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Chapter 11

Mohammad Suliman Abuhaiba,Ph.D., P.E.1

Kinematics of Particles

2/8/2019 3:49 PM

First Exam

Wednesday

2/3/2019

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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IntroductionMechanics

Mechanics = science which

describes & predicts conditions of

rest or motion of bodies under

action of forces

Divided into three parts:

1. Mechanics of rigid bodies

2. Mechanics of deformable bodies

3. Mechanics of fluids

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Introduction

Mechanics of rigid bodies is

subdivided into:

1. Statics: bodies at rest

2. Dynamics: bodies in motion

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Introduction

Dynamics is subdivided into:

1. Kinematics

study of geometry of motion

relating displacement, velocity,

acceleration, and time withoutreference to cause of motion

2. Kinetics

study of relation existing between

forces acting on a body, mass of body,and motion of body

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Introduction

A dynamic study could be done on twolevels:

1. Particle: object whose size & shape can

be ignored when studying its motion.

2. Rigid Body: a collection of particles that

remain at fixed distance from each other

at all times & under all conditions of

loading.

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Motion of Particles

1. Rectilinear Motion

2. Curvilinear Motion

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Rectilinear Motion of Particles

Position

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Rectilinear Motion of Particles

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Velocity

t

xv

t

x

t

0lim

Average velocity

Instantaneous

velocity

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Rectilinear Motion of Particles

AccelerationMohammad Suliman Abuhaiba,Ph.D., P.E.

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Instantaneous

acceleration t

va

t

0lim

t

v

Average acceleration

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Rectilinear Motion of Particles

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Consider particle with motion given by

326 ttx

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Three classes of motion may be defined:

1. Acceleration is a function of time, a = f(t)

2. Acceleration is a function of position, a = f(x)

3. Acceleration is a function of velocity, a = f(v)

Determination of Motion of a Particle

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Determination of Motion of a Particle

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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1. Acceleration is a function of time, a = f (t )

tttx

x

tttv

v

dttvxtxdttvdx

dttvdxtvdt

dx

dttfvtvdttfdv

dttfdvtfadt

dv

0

0

0

0

0

0

0

0

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Determination of Motion of a Particle

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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2. Acceleration is a function of position, a = f (x )

x

x

x

x

xv

v

dxxfvxv

dxxfdvvdxxfdvv

xfdx

dvva

dt

dva

v

dxdt

dt

dxv

0

00

2

0212

21

or or

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Determination of Motion of a Particle

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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3. Acceleration is 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

dvdt

vf

dv

dtvf

dvvfa

dt

dv

000

00

0

0

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Sample 11.2

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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1. velocity & elevation above

ground at time t

2. highest elevation reached by

ball and corresponding time

3. time when ball will hit the

ground & corresponding

velocity

Ball tossed with 10 m/s vertical

velocity from a window 20 m

above ground. Determine:

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Sample 11.3

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Brake mechanism used to reduce gun recoil consists

of piston attached to barrel moving in fixed cylinder

filled with oil. As barrel recoils with initial velocity

v0 , piston moves and oil is forced through orifices in

piston, causing piston and cylinder to decelerate at

rate proportional to their velocity; a = - k v

Determine v (t ), x (t ), and v (x ).

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Assignment #11.1

1, 6, 11, 17, 22, 29

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Uniform Rectilinear Motion

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Acceleration is zero and velocity is constant

vtxx

vtxx

dtvdx

vdt

dx

tx

x

0

0

00

constant

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Uniformly Accelerated Rectilinear Motion

Mohammad Suliman Abuhaiba,Ph.D., P.E.

20

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

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Uniformly Accelerated Rectilinear Motion

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Acceleration of the particle is constant

020

2

020

221

2

constant

00

xxavv

xxavvdxadvvadx

dvv

x

x

v

v

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Motion of Several Particles Relative Motion

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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ABAB xxx relative position of B wrt A

ABAB xxx

ABAB vvv relative velocity of B wrt A

ABAB vvv

ABAB aaa relative acceleration of B wrt A

ABAB aaa

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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

1. When & where ball hits the

elevator

2. Relative velocity of ball wrt

elevator at contact

Sample 11.4

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Motion of Several Particles: Dependent Motion

Position of B depends on

position of A

Rope length = constant

Sum of lengths of

segments = constant

constxx BA 2

(one DOF)

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Motion of Several Particles: Dependent Motion

constxxx CBA 22

(2 DOF)

022

022

CBA

CBA

aaa

vvv

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Sample 11.5Pulley 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.

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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A

B

Assignment #11.2

33, 38, 42, 47, 52, 57

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• Given x-t curve, v-t curve = x-t curve slope

• Given v-t curve, a-t curve = v-t curve slope

Graphical Solution of

Rectilinear-Motion Problems

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Given a-t curve, change in velocity between t1 &

t2 = area under a-t curve between t1 & t2.

Given v-t curve, change in position between t1 &

t2 = area under v-t curve between t1 & t2.

Graphical Solution of

Rectilinear-Motion Problems

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Sample Problem 11.6A car leaves station A; it gains speed at the rate of

4 ft/s2 for 6 s and then at the rate of 6 ft/s2 until it

has reached the speed of 48 ft/s. The car maintains

the same speed until it approaches (car does not

reach B yet) station B; brakes are then applied,

giving the car a constant deceleration and

bringing it to a stop in 6 s. The total running time

from A to B is 40 s. Draw the a−t, v−t, and x−t

curves, and determine the distance between

stations A and B.

