|
Rotational kinetic energy
| Translational and Rotational Quantities Compared | ||||||
| translational | connections | rotational | ||||
|---|---|---|---|---|---|---|
| work-energy | W = |
∫ F · ds |
W = |
∫ τ · dθ |
||
| kinetic energy | K = |
½mv2 |
K = |
½Iω2 |
||
| potential energy | U = F(x) = |
− ∫ F · ds − dU/dx |
U = τ(θ) = |
− ∫ τ · dθ − dU/dθ |
||
| power | P = |
F · v |
P = |
τ · ω | ||
For a system of point bodies
| K = | 1 | ∑ mivi2 = | 1 | ∑ ri2mi | vi2 | = | 1 | Iω2 |
| 2 | 2 | ri2 | 2 |
For an extended body
| K = | 1 | ⌠ ⌡ |
v2 dm = | 1 | ⌠ ⌡ |
v2 | r2 dm = | 1 | ω2I = | 1 | Iω2 |
| 2 | 2 | r2 | 2 | 2 |
Moment of inertia
| I = ∑r2m = | ⌠ ⌡ |
r2 dm = ρ | ⌠ ⌡ |
r2 dV |
Angular work
| W = | ⌠ ⌡ |
F · ds = | ⌠ ⌡ |
F · (dθ × r) = | ⌠ ⌡ |
dθ · (r × F) = | ⌠ ⌡ |
dθ · τ = | ⌠ ⌡ |
τ · dθ |
and so on