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Какое смещение полос ожидала каждая модель в опыте Майкельсона и Морли?

По параметрам самой статьи модель эфира ожидает 2/5 полосы — то самое «0•4 fringe», которое называют авторы, — а Лоренц и СТО ожидают ноль, и каждый по своему основанию.

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

Results

5

Collection

Длина волны выведена из двух чисел статьи: 11 м есть 2·10⁷ длин волн

0.00000055 m

Query parameters · 1
s
mm
Input facts · 9

  • the setting is declared: the operational conditions of the experiment are named

    s: mm

  • the setting is declared to be the Michelson–Morley experiment of 1887: its parameters are taken from the pinned bytes of the article

    s: mm

  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: mmv: 29979.2458 m_per_s

  • the run belongs to this theory and this setting

    rts
    mm-efirClassicalEthermm
    mm-lorentzLorentz's electrodynamics of moving bodies in the 1904 formulation: a stationary aether, local time as an auxiliary variable, contraction of bodies and altered molecular forcesmm
    mm-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesmm

  • §4: the factor k presented by the case; defined by k² = c²/(c² − w²), an identity verifiable without a square root

    r: mm-lorentzk: 1

  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: mm-einsteinmo: mm-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: mm-einsteing: 1
Why this result? →Sources: 28

Постановка берётся из закреплённых байтов статьи, а не придумывается: плечо около одиннадцати метров, оно же двадцать миллионов длин волн жёлтого света, квадрат отношения скоростей 10⁻⁸. Длина волны числом не названа и ВЫВОДИТСЯ делением одного числа статьи на другое.

Collection

Эфир ожидает 2/5 полосы — то самое «0•4 fringe» статьи

2/5

Query parameters · 3
q
question 5: the interferometer with two perpendicular arms
r
mm-efir
o
observable: the shift of the interference fringes on turning the apparatus through a right angle, in fringe widths
Input facts · 9

  • the setting is declared: the operational conditions of the experiment are named

    s: mm

  • the setting is declared to be the Michelson–Morley experiment of 1887: its parameters are taken from the pinned bytes of the article

    s: mm

  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: mmv: 29979.2458 m_per_s

  • the run belongs to this theory and this setting

    rts
    mm-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 contractionmm
    mm-lorentzLorentz's electrodynamics of moving bodies in the 1904 formulation: a stationary aether, local time as an auxiliary variable, contraction of bodies and altered molecular forcesmm
    mm-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesmm

  • §4: the factor k presented by the case; defined by k² = c²/(c² − w²), an identity verifiable without a square root

    r: mm-lorentzk: 1

  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: mm-einsteinmo: mm-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: mm-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: 74

Расчёт идеализирован: два перпендикулярных плеча равной длины, свет распространяется в пустоте, установка неподвижна относительно лаборатории. Историческая установка со сложенным ходом луча и стеклянными пластинами к этому расчёту не сводится, и выводы о ней требуют дополнительных условий.

Collection

И это же число называют сами авторы — как своё ВЫЧИСЛЕНИЕ

2/5

Query parameters · 1
s
mm
Input facts · 9

  • the setting is declared: the operational conditions of the experiment are named

    s: mm

  • the setting is declared to be the Michelson–Morley experiment of 1887: its parameters are taken from the pinned bytes of the article

    s: mm

  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: mmv: 29979.2458 m_per_s

  • the run belongs to this theory and this setting

    rts
    mm-efirClassicalEthermm
    mm-lorentzLorentz's electrodynamics of moving bodies in the 1904 formulation: a stationary aether, local time as an auxiliary variable, contraction of bodies and altered molecular forcesmm
    mm-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesmm

  • §4: the factor k presented by the case; defined by k² = c²/(c² − w²), an identity verifiable without a square root

    r: mm-lorentzk: 1

  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: mm-einsteinmo: mm-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: mm-einsteing: 1
Why this result? →Sources: 28

Модель эфира ожидает ровно 2/5 полосы, и это же число называют сами авторы как своё вычисление. Совпадение здесь — сверка расчёта, а не подгонка: формула пакета получает его из параметров статьи.

