Clairaut's theorem characterizes the surface gravity on a viscous rotating ellipsoid held in hydrostatic equilibrium by the combined action of its own gravitational field and centrifugal force. Alexis Claude Clairaut published it in 1743 in a treatise that synthesized physical and geodetic evidence that the Earth is an oblate ellipsoid, and it was initially used to relate the gravity at any point on the Earth's surface to that point's position, allowing the planet's flattening to be calculated from gravity measurements taken at different latitudes; today it has largely been superseded by the Somigliana equation.
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Source Clairaut's theorem (gravity) (Wikipedia)
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Source Clairaut's theorem, Wikipedia
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1. Clairaut's theorem, Wikipedia
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In it, he promulgated what is more formally known today as Clairaut's theorem.
Proved By: Alexis Claude Clairaut, Lead section
It was published in 1743 by Alexis Claude Clairaut in a treatise which synthesized physical and geodetic evidence that the Earth is an oblate ellipsoid.
View the SourceClairaut's theorem (gravity) (Wikipedia)
In Group: Classical Mechanics and Dynamics, Lead section
in hydrostatic equilibrium under the action of its gravitational field and centrifugal force. It was published
In Branch: Mathematical Physics, Lead section
Clairaut's theorem characterizes the surface gravity on a viscous rotating ellipsoid in hydrostatic
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