![Page 1: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/1.jpg)
Lecture 7 Chapter 9
Systems of Particles Wednesday
7-16-03
Warm-up problem
Puzzle Question:Cite two possible reasons why it appears that some basket ball players and dancers have a greaterhang time.
Physlets
![Page 2: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/2.jpg)
Topics
• Center of mass
• Newton’s 2nd law for a system of particles
• Linear momentum, 2nd law in terms of P
• Conservation of P
![Page 3: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/3.jpg)
Center of massThe center of a body or a system of bodies is the point thatmoves as though all of the mass were concentrated there and all external forces were applied there.
![Page 4: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/4.jpg)
![Page 5: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/5.jpg)
Center of MassWhy is it important? For any rigid body the motion of the body is given by the motion of the cm and the motion of the body around the cm.
As an example find the center of mass of the following system
xm M.xcm
d
m xcm = M (d-xcm) xcm = M/(m + M) d
![Page 6: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/6.jpg)
Problem 9.3
2 dimensions
Find xcm and ycm
xcm M = m1 x1 + m2 x2 + m3 x3ycm M = m1 y1 + m2 y2 + m3 y3
xcm 15 = 3*0 + 4*2 + 8*1
xcm = 16/15 = 1.1 m
ycm 15 = 3*0 +4*1 + 8*2
ycm = 20/15 = 1.33 m
.
![Page 7: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/7.jpg)
If the 8 kg mass increases, how does the cm change?
xcm =(m1 x1 + m2 x2 + m3 x3)/(m1+m2+m3)
When m3 gets very large, suppose we neglect the other masses.
xcm ~(m3 x3)/(m3) ~ x3
The center of mass moves towards the large object as it should
![Page 8: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/8.jpg)
Center of Mass for a system of particles
xcm = (m1 x1 + m2 x2 + m3 x3)/M
€
rr cm =
1
Mmi
i=1
n
∑ r r i €
ycm =1
Mmi
i=1
n
∑ y i
€
zcm =1
Mmi
i=1
n
∑ zi
€
xcm =1
Mmi
i=1
n
∑ x i
![Page 9: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/9.jpg)
Newton’s Second Law for a System of particles: Fnet= Macm
€
rr cm =
1
Mmi
i=1
n
∑ r r i take d/dt on both sides
€
rv cm =
1
Mmi
i=1
n
∑ r v i take d/dt again
€
ra cm =
1
Mmi
i=1
n
∑ r a i
€
ra cm =
1
M
r F i
i=1
n
∑
Identify ma as the force on each particle
€
ra cm =
1
M
r F net
€
rF net = M
r a cm
![Page 10: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/10.jpg)
Linear Momentum form of Newton’s 2nd Law
€
rv cm =
1
Mmi
i=1
n
∑ r v i
€
rp i = mi
r v i is the definition of momentum of i'th particle
r P cm = M
r v cm is the momentum of the cm
€
rP cm =
r p i
i=1
n
∑i
Important because it is a vector quantity that is conserved in interactions.
€
rP cm = M
r v cm Now take derivative d/dt of
€
dr P cm
dt= M
dr v cm
dt = M
r a cm
€
rF net =
dr P cm
dt
![Page 11: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/11.jpg)
Law of Conservation of Linear Momentum
If Fnet = 0 on a closed system where no mass enters or leaves the system, then dP/dt = 0 or P = constant.
Pi = Pf for a closed isolated system
Also each component of the momentum Px,Py,Pz is also constant since Fx, Fy, and Fz all = 0
If one component of the net force is not 0, then that component of momentum is not a constant. For example, consider the motion of a horizontally fired projectile. The y component of P changes while the horizontal component is fixed after the bullet is fired.
![Page 12: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/12.jpg)
Air track examples
Two carts connected by a spring. Set them into oscillation by pulling them apart and releasing them from rest. Note cm does not move.
Now repeat with spring between two carts. Analogous to exploding mass.
Again observers in two different inertial reference frames will measure different values of momentum, but both will agree that momentum is conserved.
Note if the net force vanishes in one inertial frame it will vanish in all inertial frames
![Page 13: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/13.jpg)
F(t)-F(t)
€
J = F(t)dtt i
t f
∫ =dp
dtdt
t i
t f
∫ = dpp i
p f
∫ = p f − pi
Change in momentum of ball on left or right.
![Page 14: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/14.jpg)
Andy Rodick has been clocked at serving a tennis ball up to 149 mph(70 m/s).The time that the ball is in contact with the racquet is about 4 ms. The mass of a tennis ball as is about 300 grams.
