About: Rotating spheres

Facets (new session)
Description
Metadata
Settings
- Rule:
- Inverse Functional Properties:
- "Same As":

About: Rotating spheres Goto Sponge NotDistinct Permalink

An Entity of Type : yago:ScientificResearch100641820, within Data Space : dbpedia.demo.openlinksw.com associated with source document(s)
QRcode icon

http://dbpedia.demo.openlinksw.com/c/5FYmWCQxyR

Isaac Newton's rotating spheres argument attempts to demonstrate that true rotational motion can be defined by observing the tension in the string joining two identical spheres. The basis of the argument is that all observers make two observations: the tension in the string joining the bodies (which is the same for all observers) and the rate of rotation of the spheres (which is different for observers with differing rates of rotation). Only for the truly non-rotating observer will the tension in the string be explained using only the observed rate of rotation. For all other observers a "correction" is required (a centrifugal force) that accounts for the tension calculated being different from the one expected using the observed rate of rotation. It is one of five arguments from the "prope

Attributes	Values
rdf:type	Thing yago:WikicatThoughtExperimentsInPhysics yago:Abstraction100002137 yago:Act100030358 yago:Activity100407535 yago:Event100029378 yago:Experiment100639556 yago:Investigation100633864 yago:PsychologicalFeature100023100 yago:Research100636921 yago:Work100575741 yago:YagoPermanentlyLocatedEntity yago:ScientificResearch100641820
rdfs:label	Rotating spheres (en)
rdfs:comment	Isaac Newton's rotating spheres argument attempts to demonstrate that true rotational motion can be defined by observing the tension in the string joining two identical spheres. The basis of the argument is that all observers make two observations: the tension in the string joining the bodies (which is the same for all observers) and the rate of rotation of the spheres (which is different for observers with differing rates of rotation). Only for the truly non-rotating observer will the tension in the string be explained using only the observed rate of rotation. For all other observers a "correction" is required (a centrifugal force) that accounts for the tension calculated being different from the one expected using the observed rate of rotation. It is one of five arguments from the "prope (en)
rdfs:seeAlso	Bucket argument
foaf:depiction
dcterms:subject	Thought experiments in physics Classical mechanics Isaac Newton
Wikipage page ID	19975340 (xsd:integer)
Wikipage revision ID	1122847476 (xsd:integer)
Link from a Wikipage to another Wikipage	Thought experiments in physics Argument Right-hand rule Uniform circular motion Mechanics of planar particle motion Geodesics in general relativity General relativity Coriolis force Cosmic background radiation Operational definition Ignazio Ciufolini Rotation around a fixed axis Mach's principle Space Ad hoc Centripetal force Wilkinson Microwave Anisotropy Probe Fictitious force Globe Gravitron Isaac Newton Absolute rotation Absolute space Classical mechanics John Archibald Wheeler Isaac Newton Plane of rotation Spacetime Tension (mechanics) Bucket argument Centrifugal force (rotating reference frame) Reactive centrifugal force Fixed stars Sagnac effect
sameAs	Rotating spheres Rotating spheres Rotating spheres Rotating spheres
dbp:wikiPageUsesTemplate	dbt:Div_col dbt:Div_col_end dbt:Main dbt:Quotation dbt:Reflist dbt:See_also dbt:Isaac_Newton
thumbnail	wiki-commons:Special:FilePath/Rotating_spheres.svg?width=300
has abstract	Isaac Newton's rotating spheres argument attempts to demonstrate that true rotational motion can be defined by observing the tension in the string joining two identical spheres. The basis of the argument is that all observers make two observations: the tension in the string joining the bodies (which is the same for all observers) and the rate of rotation of the spheres (which is different for observers with differing rates of rotation). Only for the truly non-rotating observer will the tension in the string be explained using only the observed rate of rotation. For all other observers a "correction" is required (a centrifugal force) that accounts for the tension calculated being different from the one expected using the observed rate of rotation. It is one of five arguments from the "properties, causes, and effects" of true motion and rest that support his contention that, in general, true motion and rest cannot be defined as special instances of motion or rest relative to other bodies, but instead can be defined only by reference to absolute space. Alternatively, these experiments provide an operational definition of what is meant by "absolute rotation", and do not pretend to address the question of "rotation relative to what?" General relativity dispenses with absolute space and with physics whose cause is external to the system, with the concept of geodesics of spacetime. (en)
prov:wasDerivedFrom	wikipedia-en:Rotating_spheres?oldid=1122847476&ns=0
page length (characters) of wiki page	24037 (xsd:nonNegativeInteger)
foaf:isPrimaryTopicOf	wikipedia-en:Rotating_spheres
is rdfs:seeAlso of	Absolute rotation
is Link from a Wikipage to another Wikipage of	Index of physics articles (R) Mechanics of planar particle motion Coriolis force Centrifugal force Fictitious force Absolute space and time Inertial frame of reference Bucket argument List of things named after Isaac Newton Non-inertial reference frame
is foaf:primaryTopic of	wikipedia-en:Rotating_spheres

Faceted Search & Find service v1.17_git147 as of Sep 06 2024

Alternative Linked Data Documents: ODE Content Formats:

RDF

ODATA

Microdata

About

OpenLink Virtuoso version 08.03.3332 as of Dec 5 2024, on Linux (x86_64-generic-linux-glibc212), Single-Server Edition (378 GB total memory, 76 GB memory in use)
Data on this page belongs to its respective rights holders.
Virtuoso Faceted Browser Copyright © 2009-2025 OpenLink Software