Physics, Page 1
Chapter 10.
Chapter 10. Rotation ( Rotation ( 회전 회전 ) )
¾ 회전운동 변수들
z각도(θ), 각변위(Δθ), 각속도(ω) , 각가속도(α)
¾ 회전 운동에너지
¾ 회전관성 (관성모멘트, moment of inertia)
¾ 돌림힘 (Torque)
Review of last lecture Review of last lecture
FaveΔt ≡ J = pf - pi = Δp
¾ 충격량 - 선운동량 정리 (Impulse-Momentum Theorem)
¾ 단일 입자인 경우 …
If F = 0, then momentum conserved (Δp = 0)
¾ 여러 입자 계인 경우 …
tf ( )
ti
Ptotal ≡ Σpi
Internal forces: forces between objects in system External forces: all other forces
FextΔt = ΔPtotal
if Fext = 0 , then total momentum conserved (ΔPtotal = 0)
¾ 탄성충돌 (운동량, 운동에너지 보존) 비 탄성충돌 (운동량만 보존) J ≡
∫
F t dt = Δpur ur ur
F d p
= dt ur ur
Physics, Page 3
변수비교
병진운동 (linear motion)
회전운동
(angular motion)
변위 (displacement) x m θ
ω α
I (1/2)Iω2
τ = Iα
- (rad)
속도 (velocity) v
m(r x v)
rad /s 가속도 (acceleration) a
m/s m/s2
kg J N
rad/s2
관성 (inertia) m kg.m2
운동에너지 (KE) (1/2)mv2 J
운동방정식 (Newton’s 2nd) F = ma N.m
N.s
모멘텀 (momentum) mv J.s
Physics, Page 5
(부호 약속 : 반시계 방향 +, 시계방향 -)
Comment on axes and sign of angle Comment on axes and sign of angle
(i.e. what is positive and negative) (i.e. what is positive and negative)
Whenever we talk about rotation, it is implied that there is a rotation “axis”.
This is usually called the “z” axis (we usually omit the z subscript for simplicity).
Counter-clockwise (increasing θ) is usually called positive.
Clockwise (decreasing θ) is usually called negative.
z
+ω
Physics, Page 7
(선변수와 각변수의 관계)
r s at
v ar
즉즉, , 가속도의가속도의관점만관점만 다르다다르다..
ar = rω2 ÅÆ at = αr
* 지름방향
Physics, Page 9
1 2 2
2 2
1 2
1 2 2
2 ( )
( )
o
o o
o o
o o
o
t
t t
t t t
ω ω α
θ θ ω α ω ω α θ θ θ θ ω ω θ θ ω
= +
= + +
= + −
= + +
= + −
( , , ; )
angular t θ ω α
1 2 2
2 2
1 2
1 2 2
2 ( )
( )
o
o o
o o
o o
o
v v at
x x v t at
v v a x x
x x v v t
x x vt t
= +
= + +
= + −
= + +
= + −
( , , ; )
linear x v a t
Physics, Page 11
(= 관성모멘트)
보기문제 : Oxygen Molecule
d
( )
12 2( )
21 2 46 22 m d m d 1.95 10 kg m
r m
I = ∑i i i = i + i = × − ⋅
d = 1.21 × 10-10m mi = 2.66 × 10-26 kg
ω = 4.6 × 1012rad/sec.
J I
K = 21
ω
2 = 2.06×10−21x
회전운동에너지 회전운동에너지
? ?
Physics, Page 13
Inertia rods
Two batons have equal mass and length.
Which will be “easier” to spin?
A) Mass on ends B) Same
C) Mass in center
I = Σ m r2 Further mass is from axis of rotation, greater moment of inertia (harder to spin)
21
회전관성 회전관성 ( ( 관성모멘트 관성모멘트 ) ) 계산법 계산법
{ } { }
2
2 2
2 2 2 2
2 2 2 2
2
( ) ( )
( ) 2 2 ( )
( ) ( )
P
CM
I r dm
x a y b dm
x y dm a xdm b ydm a b dm x y dm a b dm
I Mh
=
⎡ ⎤
= ⎣ − + − ⎦
= + − − + +
= + + +
= +
∫
∫
∫ ∫ ∫ ∫
∫ ∫
dm (x,y)
CM (0,0)
P (a,b)
P
h
P
Physics, Page 15
보기 : Cylinder 의 회전관성 R
l
r
( )
l R M M
l
R
22
ρ π
π
ρ ⋅ ⋅ = ⇒ ∴ = Density ρ
( )
{ r dr l } r lr dr
r dm
dI = ⋅
2= ρ ⋅ 2 π ⋅ ⋅ ⋅
2= 2 πρ
3(
2)
2 24 2
1 0
3
2 1 2
2 l r dr lR 1 R l R MR
I = πρ ∫
R= ρπ = ρπ =
증명 2
1 2
MR ICM =
M : mass
Z Z’
I
z’= ?
