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| Equations Of Motion |
v = v0 + at
x = x0 + v0t + ½at2
v2 = v02 + 2a(x − x0) v̅ = ½(v + v0)
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| Newton's 2nd Law |
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∑ F = m a
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| Dry Friction |
ƒ μN
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Centripetal Accel. |
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ac = − ω2r
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Impulse |
J = Δt
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| J = |  | F dt |
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| Impulse-Momentum |
Δt = mΔv
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 | F dt = Δp |
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Work |
W = Δs cos θ
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| W = |  | F · ds |
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Work-Energy |
Δs cos θ = ΔE
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 | F · ds = ΔE |
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| General Potential Energy |
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| ΔU = − |  | F · ds |
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F = − ∇U
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Gravitational Potential Energy |
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ΔUg = mgΔh
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Power |
= |
ΔW | | Δt |
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Power-Velocity
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= v cos θ
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P = F · v
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Angular Velocity |
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v = ω × r
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Angular Acceleration |
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a = α × r − ω2 r
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Equations Of Rotation |
ω = ω0 + αt
θ = θ0 + ω0t + ½αt2
ω2 = ω02 + 2α(θ − θ0)
ω̅ = ½(ω + ω0)
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Newton's second law of rotational motion |
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∑ τ = I α
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| Torque |
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τ = rF sin θ
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τ = r × F
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| Moment Of Inertia |
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I = ∑ mr2
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| I = |
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Rotational Motion |
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W = τ̅Δθ
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| W = |
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Rotational power |
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P = τω cos θ
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P = τ · ω
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| Rotational Kinetic Energy |
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K = ½Iω2
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| Angular Momentum |
L = mrv sin θ
L = r × p
L = I ω
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| Newton's Law Of Universal Gravitation |
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Gravitational Field Surrounding a Point Mass |
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Potential Energy Surrounding a Point Mass |
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| Gravitational Potential Surrounding a Point Mass |
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Elastic Potential Energy |
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Us = ½kΔx2
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| Period of a Simple Harmonic Oscillator |
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| Period of a Simple Pendulum |
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Angular-Linear Frequency Relation |
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| ω = 2pƒ |
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| Pressure-Depth Relation for a Fluid of Uniform Density |
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P = P0 + ρgh
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Archimedes' Law of Buoyancy |
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B = ρgVdisplaced
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Mass Continuity |
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ρ1A1v1 = ρ2A2v2
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Volume Continuity |
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A1v1 = A2v2
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| Bernoulli's Equation |
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P1 + ρgy1 + ½ρv12 =
P2 + ρgy2 + ½ρv22 |
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| Dynamic Viscosity |
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Δvx | | A | Δz |
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