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Advanced Rotational Dynamics for AP Physics. +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws
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Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Examples of rotation: Earth To find the direction of omega, apply the right hand rule as follows: With fingers curling in direction of rotation, the thumb gives direction of omega i.e. direction of earth’s omega is upward
rotation of the sky star trails centered on Polaris rotate once a day
sometimes the goal is rotational equilibrium • 1st condition for equilibrium: Fnet = 0 • 2nd condition for equilbrium: torque net = 0 • i.e., torque ccw = torque cw
a generic kidney shaped object rotates about a fixed axis:a thing of beauty is a joy forever!
a turbine (driven by moving fluid) rotates about a fixed axis
steam driven power plant turbine:imagine this thing rotating at 60 hzgenerating your electricity
electric motors are backwards connected generators:they are still mechanical rotators about a fixed axis
gear attached to an electric motor(sounds like a good idea to me)
nanotechology electric motor gear (the gear teeth are smaller than a red blood cell)rotating about a fixed axis, imaged with an electron microscope(end of examples of rotation)
Advanced Rotational Dynamicsfor AP Physics +Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Rotational Kinematics • Θ = angular position wrt arbitrary origin • Δθ = angular displacement (rad) • ω = Δθ / Δt = dθ / dt (rad/s) • α = Δ ω / Δt = d ω / dt = d2θ / dt2 (rad/s2) • s = r θ • v = r ω • a = r α
α = constant implies • Δθ = ω0t + ½ αt2 • ω = ω0 + α t • ω2 = ω02 + 2 αΔθ • Δθ = ½ (ω0 + ω) t • If α is variable, you need calculus
Intro Rotational Dynamics • Г = τ = r x F • I = Σ mi ri2 (collection of point masses) = ∫ r2 dm (continuous matter distribution) • I total = I 1 + I 2 + I 3 + … (composite object) • Fnet = ma becomes Гnet = τnet = I α
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
combined translation and rotation Ktotal = Ktranslational + Krotational = Kof the cm + Karound the cm = ½ mv2 + ½ I ω2
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
linear and angular velocity and acceleration are proportional
rolling without slipping • v = ω r (use with energy conservation) • atangential = α r (use with 2nd laws) • friction acts, but does no work • energy conserved as Wnc = 0
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping (pure rolling) +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping (pure rolling) +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping (pure rolling) +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
linear and angular velocities and accelerations are independent,i.e., he’s not getting very much bang (v) for his buck (ω)
rolling with slipping • v ≠ω r • atangential≠α r • apply Fnet = ma to find atangential of the cm • apply Гnet = Iα to find α around the cm • to compute t where pure rolling sets in, set a(t) = α(t) r, where a(t) and α(t) are solutions of force and torque equations
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia
Advanced Rotational Dynamicsfor AP Physics +Common Examples of Rotation +Review of Introductory Rotational Dynamics +Combined translation and rotation +Rolling without slipping +Rolling with slipping +Rotational form of Conservation Laws +Collisions involving objects having Moment of Inertia