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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. 11 Kinematics of Particles 425203 Engineering Dynamics Lecture Note

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Page 1: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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.

11 Kinematics of Particles

425203

Engineering Dynamics

Lecture Note

Page 2: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

Vector Mechanics for Engineers: Dynamics

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Contents

Introduction

Rectilinear Motion: Position,

Velocity & Acceleration

Determination of the Motion of a

Particle

Uniform Rectilinear-Motion

Uniformly Accelerated Rectilinear-

Motion

Motion of Several Particles: Relative

Motion

Motion of Several Particles:

Dependent Motion

Graphical Solution of Rectilinear-Motion

Problems

Curvilinear Motion: Position, Velocity &

Acceleration

Derivatives of Vector Functions

Rectangular Components of Velocity and

Acceleration

Motion Relative to a Frame in Translation

Tangential and Normal Components

Radial and Transverse Components

Page 3: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Introduction

• Dynamics includes:

- Kinematics: study of the geometry of motion. Kinematics is used to

relate displacement, velocity, acceleration, and time without reference to

the cause of motion.

- Kinetics: study of the relations existing between the forces acting on a

body, the mass of the body, and the motion of the body. Kinetics is used

to predict the motion caused by given forces or to determine the forces

required to produce a given motion.

• Rectilinear motion: position, velocity, and acceleration of a particle as it

moves along a straight line.

• Curvilinear motion: position, velocity, and acceleration of a particle as it

moves along a curved line in two or three dimensions.

Page 4: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Rectilinear Motion: Position, Velocity & Acceleration

• Particle moving along a straight line is said

to be in rectilinear motion.

• Position coordinate of a particle is defined by

positive or negative distance of particle from

a fixed origin on the line.

• The motion of a particle is known if the

position coordinate for particle is known for

every value of time t. Motion of the particle

may be expressed in the form of a function,

e.g., 326 ttx

or in the form of a graph x vs. t.

Page 5: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

Vector Mechanics for Engineers: Dynamics

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Rectilinear Motion: Position, Velocity & Acceleration

Page 6: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

Vector Mechanics for Engineers: Dynamics

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Rectilinear Motion: Position, Velocity & Acceleration

Page 7: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Rectilinear Motion: Position, Velocity & Acceleration

• Consider particle with motion given by

326 ttx

• at t = 0,

• at t = 2 s,

• at t = 4 s,

• at t = 6 s,

Page 8: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Determination of the Motion of a Particle

• Recall, motion of a particle is known if position is known for all time t.

• Typically, conditions of motion are specified by the type of acceleration

experienced by the particle. Determination of velocity and position requires

two successive integrations.

• Three classes of motion may be defined for:

- acceleration given as a function of time, a = f(t)

- acceleration given as a function of position, a = f(x)

- acceleration given as a function of velocity, a = f(v)

Page 9: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Determination of the Motion of a Particle

• Acceleration given as a function of time, a = f(t):

tttx

x

tttv

v

dttvxtxdttvdxdttvdxtvdt

dx

dttfvtvdttfdvdttfdvtfadt

dv

00

0

00

0

0

0

• Acceleration given as a function of position, a = f(x):

x

x

x

x

xv

v

dxxfvxvdxxfdvvdxxfdvv

xfdx

dvva

dt

dva

v

dxdt

dt

dxv

000

202

12

21

or or

Page 10: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Determination of the Motion of a Particle

• Acceleration given as a function of velocity, a = f(v):

tv

v

tv

v

tx

x

tv

v

ttv

v

vf

dvvxtx

vf

dvvdx

vf

dvvdxvfa

dx

dvv

tvf

dv

dtvf

dvdt

vf

dvvfa

dt

dv

0

00

0

0

0

0

Page 11: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Sample Problem 11.2

Determine:

• velocity and elevation above ground at

time t,

• highest elevation reached by ball and

corresponding time, and

• time when ball will hit the ground and

corresponding velocity.

Ball tossed with 10 m/s vertical velocity

from window 20 m above ground.

Page 12: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Sample Problem 11.2

Page 13: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Uniform Rectilinear Motion

For particle in uniform rectilinear motion, the acceleration is zero and

the velocity is constant.

vtxx

vtxx

dtvdx

vdt

dx

tx

x

0

0

00

constant

Page 14: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Uniformly Accelerated Rectilinear Motion

For particle in uniformly accelerated rectilinear motion, the acceleration of

the particle is constant.

atvv

atvvdtadvadt

dv tv

v

0

000

constant

221

00

221

000

00

0

attvxx

attvxxdtatvdxatvdt

dx tx

x

020

2

020

221

2

constant

00

xxavv

xxavvdxadvvadx

dvv

x

x

v

v

Page 15: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Example: Kinematics relations

Page 16: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Exercise

Page 17: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Homework

Page 18: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Motion of Several Particles: Relative Motion

• For particles moving along the same line, time

should be recorded from the same starting

instant and displacements should be measured

from the same origin in the same direction.

Page 19: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Sample Problem 11.4

Ball thrown vertically from 12 m level

in elevator shaft with initial velocity of

18 m/s. At same instant, open-platform

elevator passes 5 m level moving

upward at 2 m/s.

Determine (a) when and where ball hits

elevator and (b) relative velocity of ball

and elevator at contact.

Page 20: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

Vector Mechanics for Engineers: Dynamics

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Sample Problem 11.4

Page 21: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

Vector Mechanics for Engineers: Dynamics

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Sample Problem 11.4

Page 22: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Motion of Several Particles: Dependent Motion

Page 23: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Sample Problem 11.5

Pulley D is attached to a collar which

is pulled down at 3 cm/s. At t = 0,

collar A starts moving down from K

with constant acceleration and zero

initial velocity. Knowing that velocity

of collar A is 12 cm/s as it passes L,

determine the change in elevation,

velocity, and acceleration of block B

when block A is at L.

Page 24: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

Vector Mechanics for Engineers: Dynamics

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Sample Problem 11.5

Page 25: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Sample Problem 11.5

Page 26: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Exercise

Page 27: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Page 28: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

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Page 29: Eighth Edition - Suranaree University of Technologyeng.sut.ac.th/me/box/2_54/425203/ch11_1lecture.pdf · Eighth Edition Ferdinand P. Beer E. Russell Johnston, Jr. Lecture Notes: J

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

Vector Mechanics for Engineers: Dynamics

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Homework