Show that the acceleration of any object down an incline where friction behaves simply (that is, where fk = μk N) is a = g(sin θ − μk cos θ). Note that the acceleration is independent of mass and reduces to the expression found in the previous problem when friction becomes negligibly small (μk = 0)
Show that the acceleration of any object down an incline where friction behaves simply (that is, where fk = μk N) is a = g(sin θ − μk cos θ). Note that the acceleration is independent of mass and reduces to the expression found in the previous problem when friction becomes negligibly small (μk = 0)
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Show that the acceleration of any object down an
incline where friction behaves simply (that is, where
fk = μk N) is a = g(sin θ − μk cos θ). Note that the
acceleration is independent of mass and reduces to the
expression found in the previous problem when friction
becomes negligibly small (μk = 0).
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