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Torque and Rotational Dynamics

Six topics on rotation. Rotational kinematics is the geometry of spin: how angle, angular velocity, and angular acceleration relate over time. Connecting linear and rotational motion links a point on a rotating body to the body's spin through the radius. Torque is the rotational analogue of force; rotational inertia the analogue of mass. Rotational equilibrium generalizes Newton's first law to spinning systems, and Newton's second law in rotational form predicts angular acceleration from the net torque and the rotational inertia.

Topics
Equations For every problem in this unit
Angular velocity (constant $\alpha$)
$\omega = \omega_0 + \alpha t$
Angular displacement (constant $\alpha$)
$\theta = \omega_0 t + \tfrac{1}{2} \alpha t^2$
Squared form (constant $\alpha$)
$\omega^2 = \omega_0^2 + 2 \alpha \theta$
Linear-rotational speed link
$v = r \omega$
Tangential acceleration
$a_t = r \alpha$
Centripetal acceleration
$a_c = r \omega^2 = \dfrac{v^2}{r}$
Torque magnitude
$\tau = r F \sin\theta$
Newton's 2nd law (rotational)
$\Sigma \tau = I \alpha$
Rotational kinetic energy
$K_{\text{rot}} = \tfrac{1}{2} I \omega^2$
Angular momentum
$L = I \omega$
Rotational impulse
$\Delta L = \tau \, \Delta t$
Point mass at radius $r$
$I = m r^2$
Hoop or thin cylindrical shell (about axis)
$I = M R^2$
Solid disk or cylinder (about axis)
$I = \tfrac{1}{2} M R^2$
Solid sphere (about diameter)
$I = \tfrac{2}{5} M R^2$
Thin spherical shell (about diameter)
$I = \tfrac{2}{3} M R^2$
Thin rod (axis through center, perpendicular)
$I = \tfrac{1}{12} M L^2$
Thin rod (axis through end, perpendicular)
$I = \tfrac{1}{3} M L^2$
Parallel-axis theorem
$I = I_{\text{cm}} + M d^2$
Pythagorean
$a^2 + b^2 = c^2$
Sine, opp / hyp
$\sin\theta = \dfrac{a}{c}$
Cosine, adj / hyp
$\cos\theta = \dfrac{b}{c}$
Tangent, opp / adj
$\tan\theta = \dfrac{a}{b}$
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