chapter 4: linear momentum and collisionswebdirectory.hcmiu.edu.vn/portals/25/userdata... · 4.1....
TRANSCRIPT
4.1. The Center of Mass, Newton’s Second
Law for a System of Particles
4.2. Linear Momentum and Its Conservation
4.3. Collision and Impulse
4.4. Momentum and Kinetic Energy in Collisions
Chapter 4: Linear Momentum and Collisions
4.1. The Center of Mass. Newton’s Second Law for a System of Particles
4.1.1. The center of mass (COM)
4.1.1. The center of mass
•Consider a system of 2 particles of masses m1
and m2 separated by distance d:
dmm
mxcom
21
2
•If m1 at x1 and m2 at x2:
M
xmxm
mm
xmxmxcom
2211
21
2211
where M is the total mass of the system
•If the system has n particles that are strung out along the x axis:
n
i
iinn
com xmMM
xmxmxmx
1
2211 1...
a. Systems of Particles
•If the n particles are distributed in three dimensions:
n
i
iicom
n
i
iicom
n
i
iicom zmM
zymM
yxmM
x111
1,
1,
1
kzjyixr iiiiˆˆˆ
•If the position of particle i is given by a vector:
kzjyixr co mxo mco mco mˆˆˆ
•The center of mass of the system is determined by:
n
i
iicom rmM
r1
1
b. Solid Bodies
zdmM
zydmM
yxdmM
x comcomcom
1,
1,
1
where M is the mass of the object
•For uniform objects, their density are:
V
M
dV
dm
dVV
Mdm
zdVV
zydVV
yxdVV
x comcomcom
1,
1,
1
Sample Problem (p. 204)
Determine the center of mass of the plate
0
PS
PPSSPS
mm
xmxmx
P
SSP
m
mxx
3
1
)2( 22
2
RR
R
area
area
thickness
thickness
m
m
P
S
P
S
P
S
P
S
Rx S
RxP3
1
A system consists of three particles located as shown inthe figure. Find the center of mass of the system.
Sample Problem
4.1.2. Newton’s Second Law for a System of Particles
)1(co mn et aMF
netF
coma
zco mzn e tyco myn e txco mxn e t M aFM aFM aF ,,,,,,
: the net force for all external forces
: the acceleration of the center of mass of the system.
M : the total mass of the system.
4.2. Linear Momentum and Its Conservation
The linear momentum of a particle is a vector quantity defined as:p
vmp
ly .re s p e c tiv e p a r tic le , th eo f v e lo c ity th ea n d m a s s th ea re a n d w h e re vm
Newton’s second law is expressed in terms of momentum:
dt
pdFnet
p artic le . o n the fo rce externalnet theis w here n etF
a. Linear Momentum
(Unit: kg m/s)
•For a system of particles:
nnn vmvmvmpppP
...... 221121
comvMP
com
com aMdt
vdM
dt
Pd
The linear momentum of a system of particles is equal to the product of the total mass M of the system and the velocity of the center of mass.
Question: Why do we need momentum?
Because momentum provides us a tool for studying collision of 2 or more objects.
b. Conservation of Linear Momentum:If the net external force acting on a system of particles is zero,
0netF
co nstantP
:z)o r y, x,X(0 If , Xn etFco nstantXP
14. Two particles are launched from the origin of the coordinatessystem at time t=0. m1=5.0 g is shot directly along the x axis with aconstant speed of 10 m/s. m2=3.0 g is shot with a velocity ofmagnitude 20.0 m/s, at an upward angle such that it always staysdirectly above particle 1 during its flight.(a) What is the maximum height Hmax reached by the COM of the two
particle system?(b) In unit-vector notation, what are the (b) velocity and (c)
acceleration of the com when the com reaches Hmax?
