my aim was to build particles out of spacetime (of GR), hence > assume the real existence of something like the z-plane (which I simply > called 'complex plane'), but 'in volume'. > > Then the axis of time is local and in a cone around it we find what we > call 'space' and perpendicular as an inverse to time the hyperplane of > the present. > > The combination of a static field, which is timeless, hence belongs to > the hyperplane of the present, and the axis of time gives an atom, > because mass is timelike. > > This 'atom' is 'relativistic', because it depends on the local axis of > time what we call 'atom'. > > This 'z-plane in volume' could be achieved, if we take a complex plane > and 'multiply it by three' as three perpendicular complex planes. > > Then we combine it with a 'perpendicular' imaginary axis of time and > need something like a 'bi-quaternion field', > > This is quite abstract, sure, but I had written kind of book about this > concept called 'structured spacetime' many years ago: > > https://docs.google.com/presentation/d/1Ur3_giuk2l439fxUa8QHX4wTDxBEaM6lOlgVUa0cFU4/edit?usp=sharing > > > This concept behaves imho quite well and is astonishingly simple. > > But it is only sooooo different to anything you ever heard of, that > hardly anybody understands it. > > > TH > One may aver that it's changes in acceleration where SR no longer applies. For example an account of rest-exchange-momentum, along with light-speed-rest-frame, both of which are simple admissible interpretations of inertial frames and Lorentzian invariance, then has that the "boost" and so on, which lives in the kinetic, would falsify usual assumptions of usual theories about SR, which is governed by the light-like, or vice-versa.
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| From | Ross Finlayson <ross.a.finlayson@gmail.com> |
|---|---|
| Date | 2026-08-06 01:13 -0700 |
| Message-ID | <m5ucnXdPUv233-n3nZ2dnZfqn_udnZ2d@giganews.com> |
| In reply to | #647159 |
On 08/05/2026 09:48 PM, Ross Finlayson wrote: > On 08/05/2026 08:33 PM, Thomas Heger wrote: >> Am Montag000003, 03.08.2026 um 14:01 schrieb Brooks Mikhaltsov: >>> Thomas Heger wrote: >>> >>>> I compare spacetime diagrams with Argand diagrams and find >>>> similarities. >>>> >>>> That's why I thought, that spacetime of GR is real and has complex >>>> valued components. >>> >>> The z-plane is a discrete-time version of the s-plane, where >>> z-transforms >>> are used instead of the Laplace transformation. >> >> That's true. >> >> But I wanted to start at the GR side and proceed from there to the >> QM-side. >> >> Actually my aim was to build particles out of spacetime (of GR), hence >> assume the real existence of something like the z-plane (which I simply >> called 'complex plane'), but 'in volume'. >> >> Then the axis of time is local and in a cone around it we find what we >> call 'space' and perpendicular as an inverse to time the hyperplane of >> the present. >> >> The combination of a static field, which is timeless, hence belongs to >> the hyperplane of the present, and the axis of time gives an atom, >> because mass is timelike. >> >> This 'atom' is 'relativistic', because it depends on the local axis of >> time what we call 'atom'. >> >> This 'z-plane in volume' could be achieved, if we take a complex plane >> and 'multiply it by three' as three perpendicular complex planes. >> >> Then we combine it with a 'perpendicular' imaginary axis of time and >> need something like a 'bi-quaternion field', >> >> This is quite abstract, sure, but I had written kind of book about this >> concept called 'structured spacetime' many years ago: >> >> https://docs.google.com/presentation/d/1Ur3_giuk2l439fxUa8QHX4wTDxBEaM6lOlgVUa0cFU4/edit?usp=sharing >> >> >> >> This concept behaves imho quite well and is astonishingly simple. >> >> But it is only sooooo different to anything you ever heard of, that >> hardly anybody understands it. >> >> >> TH >> > > > One may aver that it's changes in acceleration where SR no longer applies. > > > For example an account of rest-exchange-momentum, along with > light-speed-rest-frame, both of which are simple admissible > interpretations of inertial frames and Lorentzian invariance, > then has that the "boost" and so on, which lives in the kinetic, > would falsify usual assumptions of usual theories about SR, > which is governed by the light-like, or vice-versa. > > Feynman and Wheeler call that "advanced" and "retarded", the potentials, since the potential fields are outside the usual theory where the classical fields are the real fields, in a potentialistic setting where the potential fields are the real fields. Of course these are at least yet still "fields", not "non-fields" like "Higgs field: not a classical field".
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| From | Mercury Abdrahmanoff <frm@rbrh.ru> |
|---|---|
| Date | 2026-08-06 13:51 +0000 |
| Message-ID | <11523gu$g130$2@news.nntp4.net> |
| In reply to | #647158 |
Thomas Heger wrote: >>> I compare spacetime diagrams with Argand diagrams and find >>> similarities. >>> >>> That's why I thought, that spacetime of GR is real and has complex >>> valued components. >> >> The z-plane is a discrete-time version of the s-plane, where >> z-transforms are used instead of the Laplace transformation. > > That's true. > > But I wanted to start at the GR side and proceed from there to the > QM-side. > > Actually my aim was to build particles out of spacetime (of GR), hence > assume the real existence of something like the z-plane (which I simply > called 'complex plane'), but 'in volume'. > > Then the axis of time is local and in a cone around it we find what we > call 'space' and perpendicular as an inverse to time the hyperplane of > the present. unbelievable so much crap in a short sentence. A z-plane involves discrete sampled frequencies. Do it again, one more time
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