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VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J. Walt Oler Texas Tech University CHAPTER © 2007 The McGraw-Hill Companies, Inc. All rights reserved. 14 Systems of Particles Adapted for 425203 Engineering Dynamics

Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

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Page 1: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

VECTOR MECHANICS FOR ENGINEERS:

DYNAMICS

Eighth Edition

Ferdinand P. Beer

E. Russell Johnston, Jr.

Lecture Notes:

J. Walt Oler

Texas Tech University

CHAPTER

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

14Systems of Particles

Adapted for 425203

Engineering Dynamics

Page 2: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

Eig

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ition

14 - 2

Application of Newton’s Laws. Effective Forces• Newton’s second law for each particle Pi

in a system of n particles,

Page 3: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

Eig

hth

Ed

ition

14 - 3

Application of Newton’s Laws. Effective Forces

Page 4: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

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14 - 4

Linear & Angular Momentum

LF &rr

=∑ OO HM &rr

=∑

Page 5: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

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14 - 5

Motion of the Mass Center of a System of Particles

• Differentiating twice,

==

==

=

=

=

FLam

Lvmvm

rmrm

G

n

iiiG

n

iiiG

r&rr

rrr

&r

&r

1

1

Page 6: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

Eig

hth

Ed

ition

14 - 6

Angular Momentum About the Mass Center

( )

=

′×′=′=

G

n

iiiiG

M

vmrH

r

rrr

1

iGi aaa ′+=rrr

Page 7: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

Eig

hth

Ed

ition

14 - 7

Angular Momentum About the Mass Center

( )∑=

′×′=′n

iiiiG vmrH

1

rrr

GGi vvv ′+=rrr

Page 8: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

Eig

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14 - 8

Conservation of Momentum

• If no external forces act on the particles of a system, then the linear momentum and angular momentum about the fixed point O are conserved.

constant constant

00

==

==== ∑∑

O

OO

HL

MHFLrr

r&rr

&r

• In some applications, such as problems involving central forces,

constant constant

00

=≠

==≠= ∑∑

O

OO

HL

MHFLrr

r&rr

&r

• Concept of conservation of momentum also applies to the analysis of the mass center motion,

constant constant

constant

00

==

==

==== ∑∑

GG

G

GG

Hv

vmL

MHFL

rr

rr

r&rr

&r

Page 9: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

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14 - 9

Sample Problem 14.2

A 20 N projectile is moving with a velocity of 100 m/s when it explodes into 5 and 15 N fragments. Immediately after the explosion, the fragments travel in the directions θA = 45o and θB = 30o.

Determine the velocity of each fragment.

Page 10: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

Eig

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14 - 10

Kinetic Energy• Kinetic energy of a system of particles,

( ) ∑∑==

=•=n

iii

n

iiii vmvvmT

1

221

121 rr

iGi vvv ′+=rrr

Page 11: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

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14 - 11

Principle of Impulse and Momentum

Page 12: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

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Vector Mechanics for Engineers: Dynamics

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14 - 12

Sample Problem 14.4

Ball B, of mass mB, is suspended from a cord, of length l, attached to cart A, of mass mA, which can roll freely on a frictionless horizontal tract. While the cart is at rest, the ball is given an initial velocity

Determine (a) the velocity of B as it reaches it maximum elevation, and (b) the maximum vertical distance hthrough which B will rise.

.20 glv =

Page 13: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

Eig

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14 - 13

Sample Problem 14.4

x

y

Page 14: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

© 2007 The McGraw-Hill Companies, Inc. All rights reserved.

Vector Mechanics for Engineers: Dynamics

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14 - 14

Sample Problem 14.4

Page 15: Ferdinand P. Beer Systems of Particles Adapted for ...eng.sut.ac.th/me/box/2_54/425203/ch14 system of particle.pdf · VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Eighth Edition Ferdinand

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Vector Mechanics for Engineers: Dynamics

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14 - 15

Sample Problem 14.5

Ball A has initial velocity v0 = 10 m /s parallel to the axis of the table. It hits ball B and then ball C which are both at rest. Balls A andC hit the sides of the table squarely at A’ andC’ and ball B hits obliquely at B’.

Assuming perfectly elastic collisions, determine velocities vA, vB, and vC with which the balls hit the sides of the table.