r. field 10/10/2013 university of florida phy 2053page 1 center-of-mass system of particles:...

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R. Field 10/10/201 3 Univers PHY 2053 Page 1 Center-of- Mass System of Particles: Center- of-Mass Acceleration of the Center-of-Mass: Location of the Center-of-Mass: N N N i i tot cm tot v m v m v m v m p P v M 3 3 2 2 1 1 1 cm tot tot net a M dt P d F Velocity of the Center-of-Mass: (net force acting on the system of particles) (total mass of the system) N N N i i i cm tot r m r m r m r m r m r M 3 3 2 2 1 1 1 tot N N N i i i tot cm M r m r m r m r m r m M r 3 3 2 2 1 1 1 1 N N i i tot m m m m m M 3 2 1 1 tot N N N i i tot tot tot cm M v m v m v m v m p M M P v 3 3 2 2 1 1 1 1 N N N i i i cm tot net a m a m a m a m a m a M F 3 3 2 2 1 1 1 (total momentum of the system) The center-of-mass of a system of particles is the point that moves as though (1) all of the systems mass were concentrated there and (2) all external forces were applied there.

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Page 1: R. Field 10/10/2013 University of Florida PHY 2053Page 1 Center-of-Mass System of Particles: Center-of-Mass Acceleration of the Center-of-Mass: Location

R. Field 10/10/2013 University of Florida

PHY 2053 Page 1

Center-of-Mass

System of Particles: Center-of-Mass

• Acceleration of the Center-of-Mass:

• Location of the Center-of-Mass:

NN

N

iitotcmtot vmvmvmvmpPvM

332211

1

cmtottot

net aMdt

PdF

• Velocity of the Center-of-Mass:

(net force acting on the system of particles)

(total mass of the system)

NN

N

iiicmtot rmrmrmrmrmrM

332211

1

tot

NNN

iii

totcm M

rmrmrmrmrm

Mr

332211

1

1

N

N

iitot mmmmmM

3211

tot

NNN

ii

tottot

totcm M

vmvmvmvmp

MM

Pv

332211

1

1

NN

N

iiicmtotnet amamamamamaMF

332211

1

(total momentum of the system)

The center-of-mass of a system of particles is the point that moves as though (1) all of the systems mass were concentrated there and (2) all external forces were applied there.

Page 2: R. Field 10/10/2013 University of Florida PHY 2053Page 1 Center-of-Mass System of Particles: Center-of-Mass Acceleration of the Center-of-Mass: Location

R. Field 10/10/2013 University of Florida

PHY 2053 Page 2

Center-of-Mass: Superposition

BA

BcmB

AcmABA

cm MM

rMrMr

What is the x-coordinate of the center-of-mass of the circular disk of radius 2R with a circular hole of radius R as shown in the figure? Assume the disk has a uniform mass density .

cm

2R

R

hole

Uniform density

Disk A

Let object A+B be a uniform disk of radius 2R, height h, and center at x=y=0.Let object A be the disk with the hole in it.Let object B be a uniform disk with radius R, height h, and center at y=0, x=-R.

• Superposition:

2R

R

Disk B

Disk A+B

3))2((

)(22

2 RR

hRR

hRx

M

Mx

M

Mx

M

MMx B

cmA

BBcm

A

BBAcm

A

BAAcm

If object A has mass MA and its center-of-mass is located at and object B has mass MB and its center-of-mass is located at then the center of mass of the system A+B is located at

Acmr

BA

BcmB

AcmABA

cm MM

xMxMx

0

Bcmr

• Example:

Answer: R/3

0

Page 3: R. Field 10/10/2013 University of Florida PHY 2053Page 1 Center-of-Mass System of Particles: Center-of-Mass Acceleration of the Center-of-Mass: Location

R. Field 10/10/2013 University of Florida

PHY 2053 Page 3

Center-of-Mass: Example

The figure shows a cubical box with each side consisting of a uniform metal plate of negligible thickness. Each of the four sides have mass, M, and the bottom has mass Mbottom. The box is open at the top (at z = L) and has edge length L. If the the z-coordinate of the center-of-mass is at zCM = L/3, what is Mbottom?

• Fall 2011 Exam 2 Problem 22:

Answer: 2M% Right: 24%

bottombottombottom

cmbottombottom

cmcmcmcm

cm MM

ML

MM

LM

MMMMM

zMzMzMzMzMz

4

2

4

)2/(4

4321

44332211

z

y

x

MLMMz bottomcm 2)4(

MML

MLM

z

MLM

cmbottom 24

)3/(

24

2

0

Page 4: R. Field 10/10/2013 University of Florida PHY 2053Page 1 Center-of-Mass System of Particles: Center-of-Mass Acceleration of the Center-of-Mass: Location

R. Field 10/10/2013 University of Florida

PHY 2053 Page 4

Collisions in 1 Dimension: Elastic

v2 =0 v1

x-axis M1 M2

Lab Frame Before

121

12

2' v

MM

Mv

• Elastic Collision:An elastic collision is one in which the kinetic energy is conserved (i.e. the initial total kinetic energy is equal to the final total kinetic energy). If a projectile with mass M1 and speed v1 traveling to the right along the x-axis collides with a target particle at rest with mass M2, what are the velocities of the two particles after they undergo an elastic collision?

22112211 '' vMvMpvMvMp finalinitial

v'2 v'1

x-axis M1 M2

Lab Frame After

22111 ')'( vMvvM

2222

12112

12222

12112

1 )'()'( vMvMKEvMvMKE finalinitial 2

2221

11111212

12112

1 )'()')('())'(( vMvvvvMvvM

(momentum conservation)

211 '' vvv

(energy conservation)

(1)

(2)

(3)

121

211' v

MM

MMv

Divide eq. 2 by eq. 1 and multiply by 2

Note: a2 - b2 = (a-b)(a+b)

Multiply eq. 3 by M1 and add it to eq. 1

0

0

121 '' vvv (4)

(5)Insert eq. 5 into eq.4

Page 5: R. Field 10/10/2013 University of Florida PHY 2053Page 1 Center-of-Mass System of Particles: Center-of-Mass Acceleration of the Center-of-Mass: Location

R. Field 10/10/2013 University of Florida

PHY 2053 Page 5

1d Collisions: Completely Inelastic

v2 v1

x-axis M1 M2

CM Frame Before

V

x-axis M1+M2

Lab Frame After

• Completely Inelastic Collision (Lab Frame):A projectile with mass M1 and speed v1 traveling to the right along the x-axis collides with a target particle at rest with mass M2. If the two particles stick together to form a single particle of mass M1+M2, what is its velocity? What is the velocity of the center-of-mass of the two particles system before the collision? What is the change in the kinetic energy before and after the collision?

21

21

211

21

1

2

1v

MM

MMKEKEKEv

MM

MVV ifcm

VMMpvMvMp finalinitial )( 212211 (momentum conservation)

0

v2 =0 v1

x-axis M1 M2

Lab Frame Before

V = 0

x-axis M1+M2

CM Frame After

0

• Completely Inelastic Collision (CM Frame):

In the CM frame the initial two particles have equal and opposite momentum.They stick together and are at rest with zero final momentum and zero final kinetic energy. This corresponds to the maximal loss of kinetic energy consistent with momentum conservation.

CMCMcmtotcmtot ppPvM 210

CMCM pp 21

0)( 2121 VMMpppP CMf

CMCMcmtot