몇 가지 물체의 회전관성
Physics, Page 17
Rolling Race
(Hoop vs Cylinder)
A hoop and a cylinder of equal mass roll down a ramp with height h. Which has greatest KE at bottom?
A) Hoop B) Same C) Cylinder
“they both start with the same potential energy so they have to end with the same kinetic energy because of conservation of energy.
24
Rolling Race
(Hoop vs Cylinder)
A hoop and a cylinder of equal mass roll down a ramp with height h. Which has greatest speed at the bottom of the ramp?
A) Hoop B) Same C) Cylinder
Cylinder will get to the bottom first because inertia for a cylinder is less than that for a hoop type object.
I = MR2 I = ½ MR2
Physics, Page 19
돌림힘 (회전력, Torque)
( sin )
r F r F r F
τ r = × r ur = φ =
⊥r : ⊥ 모멘트 팔(의 길이)
( sin )
tr F r F rF
τ r = × r ur = φ =
F : t 힘의 접선성분
Ft
r
rㅗ F
τ r r ur = × r F
[ N m ]
= ⎣⎡kg m
2 /s
2⎤⎦r F
] / [
]
[ N ⋅ m = kg ⋅ m
2s
2☞ Vector Product
θ
sin AB CC = = Cr Ar Br , ⊥
B A
C
In (x,y,z)-coordinates iˆ×iˆ = jˆ× jˆ = kˆ×kˆ = 0
jˆ kˆ iˆ iˆ
kˆ
iˆ jˆ kˆ kˆ
jˆ
kˆ iˆ jˆ jˆ
iˆ
=
×
−
=
×
=
×
−
=
×
=
×
−
=
×
r r r = ×
Scalar Product and Vector Product
kˆ b jˆ b iˆ b B
kˆ a jˆ a iˆ a A
3 2
1
3 2
1
+ +
=
+ +
r =
r Scalar Product ≡ Ar⋅Br = A B cosθ
(
a1iˆ + a2 jˆ + a3kˆ) (
⋅ b1iˆ +b2 jˆ +b3kˆ)
=
3 3 2
2 1
1b a b a b
a + +
=
Vector Product ≡ Ar×Br = A B sinθcˆ ( ) B , A cˆ r r
(
a1iˆ +a2 jˆ +a3kˆ) (
× b1iˆ +b⊥2 jˆ +b3kˆ)
=
(
a b −a b) (
kˆ + a b −a b) (
jˆ + a b −a b)
iˆ=
Physics, Page 21
τ τ = r = × r F r ur
( )
( )
( ) ( )
2sin
t t
r F rF r ma rm r
mr I
τ φ
α
α α
=
=
=
=
= =
net
I τ = α
r s at
v ar
a
t= α r
(ar = rω2 와는 다르다)
Fr = mar 와는 다르다
⋅
제2법칙
τω
=
= dt P dW
⇒ Power
Physics, Page 23
보기문제 10-8 : 추의 가속도는?
τ =
물체의 가속도 (a) 방향을
각가속도 (α) 방향 (+θ 인 반시계방향) 과 동일하게 잡았다.
h
R M
vrCM
ω
Kinetic Energy of Rolling object
2 2
1 ω
= IP K
Kinetic Energy of the Disc.
MR2
I
IP = CM +
U K
K U
K
ET = T + = R,CM + L,CM + Parallel axis theorem
2 2 2
2 1 2
1 ω + ω
= I MR
K CM
2 2
2 1 2
1
CM
CM Mv
I
K = ω +
CM을 중심으로
하는 질량중심의
선형운동에너지
2 2
2 1 2 1
CM
T Mgh I Mv
E = = ω +
Total Energy
보기문제
vrCM
ω
P• R
매 순간을 보면 P 점을 중심으로 회전하고 있다.