PDF-Mechanics2.8.FrictionConsideraparticleofmassM,whichisona
Author : test | Published Date : 2016-12-21
rough horizontalplaneGivenahorizontalforceofmagnitudeSisappliedasinFigure1thenassumingtheparticleremainsinequilibriumthemagnitudeofthe frictionalforce FopposinganymotionwillbeequaltoSieFS
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Mechanics2.8.FrictionConsideraparticleofmassM,whichisona: Transcript
rough horizontalplaneGivenahorizontalforceofmagnitudeSisappliedasinFigure1thenassumingtheparticleremainsinequilibriumthemagnitudeofthe frictionalforce FopposinganymotionwillbeequaltoSieFS. F=ma ,onpar-ticleB,inthedirectionofmotion(#),gives:8g T=8a(1)UsingNewton'ssecondlaw, F=ma ,onpar-ticleC,inthedirectionofmotion("),gives:T 2g=2a(2) TTBC Thesimultaneousequations(1)and(2)cannowbesolved. F=R Mgsin=MgcosMgsin Mgcos=tan=Note:tan=sin cos MgRF q Figure1Thiscanbewrittenas=arctan;isreferredtoasthe AngleofFriction .WorkedExample2.Aboxofmass6kgisonthepointofslippingdownaroughs Nature of science: . Observations: The ideas of motion are fundamental to many areas of physics, providing a link to the consideration of forces and their implication. The kinematic equations for uniform acceleration were developed through careful observations of the natural world.. Nature of science: . Theories: Many phenomena can be fundamentally understood through application of the theory of conservation of energy. Over time, scientists have utilized this theory both to explain natural phenomena and, more importantly, to predict the outcome of previously unknown interactions. The concept of energy has evolved as a result of recognition of the relationship between mass and energy..
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