One of the most beautiful things in mechanics is that the laws of rotation have exactly the same structure as those of translation. It is not an approximate resemblance: it is a perfect translation dictionary, where every translational quantity has a rotational counterpart that inherits all its properties.

The translation ↔ rotation dictionary

TranslationRotationRelation
Position ssAngle θ\thetas=rθs = r\theta
Velocity vvAngular velocity ω\omegav=rωv = r\omega
Acceleration aaAngular acceleration α\alphaat=rαa_t = r\alpha
Mass mmMoment of inertia III=miri2I = \sum m_i r_i^2
Force F\vec{F}Moment MMM=FrsinθM = Fr\sin\theta
F=ma\sum F = maM=Iα\sum M = I\alpha
p=mv\vec{p} = m\vec{v}L=IωL = I\omega
Ecin=12mv2E_\text{cin} = \tfrac{1}{2}mv^2Ecin,rot=12Iω2E_\text{cin,rot} = \tfrac{1}{2}I\omega^2
Impulse I\vec{I}Angular impulse IangI_\text{ang}

The equations of uniformly accelerated rotational motion

Since θ\theta, ω\omega, α\alpha stand to ss, vv, aa as their twins, the equations of motion for uniformly accelerated rotation with α\alpha constant are the same as for uniformly accelerated straight-line motion, word for word:

θBθA=ωA(tBtA)+12α(tBtA)2\theta_B - \theta_A = \omega_A(t_B-t_A) + \tfrac{1}{2}\alpha(t_B-t_A)^2

ωBωA=α(tBtA)\omega_B - \omega_A = \alpha(t_B - t_A)

ωB2ωA2=2α(θBθA)\omega_B^2 - \omega_A^2 = 2\alpha(\theta_B - \theta_A)

There is nothing new to learn: you just swap the symbols. Whoever has understood straight-line kinematics has already understood, for free, rotational kinematics.

An analogy that never ends

The analogy is so deep that every theorem of translational mechanics has a rotational counterpart: conservation of momentum p\vec{p} becomes conservation of angular momentum LL, the impulse theorem becomes the angular impulse theorem, and even the Atwood machine has a rotational analogue with massive pulleys. Every time you meet a formula for a rotating body, try to recognise which translational formula is “redoing its make-up” in angular coordinates.

Collegamenti

Argomenti: Dinamica rotazionale Concetti: Momento angolare · Energia cinetica rotazionale Metodi: Analogia traslazione-rotazione

Esercizi collegati: Esercizio svolto — sfera che rotola giù da un piano · Problema — Momento torcente rettangolare e L(t) · Problema — Asta incernierata che cade dall’orizzontale