Tangential — Rotational
| ΔS
= rΔθ |
vtangential = rω |
atangential = rα |
|
Rolling
| ΔS
= Δx |
|
atangential = alinear
|
Newton?s Laws
Torque
| τ = Iα |
τ = r ×
F
|
τz = rFperpendicular
= rFsinφ = xFy −
yFx
|
Moment of Inertia
| Itotal
= I1 + I2 + I3 + … |
I = ICM + Md2
|
Work and Energy
| Wnc
= ΔK + ΔU |
W = FΔxcos(φ) |
Klinear = ½mv2
|
| Krotational = ½Iω2 |
Ugravity = mgh |
Uspring = ½Kx2
|
Collisions
| p =
mv |
|
Pf = Pi
|
v1f −
v2f = − (v1i −
v2i) |
I =ΔP
=Faveraget
|
Angular Momentum
| L = r ×
p |
Lz = xpy −
ypx = rpsinφ
|
Lfinal = Linitial
|
| Ltotal
= L1 + L2 + ? |
Llinear = bmv
|
Lorbital = r2mω
|
LA = IAωA
|
Simple Harmonic Motion
| x(t)
= Acos(ωt + δ) |
v(t) = −ωAsin(ωt
+ δ)
|
a(t) = −ω2Acos(ωt
+ δ)
|
 |
|
|
Waves
Standing Waves
If the string is fixed at both ends or air column is open at both
ends
Use
Use
If the string or air column has one open end and one fixed end
Use
Use
| yn(x,t) = Ancos(ωnt)sin(knt) |
ωn = 2πfn
|
|
Sound Level / Decibels / Sound Intensity
| Itotal = I1
+ I2 + I3 + ? |
|
|
| Itotal = I0×
10(β/10) |
I0 = 1 ×
10-12 W/m2
|
Doppler Shift
Use
Interference
Constructive interference (maximum amplitude) when Δx
= nλ, n = 1,2,3, ?
Destructive interference (zero or minimum amplitude) when
Δx
= ½nλ, n = 1,3,5, ?
Beats
fbeat = |f1 − f2|
Fluids
 |
 |
P2 = P1 + ρgΔh
|
Ainvin = Aoutvout
|
| Fbuoyant =ρfluidVdisplaced
fluidg |
P2 + ½ρ(v2)2
+ ρgh2 = P1 + ½ρ(v1)2
+ ρgh1
|
Quadratic Formula
if ax2 + bx + c = 0 ,
then
.