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Что происходит с расхождением моделей при малых скоростях?

При 0,001 c галилеева сумма даёт 1/500, релятивистская — 2000/1000001. Расхождение около 2·10⁻⁹ лежит в пределах объявленного допуска 10⁻⁶, но «в пределах допуска» не есть «совпало»: числа разные.

This is an assistant explanation, not a calculation result. Check the grounds and sources below.

Results

4

Collection

При 0,001 c галилеева сумма даёт 1/500

1/500

Query parameters · 3
q
question 8: the divergence of the models at small speeds under a declared tolerance
r
slow-efir
o
observable: the ratio of the composed speed to the speed of light — a dimensionless exact fraction
Input facts · 10
  • the setting is declared: the operational conditions of the experiment are named

    s: slow
  • both frames of the setting are declared inertial

    s: slow
  • what is carried is a body with rest mass, not a light signal

    s: slow
  • the speed of the body relative to the SECOND frame along the x axis — the speed to be composed with the frame speed

    s: slowu: 299792.458 m_per_s
  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: slowv: 299792.458 m_per_s
  • the comparison tolerance for a dimensionless observable: an exact fraction declared by the setting

    s: slowo: observable: the ratio of the composed speed to the speed of light — a dimensionless exact fractiontol: 1/1000000
  • the run belongs to this theory and this setting

    rts
    slow-efirthe simple stationary luminiferous ether model in an authored reconstruction: a preferred frame, absolute time, Galilean transformations, c relative to the medium, no dragging and no contractionslow
    slow-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesslow
  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: slow-einsteinmo: slow-dvizhenie
  • §3: the Lorentz factor presented by the case; its agreement with the speed is checked by the computing package by an identity without a square root

    r: slow-einsteing: 1
Issues · 2
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
Why this result? →Sources: 68

Collection

Релятивистская — 2000/1000001, и обе дроби точны

2000/1000001

Query parameters · 3
q
question 8: the divergence of the models at small speeds under a declared tolerance
r
slow-einstein
o
observable: the ratio of the composed speed to the speed of light — a dimensionless exact fraction
Input facts · 10
  • the setting is declared: the operational conditions of the experiment are named

    s: slow
  • both frames of the setting are declared inertial

    s: slow
  • what is carried is a body with rest mass, not a light signal

    s: slow
  • the speed of the body relative to the SECOND frame along the x axis — the speed to be composed with the frame speed

    s: slowu: 299792.458 m_per_s
  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: slowv: 299792.458 m_per_s
  • the comparison tolerance for a dimensionless observable: an exact fraction declared by the setting

    s: slowo: observable: the ratio of the composed speed to the speed of light — a dimensionless exact fractiontol: 1/1000000
  • the run belongs to this theory and this setting

    rts
    slow-efirthe simple stationary luminiferous ether model in an authored reconstruction: a preferred frame, absolute time, Galilean transformations, c relative to the medium, no dragging and no contractionslow
    slow-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesslow
  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: slow-einsteinmo: slow-dvizhenie
  • §3: the Lorentz factor presented by the case; its agreement with the speed is checked by the computing package by an identity without a square root

    r: slow-einsteing: 1
Issues · 2
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
Why this result? →Sources: 68

При малых скоростях модели сближаются: при 0,001 c галилеева сумма даёт 1/500, релятивистская — 2000/1000001, и обе дроби точны.

