Linear/translational quantities |
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Angular/rotational quantities |
Dimensions |
1 |
L |
L2 |
Dimensions |
1 |
θ |
θ2 |
T |
time: t s |
absement: A m s |
|
T |
time: t s |
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|
1 |
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distance: d, position: r, s, x, displacement m |
area: A m2 |
1 |
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angle: θ, angular displacement: θ rad |
solid angle: Ω rad2, sr |
T−1 |
frequency: f s−1, Hz |
speed: v, velocity: v m s−1 |
kinematic viscosity: ν, specific angular momentum: h m2 s−1 |
T−1 |
frequency: f, rotational speed: n, rotational velocity: n s−1, Hz |
angular speed: ω, angular velocity: ω rad s−1 |
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T−2 |
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acceleration: a m s−2 |
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T−2 |
rotational acceleration s−2 |
angular acceleration: α rad s−2 |
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T−3 |
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jerk: j m s−3 |
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T−3 |
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angular jerk: ζ rad s−3 |
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M |
mass: m kg |
weighted position: M ⟨x⟩ = ∑ m x |
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ML2 |
moment of inertia: I kg m2 |
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MT−1 |
Mass flow rate: <math>\dot{m}</math> kg s−1 |
momentum: p, impulse: J kg m s−1, N s |
action: 𝒮, actergy: ℵ kg m2 s−1, J s |
ML2T−1 |
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angular momentum: L, angular impulse: ΔL kg m2 s−1 |
action: 𝒮, actergy: ℵ kg m2 s−1, J s |
MT−2 |
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force: F, weight: Fg kg m s−2, N |
energy: E, work: W, Lagrangian: L kg m2 s−2, J |
ML2T−2 |
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torque: τ, moment: M kg m2 s−2, N m |
energy: E, work: W, Lagrangian: L kg m2 s−2, J |
MT−3 |
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yank: Y kg m s−3, N s−1 |
power: P kg m2 s−3, W |
ML2T−3 |
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rotatum: P kg m2 s−3, N m s−1 |
power: P kg m2 s−3, W |