Favg = J/t = p/ t
p =70( 0.3) - 0 = 21 kg-m/s
Favg = 21/0.004 = 5000 Newtons
What is the acceleration of the ball?
a = Favg /m = 5000N/0.3 kg = 16,667 m/s2
What is the average force exerted by the racquet on the ball?
What distance the racquet go through while the ball is still in contact?
V2f - V2
i =2axx = V2
f /2a = (70)2/2(16667) = 0.15 m
![Page 15: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/15.jpg)
hi
Initial
-vf
Beforebounce
vf
Afterbounce
BOUNCING BALLE = PE = mgh
E = KE = 1/2mv2
hf
![Page 16: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/16.jpg)
Measuring velocities and heights of balls bouncing from a infinitely massive hard floor
Type of Ball
Coefficient of Restitution
(C.O.R.)
Rebound Energy/
Collision Energy
(R.E./C.E.)
Superball 0.90 0.81
Racquet ball 0.85 0.72
Golf ball 0.82 0.67
Tennis ball 0.75 0.56
Steel ball bearing 0.65 0.42
Baseball 0.55 0.30
Foam rubber ball 0.30 0.09
Unhappy ball 0.10 0.01
Beanbag 0.05 0.002
R.E./C.E.= Hi/Hf
Almost elastic collision
Almost inelastic collision
C.O.R. = Vf/Vi
![Page 17: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/17.jpg)
Conservation of MomentumIn a closed isolated system containing a collision, the linear momentum of each colliding body may change but the total linear momentum P of the system can not change, whether the collision is elastic or inelastic.
Fnet = 0, dP/dt = 0, Hence, P = constant .
Each x,y, and z component of the momentum is a constant.
![Page 18: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/18.jpg)
One Dimension Collision
m1v1i + m2v2i = m1v1f + m2v2f
Total momentum before = Total momentum after
1/2 m1v1i2 = 1/2 m1v1f
2 + 1/2m2v2f2
Kinetic energy is conserved too.
€
v1 f =m1 − m2
m1 + m2
v1i
€
v2 f =2m1
m1 + m2
v1i
![Page 19: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/19.jpg)
Balls bouncing off massive floors, we have m2 >>m1
€
≅−m2
m2
v1i ≅ −v1i
€
v2 f =2m1
m1 + m2
v1i
€
v1 f =m1 − m2
m1 + m2
v1i
€
≅2m1
m2
v1i
€
≅0
m1
m2
![Page 20: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/20.jpg)
Lecture 8 Chapter 10
Collisions Thursday
7-17-03
![Page 21: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/21.jpg)
Colliding pool balls The excutive toy
m2 = m1
€
v2 f =2m1
m1 + m2
v1i
€
v1 f =m1 − m2
m1 + m2
v1i
€
≅v1i€
≅0
![Page 22: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/22.jpg)
Two moving colliding objects: Problem 45
m1v1i + m2v2i = m1v1f + m2v2f
1/2 m1v1i2 + 1/2 m2v2i
2 = 1/2 m1v1f2 + 1/2m2v2f
2
-v
-v-vv
v1f
v
m1
m2
€
v1 f =m1 − m2
m1 + m2
v1i +2m2
m1 + m2
v2i
Just before each hits the floor
Just after the big ball bounced
Just after the little ball bounced off the big ball
![Page 23: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/23.jpg)
€
v1 f =m1 − m2
m1 + m2
v1i +2m2
m1 + m2
v2i -vv
€
v1 f =m1 − m2
m1 + m2
(−V ) +2m2
m1 + m2
(V )
For m2 =3m1 ,v1f = 8/4V =2Vsuperball has twice as much speed.
€
v1 f =3m2 − m1
m1 + m2
(V )
How high does it go?€
h =V1 f
2
2g
4 times higher
V1f=2V
V2f =0
![Page 24: Lecture 7 Chapter 9 Systems of Particles Wednesday 7-16-03](https://reader030.vdocuments.us/reader030/viewer/2022032708/56812d16550346895d91ff94/html5/thumbnails/24.jpg)
€
v1 f =m1 − m2
m1 + m2
v1i +2m2
m1 + m2
v2i -vv
€
v1 f =m1 − m2
m1 + m2
(−V ) +2m2
m1 + m2
(V )
€
v1 f =3m2 − m1
m1 + m2
(V )
How high does it go?
€
h =V 2
2g
V1f=3V
V2f = -V
9 times higher
For maximum height consider m2 >>m1
V1f=3V
V2f = -V