Late Proterozoic and Paleozoic Tides, Retreat of the Moon, and Rotation of the Earth

The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate...

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Published inScience (American Association for the Advancement of Science) Vol. 273; no. 5271; pp. 100 - 104
Main Authors Sonett, C. P., Kvale, E. P., Zakharian, A., Chan, Marjorie A., Demko, T. M.
Format Journal Article
LanguageEnglish
Published Washington, DC American Society for the Advancement of Science 05.07.1996
American Association for the Advancement of Science
The American Association for the Advancement of Science
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Abstract The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate that the rate of retreat of the lunar orbit is dξ/dt ∼ k$_2$ sin(2δ) (where ξ is the Earth-moon radius vector, k$_2$ is the tidal Love number, and δ is the tidal lag angle) and that this rate has been approximately constant since the late Precambrian. When the contribution to tidal friction from the sun is taken into account, these data imply that the length of the terrestrial day 900 million years ago was ∼ 18 hours.
AbstractList The tidal rhythmites in Utah, Alabama, Indiana and southern Australia indicate that the rate of retreat of the lunar orbit has been approximately constant since the late Precambrian era. When the contribution to tidal friction from the sun is taken into account, these data imply that the length of the terrestrial day 900 million years ago was equivalent to 18 hours.
The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate that the rate of retreat of the lunar orbit is dξdt [similar] [k.sub.2] sin(2ξ) (where ξ is the Earth-moon radius vector, [k.sub.2] is the tidal Love number, and δ is the tidal lag angle) and that this rate has been approximately constant since the late Precambrian. When the contribution to tidal friction from the sun is taken into account, these data imply that the lenath of the terrestrial day 900 million years ago was ^18 hours.
The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate that the rate of retreat of the lunar orbit is d xi /dt similar to k sub(2) sin(2 delta ) (where xi is the Earth-moon radius vector, k sub(2) is the tidal Love number, and delta is the tidal lag angle) and that this rate has been approximately constant since the late Precambrian. When the contribution to tidal friction from the sun is taken into account, these data imply that the length of the terrestrial day 900 million years ago was similar to 18 hours.
The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate that the rate of retreat of the lunar orbit is d[xi]dt [similar] [k.sub.2] sin(2[xi]) (where [xi] is the Earth-moon radius vector, [k.sub.2] is the tidal Love number, and [delta] is the tidal lag angle) and that this rate has been approximately constant since the late Precambrian. When the contribution to tidal friction from the sun is taken into account, these data imply that the lenath of the terrestrial day 900 million years ago was ^18 hours.
The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate that the rate of retreat of the lunar orbit is dxi/dt approximately k2 sin(2delta) (where xi is the Earth-moon radius vector, k2 is the tidal Love number, and delta is the tidal lag angle) and that this rate has been approximately constant since the late Precambrian. When the contribution to tidal friction from the sun is taken into account, these data imply that the length of the terrestrial day 900 million years ago was approximately18 hours.
The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate that the rate of retreat of the lunar orbit is dξ/dt ∼ k$_2$ sin(2δ) (where ξ is the Earth-moon radius vector, k$_2$ is the tidal Love number, and δ is the tidal lag angle) and that this rate has been approximately constant since the late Precambrian. When the contribution to tidal friction from the sun is taken into account, these data imply that the length of the terrestrial day 900 million years ago was ∼ 18 hours.
The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern Australia), and the Lower Pennsylvanian Pottsville Formation (Alabama, United States) and Mansfield Formation (Indiana, United States) indicate that the rate of retreat of the lunar orbit is d ξ/ dt ∼ k 2 sin(2δ) (where ξ is the Earth-moon radius vector, k 2 is the tidal Love number, and δ is the tidal lag angle) and that this rate has been approximately constant since the late Precambrian. When the contribution to tidal friction from the sun is taken into account, these data imply that the length of the terrestrial day 900 million years ago was ∼18 hours.
Audience Academic
Author Sonett, C. P.
Chan, Marjorie A.
Kvale, E. P.
Zakharian, A.
Demko, T. M.
Author_xml – sequence: 1
  givenname: C. P.
  surname: Sonett
  fullname: Sonett, C. P.
– sequence: 2
  givenname: E. P.
  surname: Kvale
  fullname: Kvale, E. P.
– sequence: 3
  givenname: A.
  surname: Zakharian
  fullname: Zakharian, A.
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  givenname: Marjorie A.
  surname: Chan
  fullname: Chan, Marjorie A.
– sequence: 5
  givenname: T. M.
  surname: Demko
  fullname: Demko, T. M.
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ContentType Journal Article
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Issue 5271
Keywords rhythmite
length of day
Moon
rotation
Pennsylvanian
Precambrian
friction
tides
Paleozoic
sedimentary rocks
laminites
periodicity
Proterozoic
clastic rocks
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STACEY F.D. (e_1_2_1_24_2) 1977
VAUTARD R (e_1_2_1_27_2) 1992; 58
PLATZMAN G.W. (e_1_2_1_20_2) 1972; 2
BRETTHORST G.L. (e_1_2_1_4_2) 1988; 48
PUGH D.T. (e_1_2_1_21_2) 1987
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KAULA W.M. (e_1_2_1_13_2) 1968
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TAKEUCHI H (e_1_2_1_25_2) 1951; 2
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FELDMAN H.R. (e_1_2_1_10_2) 1993; 8
ALLEN C.W. (e_1_2_1_2_2) 1973
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Snippet The tidal rhythmites in the Proterozoic Big Cottonwood Formation (Utah, United States), the Neoproterozoic Elatina Formation of the Flinders Range (southern...
The tidal rhythmites in Utah, Alabama, Indiana and southern Australia indicate that the rate of retreat of the lunar orbit has been approximately constant...
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StartPage 100
SubjectTerms Angular momentum
Astronomical rotation
Earth
Earth rotation
Earth sciences
Earth, ocean, space
Earths Moon
Exact sciences and technology
Geology
History
Internal geophysics
Lunar orbits
Lunar tides
Marine
Moon
Orbits
Petrology of sedimentary rocks except quaternary rocks
Rotation
Sedimentary rocks
Semimajor axis
Solar orbits
Solid-earth geophysics, tectonophysics, gravimetry
Sun
Tides
Title Late Proterozoic and Paleozoic Tides, Retreat of the Moon, and Rotation of the Earth
URI https://www.jstor.org/stable/2890055
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