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Chapter 6: Work and Kinetic Energy
Chapter 7: Potential Energy, Energy Conservation
Chapter 8: Momentum, Impulse, Collision
Chapter 6: Work and Kinetic Energy
m = mass |
g = 9.8 m/s |
F = Weight (N) |
F = m ⋅ g |
s = distance |
|
W = Workdone |
Power = P (Watts) |
x = cos y = sin |
1 km = 1000m |
1kg = 1000g |
|
Friction = always negative |
g = -9.8 (decreasing) |
g = 9.8 (normal) |
a = g (gravitational acceleration) |
Θ = Angle between F and s |
|| = Component of F parallel to dl |
v = velocity |
|
|
W = (∫P 2
to P 1
) F⋅cosΘ⋅dl |
W = F ⋅ s (Joules) |
|
P = lim Δt > 0 (ΔW / Δt) = dW / dt |
|
P = (W/t) |
Constant Speed : (a = 0) |
F = force P = F ⋅ v |
Friction (opposite) = cos(180o) |
W x
= F (cosΘ)⋅s || W y
= F (sinΘ)⋅s |
|
F s
= (1/2)⋅m⋅V f 2 - (1/2)⋅m⋅V i 2 |
|
P = (W/t) |
|
|
|
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Chapter 7: Potential Energy, Energy Conservation
|
|
K = Kinetic Energy |
R = Radius |
|
|
Δs = Δxî + Δyĵ |
|
|
k = constant of spring |
|
W grav
= w-vector ⋅ Δs-vector |
Diameter = 2 ⋅ Radius |
W f
= Work Done by Friction |
|
|
W grav
= m ⋅ g ⋅ y i
- m ⋅ g ⋅ y f
|
|
(1/2)⋅m⋅V i 2 + m⋅g⋅y i
= (1/2)⋅m⋅V f 2 + m⋅g⋅y f
|
if gravity does work.... E = K + U grav
|
W total
= K f
- K i W total
= W grav
+ W el
+ W other
|
W other
+ U i
- U f
= K f
- K i arrange to.... K i
+ U i
+ W other
= K f
+ U f
|
Work done on a spring W = (1/2)K E
⋅X f 2 - (1/2)K E
⋅X i 2 Work done by a spring W = (1/2)K E
⋅X i 2 - (1/2)K E
⋅X f 2 |
|
Elastic Potential Energy U el
= (1/2)⋅K E
⋅x 2 Work Done by Elastic Force W el
= (1/2)⋅K E
⋅x i 2 - (1/2)⋅K E
⋅x f 2 |
if elastic force does work, and mechanical energy is conserved K i
+ U el
, i
= K f
+ U el
, f
|
Work Done by Friction: W f
= -W fric
W f
= -(-f k
⋅ s) W f
= μ k
⋅m⋅g⋅s |
Law of Conservation of Energy ΔK + ΔU + ΔU int
= 0 |
F = F x
+ F y
+ F z
F x
(x) = -m⋅g F y
(y) = -m⋅g F z
(z) = -m⋅g |
|
|
|
Chapter 8: Momentum, Impulse, Collisions
p = momentum |
J = Impulse |
m = mass |
v = velocity |
P = m ⋅ v (kg ⋅ m/s) |
F = d p
/ d t J y
= (∫t f
to t i
) ΣFy dt J y
= (F av
) y
(t f
- t i
) J y
= P fy
- P iy J y
= (m⋅V fy
) - (m⋅V iy
) |
J = ΣF (t f
- t i
) J = ΣF⋅Δt J = (∫t f
to t i
) ΣF dt J x
= (∫t f
to t i
) ΣFx dt J x
= (F av
) x
(t f
- t i
) J x
= P fx
- P ix J x
= (m⋅V fx
) - (m⋅V ix
) |
ΣF = (P f
- P i
) / (t f
- t i
) |
|
J = (P f
- P i
) = {F} : Change in Momentum |
|
Assuming m 1
and m 2
don't change |
|
|
|
|
V f
= (m 1
⋅v 1
+m 2
⋅v 2
) / (m 1
++m 2
) |
|
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