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Assignment #11.3

61, 67, 73, 79, 87

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Curvilinear Motion: Position, Velocity & Acceleration

• Curvilinear motion: Particle moving along a

curve

• Position vector of a particle at time t

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Curvilinear Motion: Position, Velocity & Acceleration

dt

ds

t

sv

dt

rd

t

rv

t

t

0

0

lim

lim

instantaneous velocity (vector)

instantaneous speed (scalar)

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Curvilinear Motion: Position, Velocity & Acceleration

dt

vd

t

va

t

0lim

instantaneous acceleration

(vector)

• In general, acceleration vector is

not tangent to particle path

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Rectangular Components of Velocity & Acceleration

kzjyixr

kvjviv

kzjyixkdt

dzj

dt

dyi

dt

dxv

zyx

kajaia

kzjyixkdt

zdj

dt

ydi

dt

xda

zyx

2

2

2

2

2

2

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Rectangular Components of Velocity & Acceleration

Motion of a projectile

00 zyx agaa

initial conditions:

0000 zyx

Integrating twice:

0

02

21

00

00

zgttvytvx

vgtvvvv

yx

zyyxx

Mohammad Suliman Abuhaiba,Ph.D., P.E.36

Sample Problem 11.7A projectile is fired from edge of a 150-m cliff with

an initial velocity of 180 m/s at an angle of 30° with

the horizontal. Neglecting air resistance, find:

a. horizontal distance from the gun to point where

projectile strikes the ground

b. greatest elevation above ground reached by

the projectile

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Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Motion Relative to a Frame in Translation xyz = fixed frame of reference

x’y’z’ = moving frame

position of B wrt

moving frame Ax’y’z’ABr

ABAB rrr

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Motion Relative to a Frame in Translation

ABAB vvv

ABAB aaa

Absolute motion of B = motion of A + relative motion

of B wrt moving reference frame attached to A

Mohammad Suliman Abuhaiba,Ph.D., P.E.39

Sample Problem 11.9

Car A is traveling east at

constant speed of 36 km/h.

As car A crosses the

intersection, car B starts

from rest 35 m north of the

intersection & moves south

with a constant

acceleration of 1.2 m/s2.

Determine position,

velocity, and acceleration

of B relative to A 5 s after A

crosses the intersection.

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Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Assignment #11.4

89, 95, 101, 107, 113, 120, 126

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Tangential and Normal Components

Velocity vector is tangent

to path

ttt eee

d

ede

ee

e

tn

nt

t

2

2sinlimlim

2sin2

00

Mohammad Suliman Abuhaiba,Ph.D., P.E.42

Tangential and Normal Components

dt

ds

ds

d

d

edve

dt

dv

dt

edve

dt

dv

dt

vda

tt

t

2

2

va

dt

dva

ev

edt

dva

nt

nt

vdt

dsdsde

d

edn

t

Mohammad Suliman Abuhaiba,Ph.D., P.E.43

Tangential and Normal Components Tangential component of

acceleration reflects

change of speed

Normal component reflects

change of direction

Tangential component may

be +ve or -ve

Normal component always

points toward center of

path curvatureMohammad Suliman Abuhaiba,Ph.D., P.E.

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Tangential and Normal Components – 3D Path

22 va

dt

dvae

ve

dt

dva ntnt

Osculating plane: Plane

containing tangential &

normal unit vectors

ntb eee

binormale

normalprincipal e

b

n

No Acceleration component

along binormalMohammad Suliman Abuhaiba,Ph.D., P.E.

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Sample 11.10A motorist is traveling on

curved section of highway at 88

m/s. The motorist applies

brakes causing a constant

deceleration rate.

Knowing that after 8 s the speed

has been reduced to 66 m/s,

determine the acceleration of

the automobile immediately

after the brakes are applied.

Mohammad Suliman Abuhaiba,Ph.D., P.E.46

Radial and Transverse Components

rr e

d

ede

d

ed

dt

de

dt

d

d

ed

dt

ed rr

dt

de

dt

d

d

ed

dt

edr

rerr

Mohammad Suliman Abuhaiba,Ph.D., P.E.

Radial and Transverse Components

erer

edt

dre

dt

dr

dt

edre

dt

drer

dt

dv

r

rr

rr

Mohammad Suliman Abuhaiba,Ph.D., P.E.

errerr

dt

ed

dt

dre

dt

dr

edt

d

dt

dr

dt

ed

dt

dre

dt

rd

edt

dre

dt

dr

dt

da

r

rr

r

22

2

2

2

2

Radial and Transverse Components

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Radial and Transverse Components – 3D

kzeRr R

kzeReRdt

rdv R

kzeRReRR

dt

vda

R

22

Mohammad Suliman Abuhaiba,Ph.D., P.E.

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Sample 11.12The rotation of the 0.9 m arm OA about O is defined by the

relation 0.15t2 where is expressed in radians and t in

seconds. Collar B slides along the arm in such a way that its

distance from O is r = 0.9 - 0.12 t2, where r is expressed in

meters and t in seconds. After the arm OA has rotated through

30o, determine

Mohammad Suliman Abuhaiba,Ph.D., P.E.

51

a. Total velocity of collar

b. Total acceleration of collar

c. Relative acceleration ofcollar wrt arm

Assignment #11.5

133, 140, 146, 153, 167

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