Condition

При допуске 10⁻⁶ расхождение лежит в его пределах

Established

Query parameters · 4
q
question 8: the divergence of the models at small speeds under a declared tolerance
a
slow-efir
b
slow-einstein
o
observable: the ratio of the composed speed to the speed of light — a dimensionless exact fraction
Input facts · 10
  • the setting is declared: the operational conditions of the experiment are named

    s: slow
  • both frames of the setting are declared inertial

    s: slow
  • what is carried is a body with rest mass, not a light signal

    s: slow
  • the speed of the body relative to the SECOND frame along the x axis — the speed to be composed with the frame speed

    s: slowu: 299792.458 m_per_s
  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: slowv: 299792.458 m_per_s
  • the comparison tolerance for a dimensionless observable: an exact fraction declared by the setting

    s: slowo: observable: the ratio of the composed speed to the speed of light — a dimensionless exact fractiontol: 1/1000000
  • the run belongs to this theory and this setting

    rts
    slow-efirthe simple stationary luminiferous ether model in an authored reconstruction: a preferred frame, absolute time, Galilean transformations, c relative to the medium, no dragging and no contractionslow
    slow-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesslow
  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: slow-einsteinmo: slow-dvizhenie
  • §3: the Lorentz factor presented by the case; its agreement with the speed is checked by the computing package by an identity without a square root

    r: slow-einsteing: 1
Issues · 2
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
Why this result? →Sources: 68

Расхождение равно примерно 2·10⁻⁹, и при объявленном постановкой допуске 10⁻⁶ оно лежит в его пределах. Допуск здесь — объявленная величина постановки, а не погрешность измерения: это разные вещи, и вторая в этом расчёте не участвует.

Condition

Но «в пределах допуска» не есть «совпало»: числа разные

Not established

Query parameters · 4
q
question 8: the divergence of the models at small speeds under a declared tolerance
a
slow-efir
b
slow-einstein
o
observable: the ratio of the composed speed to the speed of light — a dimensionless exact fraction
Input facts · 10
  • the setting is declared: the operational conditions of the experiment are named

    s: slow
  • both frames of the setting are declared inertial

    s: slow
  • what is carried is a body with rest mass, not a light signal

    s: slow
  • the speed of the body relative to the SECOND frame along the x axis — the speed to be composed with the frame speed

    s: slowu: 299792.458 m_per_s
  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: slowv: 299792.458 m_per_s
  • the comparison tolerance for a dimensionless observable: an exact fraction declared by the setting

    s: slowo: observable: the ratio of the composed speed to the speed of light — a dimensionless exact fractiontol: 1/1000000
  • the run belongs to this theory and this setting

    rts
    slow-efirthe simple stationary luminiferous ether model in an authored reconstruction: a preferred frame, absolute time, Galilean transformations, c relative to the medium, no dragging and no contractionslow
    slow-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesslow
  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: slow-einsteinmo: slow-dvizhenie
  • §3: the Lorentz factor presented by the case; its agreement with the speed is checked by the computing package by an identity without a square root

    r: slow-einsteing: 1
Issues · 2
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
  • редакция urn:bipm:clir:si-brochure#SI_BROCHURE_8_EN на дату права 2026-09-08 закрыта (in_force с 2006-01-01) — 4 узлов не участвуют в вычислении (§92.3/§31, E-0095)
Why this result? →Sources: 68

«В пределах допуска» не есть «совпало»: числа разные, и совпадение предсказаний не выводится. Предельного перехода два числовых примера не доказывают, и методика его не утверждает.

How to cite

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Citation
“Что происходит с расхождением моделей при малых скоростях?”. Arxo Lens, as of 2026-09-08. https://lens.arxo.io/a/b_b77c55cf132e4f8a6e7454c04d2e1455a0d3e2ed2afc6c54842a1ba9213bf245. Snapshot SHA-256: b77c55cf132e4f8a6e7454c04d2e1455a0d3e2ed2afc6c54842a1ba9213bf245.
BibTeX
@misc{arxo-lens-b_b77c55cf132e,
  title = {Что происходит с расхождением моделей при малых скоростях?},
  howpublished = {Arxo Lens},
  url = {https://lens.arxo.io/a/b_b77c55cf132e4f8a6e7454c04d2e1455a0d3e2ed2afc6c54842a1ba9213bf245},
  note = {as of 2026-09-08; SHA-256 b77c55cf132e4f8a6e7454c04d2e1455a0d3e2ed2afc6c54842a1ba9213bf245}
}
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