gyvv yy 22
0,22
,2
(a) At the maximum height:
max2
0,2 2gyv y
Particle 2 always stays directly above P.1:
xx vv ,1,2
(m/s) 17.32
,1
22
2
,2
220,2
xxy vvvvv
(m) 3.15max y (m) 74.521
max2max
mm
ymH
(b)
21
2211
1
1
mm
vmvmvm
Mv
n
iiicom
n
i
iicom amaM1
At the maximum height, v2,y=0:
x
xx
xcomycom vmm
vmvmvv ,1
21
,22,11
,, ;0
im/s) 10(comv
(c)
21
2211
mm
amamacom
)(m/s 68.3 2
21
2
mm
gmacom
j )m/s 68.3( 2coma
:hence downward, iscoma
4.3. Collision and Impulse• Consider a collision between a bat and a ball:
The change in the ball’s momentum is:
d ttFpd )(
from a time ti to a time tf:
f
i
f
i
t
t
t
tdttFpd )(
• The impulse of the collision is defined by:
f
i
t
tdttFJ )(
Jp
the change in the object’s momentum
the impulse ofthe object
(Unit: kg m/s)
If F(t) function is unknown: tFJ a vg
Examples:
1. A 0.70 kg ball is moving horizontally with a speed of 5.0 m/s whenit strikes a vertical wall. The ball rebounds with a speed of 2.0 m/s.What is the magnitude of the change in linear momentum of the ball?
vmpvmp
;
Since the ball is moving horizontally, therefore, this is one dimensional motion:
xx vmp
)( ifxx vvmvmp
m/s) (kg 4.95)-(-20.7 :m/s 5 m/s; 2 xif pvv
ivmp ˆkg.m/s)9.4(
x
iv
fv
2. A 1500-kg car travelling at a speed of 5.0 m/s makes a 900 turn in a time of 3.0 s and emerges from this turn with a speed of 3.0 m/s: (a) What is the magnitude of the impulse that acts on the car during this turn? Draw the impulse vector. (b) What is the magnitude of the average force on the car during this turn? (Final exam, June 2014)
iv
fv
ip
fppJ
(a)
if pppJ
)m/s kg(874622 ifppJ
(b)
(N)29153
8746avg
t
JF
4.4. Momentum and Kinetic Energy in Collisions
Three types of collisions: We consider a system of 2 bodies
1. Inelastic collision:
constantP :momentum total
ffii pppp 2121
constantKE
Some energy (KE) is transferred to other forms, e.g. heat, sound.
constant21
21
21
21
21
mm
pp
mm
pp
mm
Pv
ffiicom
2. Elastic collision: conserved. are and KEp
ffii pppp 2121
ffii KKKK 2121
• In one dimension: ffii vmvmvmvm 22112211
2
222
112
222
112
1
2
1
2
1
2
1ffii
vmvmvmvm
Special cases:
:02 iv
if
if
vmm
mv
vmm
mmv
1
21
12
1
21
211
2
:21 mm iff vvv 121 ;0
:12 mm ifif v
m
mvvv 1
2
1211
2;
:21 mm ifif vvvv 1211 2;
3. Perfectly inelastic collision: two bodies stick together after collision:
KE.not but conserved p
:21 fff vvv fii vmmvmvm )( 212211
Case 3
3.1. In one dimension:
3.2. In two dimensions:
fii vmmvmvm
)( 212211
Example: (Perfectly inelastic collision)
A 1000-kg car travelling east at 80.0 km/h collides with a 3000 kg car traveling south at 50.0 km/h. The two cars stick together after the collision. What is the speed of the cars after the collision?(Final exam, June 2014)
fii vmmvmvm
)( 212211
80 km/h
50 km/hfii ppp
21
ip1
ip2
fp
)km/h kg(170000
0.5030000.801000 2222
21
f
iif
p
ppp
m/s 11.8or )km/h(5.42)( 21
mm
pv
ff
1. Center of mass:
n
iiicom rm
Mr
1
1
3. Impulse:tFJ avg theorem)impulse-momentum(linear Jp
4. Conservation of Linear Momentum:
( a closed, isolated system)
constantP
•Inelastic Collisions: ffii pppp 2121
constantKE
•Elastic Collisions: ffii pppp 2121
ffii KKKK 2121
Review:
5. Momentum and Kinetic Energy in Collisions
Unit: kg m/s2. Linear Momentum vmp
dt
PdFnet
f
i
t
tdttFJ )(