Rotational Energy
Discussion
Rotational kinetic energy
For a system of point bodies
K = | 1 | ∑mivi2 |
2 |
K = | 1 | ∑ri2mi | vi2 |
2 | ri2 |
K = | 1 | Iω2 |
2 |
For an extended body
K = | 1 | ⌠ ⌡ |
v2 dm |
2 |
K = | 1 | ⌠ ⌡ |
v2 | r2 dm |
2 | r2 |
K = | 1 | ω2I |
2 |
K = | 1 | Iω2 |
2 |
Moment of inertia
I = | ⌠ ⌡ |
r2 dm = ρ | ⌠ ⌡ |
r2 dV |
Angular work
W = | ⌠ ⌡ |
F · ds |
W = | ⌠ ⌡ |
F · (dθ × r) |
W = | ⌠ ⌡ |
dθ · (r × F) |
W = | ⌠ ⌡ |
dθ · τ |
W = | ⌠ ⌡ |
τ · dθ |
and so on.
concept | translation | connection | rotation | |||
---|---|---|---|---|---|---|
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 |