Эфир ожидает 2/5 полосы — то самое «0•4 fringe» статьи

Collection

Лоренц ожидает ноль — гипотезы §8 гасят разность времён

0

Query parameters · 3
q
question 5: the interferometer with two perpendicular arms
r
mm-lorentz
o
observable: the shift of the interference fringes on turning the apparatus through a right angle, in fringe widths
Input facts · 9

  • the setting is declared: the operational conditions of the experiment are named

    s: mm

  • the setting is declared to be the Michelson–Morley experiment of 1887: its parameters are taken from the pinned bytes of the article

    s: mm

  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: mmv: 29979.2458 m_per_s

  • the run belongs to this theory and this setting

    rts
    mm-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 contractionmm
    mm-lorentzLorentz's electrodynamics of moving bodies in the 1904 formulation: a stationary aether, local time as an auxiliary variable, contraction of bodies and altered molecular forcesmm
    mm-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesmm

  • §4: the factor k presented by the case; defined by k² = c²/(c² − w²), an identity verifiable without a square root

    r: mm-lorentzk: 1

  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: mm-einsteinmo: mm-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: mm-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: 74

Collection

СТО ожидает ноль — скорость света одна во всех направлениях

0

Query parameters · 3
q
question 5: the interferometer with two perpendicular arms
r
mm-einstein
o
observable: the shift of the interference fringes on turning the apparatus through a right angle, in fringe widths
Input facts · 9

  • the setting is declared: the operational conditions of the experiment are named

    s: mm

  • the setting is declared to be the Michelson–Morley experiment of 1887: its parameters are taken from the pinned bytes of the article

    s: mm

  • the speed of the second frame relative to the laboratory along the x axis; the sign is the direction of the transition

    s: mmv: 29979.2458 m_per_s

  • the run belongs to this theory and this setting

    rts
    mm-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 contractionmm
    mm-lorentzLorentz's electrodynamics of moving bodies in the 1904 formulation: a stationary aether, local time as an auxiliary variable, contraction of bodies and altered molecular forcesmm
    mm-einsteinspecial relativity in the 1905 formulation: an operational definition of simultaneity, two principles, the transformation of coordinates and time, the composition of velocitiesmm

  • §4: the factor k presented by the case; defined by k² = c²/(c² − w²), an identity verifiable without a square root

    r: mm-lorentzk: 1

  • the relative motion of the two frames to which the computing package will refer the quantities of this run

    r: mm-einsteinmo: mm-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: mm-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: 74

Лоренц и СТО ожидают ноль по РАЗНЫМ основаниям: у первого плечо вдоль движения укорачивается ровно настолько, чтобы скомпенсировать разность времён; у второго разности времён не возникает вовсе, потому что скорость света в лаборатории одна во всех направлениях.

Лоренц ожидает ноль — гипотезы §8 гасят разность времён

How to cite

The snapshot is immutable: the SHA-256 of the downloadable JSON pins it, so no access date is needed.

Citation
“Какое смещение полос ожидала каждая модель в опыте Майкельсона и Морли?”. Arxo Lens, as of 2026-09-08. https://lens.arxo.io/a/b_239856525a226801bb8dc2e6885a5901a41348110a0f002458ae6963c67b10ca. Snapshot SHA-256: 239856525a226801bb8dc2e6885a5901a41348110a0f002458ae6963c67b10ca.
BibTeX
@misc{arxo-lens-b_239856525a22,
  title = {Какое смещение полос ожидала каждая модель в опыте Майкельсона и Морли?},
  howpublished = {Arxo Lens},
  url = {https://lens.arxo.io/a/b_239856525a226801bb8dc2e6885a5901a41348110a0f002458ae6963c67b10ca},
  note = {as of 2026-09-08; SHA-256 239856525a226801bb8dc2e6885a5901a41348110a0f002458ae6963c67b10ca}
}
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