* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Part VI
Rolling resistance wikipedia , lookup
Modified Newtonian dynamics wikipedia , lookup
Center of mass wikipedia , lookup
Eigenstate thermalization hypothesis wikipedia , lookup
Classical mechanics wikipedia , lookup
Equations of motion wikipedia , lookup
Internal energy wikipedia , lookup
Seismometer wikipedia , lookup
Electromagnetic mass wikipedia , lookup
Thermodynamic temperature wikipedia , lookup
Classical central-force problem wikipedia , lookup
Work (thermodynamics) wikipedia , lookup
Rotational spectroscopy wikipedia , lookup
Mass versus weight wikipedia , lookup
Centripetal force wikipedia , lookup
Rigid body dynamics wikipedia , lookup
Hunting oscillation wikipedia , lookup
Newton's laws of motion wikipedia , lookup
Section 10.8: Energy in Rotational Motion Translation-Rotation Analogues & Connections Translation Rotation Displacement x θ Velocity v ω Acceleration a α Force (Torque) F τ Mass (moment of inertia) m I Newton’s 2nd Law ∑F = ma ∑τ = Iα Kinetic Energy (KE) (½)mv2 (½)Iω2 CONNECTIONS: v = rω, atan= rα aR = (v2/r) = ω2r , τ = rF , I = ∑(mr2) • Work done by force F on an object as it rotates through an infinitesimal distance ds = rdθ dW = Fds = (Fsinφ)rdθ dW = τdθ • The radial component of F does no work because it is perpendicular to the displacement. Power • The rate at which work is being done in a time interval Δt is • This is analogous to P = Fv for translations. Work-Kinetic Energy Theorem • The work-kinetic energy theorem in rotational language states that the net work done by external forces in rotating a symmetrical rigid object about a fixed axis equals the change in the object’s rotational kinetic energy Ex. 10.11: Rod Again Sect. 10.9 Rolling Objects • The curve shows the path moved by a point on the rim of the object. This path is called a cycloid • The line shows the path of the center of mass of the object • In pure rolling motion, an object rolls without slipping • In such a case, there is a simple relationship between its rotational and translational motions Rolling Object The velocity of the center of mass is The acceleration of the center of mass is • A point on the rim, P, rotates to various positions such as Q and P. At any instant, a point P on the rim is at rest relative to the surface since no slipping occurs • Rolling motion is thus a combination of pure translational motion and pure rotational motion Total Kinetic Energy • The total kinetic energy of a rolling object is the sum of the translational energy of its center of mass and the rotational kinetic energy about its center of mass K = (½)Mv2 + (½)Iω2 • Accelerated rolling motion is possible only if friction is present between the sphere and the incline Example: Sphere rolls down incline (no slipping or sliding). v = 0 KE+PE conservation: ω = 0 (½)Mv2 + (½)Iω2 +MgH = constant, or (KE)1 +(PE)1 = (KE)2 + (PE)2 where KE has 2 parts: (KE)trans = (½)Mv2 (KE)rot = (½)Iω2 v=? y=0 Summary of Useful Relations Translation-Rotation Analogues & Connections Translation Rotation Displacement x θ Velocity v ω Acceleration a α Force (Torque) F τ Mass (moment of inertia) m I Newton’s 2nd Law ∑F = ma ∑τ = Iα Kinetic Energy (KE) (½)mv2 (½)Iω2 CONNECTIONS: v = rω, atan= rα aR = (v2/r) = ω2r , τ = rF , I = ∑(mr2) Ex. 10.12: Energy & Atwood Machine