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Lec 03 Vehicle Motion ( Transportation Engineering Dr.Lina Shbeeb )

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Vehicle motion
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Vehicle motion

Transportation

Engineering

Dr. Lina Shbeeb 2

Definitions

• Kinematic is the study of motion irrespective of the forces that cause it

• Kinetic is the study of motion that accounts the forces that cause it.

• The motion of a body can be linear or curvilinear

• It can be investigated in relation to a fixed coordinate system (absolute motion) or in relation to a moving coordinate system (relative motion)

Vehicle motion can be described based on kinematic and kinetic equations

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Equation of motion/ Rectilinear Motion

• The rectilinear position of x is measured from a

reference point and has unit of length

• The displacement is the difference in its position

between two instants.

• Velocity v is the displacement of the particle divided by

time over which the displacement occurs. It is given by

the derivative of the displacement with respect of time

• Speed is a scalar quantity and it is equal to the

magnitude of the velocity, which is a vector

dt

dxv

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Equation of motion/ Rectilinear Motion

• Acceleration a is the rate of change

of velocity with respect to time.

• It can be positive, zero or negative.

Negative acceleration or what is

common known as deceleration is

often denoted as d and its

magnitude is given in the positive

(d of 16 ft/s2 equals the same as an

acceleration of - ft/s2) adxvdv

toleadswhich

vdx

dva

dt

dx

dx

dva

dt

dva

Equation derivation

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Equation of motion/ Rectilinear Motion • The simplest case of rectilinear motion is the

case of constant acceleration where

oo

oo

o

t

o

v

v

xtvatx

Thus

xxavv

leadwhichadxvdv

inegratingbycedisoffunctionaasressedbecanvelocityThe

vatv

dtadv

givesttotittheoveregratingby

adtdv

tconsadt

dv

o

2

22

2

1

)(2

1

,

tanexp

0limint

tan

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Dr. Lina Shbeeb 6

…Equation of motion/ Rectilinear Motion

• The acceleration of a vehicle from an initial speed vo is

given by the relationship

Acceleration as a function of velocity

)1()1(

)(

,

)1(

)ln(1

tan

2

BtoBt

Bt

o

Bt

o

Bt

v

v

t

o

v

v

eB

ve

B

At

B

Ax

eBvAa

equalsaBvAainsubstituteisvif

eveB

Av

leadwhich

tBvAB

dtBvA

dv

consareBandA

BvAdt

dva

o

o

Dr. Lina Shbeeb

Travel Speed

12

12

tt

xxv

Time

Distance

t2

t1

x1

x2

Dr. Lina Shbeeb

Spot Speed

dt

dxv

Time

Distance

t1

x1

V

Dr. Lina Shbeeb

Spot Speed Measurements

t1 t2 t3 Time

x3

x2

x1

Dis

tance

45.0

40.0

30.0

Distance

x

(ft)

4.0

3.0

2.0

Time

t

(s)

(40-30)/(3-2)

=10.0

---

Speed 1

v

(ft/s)

---

(45-30)/(4-2)

= 7.5

---

Speed 2

v

(ft/s)

(45-40)/(3-2)

=5.0

Dr. Lina Shbeeb

Spot Speed Measurements

Time

(s)

Distance

(ft)

Speed

(ft)

0.0 0.0 -

0.1 2.13 21.5

0.2 4.30 21.9

0.3 6.51 22.4

0.4 8.78 22.4

0.5 10.99 21.3

0.6 13.04 -

Dr. Lina Shbeeb

Average Acceleration Rate

12

12

tt

vva

Time

Speed

t2

t1

v1

v2

Dr. Lina Shbeeb

Spot Acceleration Rate

dt

dva

Time

speed

t1

v1

a

Dr. Lina Shbeeb

Measuring Acceleration

Rates

Time

(s)

Distance

(ft)

Speed

(ft/s)

Acceleration

(ft/s2)

0.0 0.0 - -

0.1 2.13 21.5 -

0.2 4.30 21.9 4.5

0.3 6.51 22.4 2.5

0.4 8.78 22.4 -5.5

0.5 10.99 21.3 -

0.6 13.04 - -

Dr. Lina Shbeeb

Constant Acceleration Motion

constadt

dv

tv

vadtdv

00

0vatv

avdx

dv

xv

vadxvdv

00

a

vvx

2

20

2

dtvatvdtdx )( 0

x t

dtvatdx0 0 0 )(

tvatx 0

2

2

1

Remark: The equation used for design is , where the

deceleration rate has a positive value.

a

vvx

2

220

Dr. Lina Shbeeb

Exercise

•From the following data,

calculate the acceleration

rate at the distance of 2

feet from the reference

point.

Distance

(ft) Speed

(ft/s)

0 19.4

1 19.6

2 20.0

3 20.8

4 21.3

a=5.91ft/s2???

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Constant Acceleration Motion

constadt

dv

tv

vadtdv

00

0vatv

avdx

dv

xv

vadxvdv

00

a

vvx

2

20

2

dtvatvdtdx )( 0

x t

dtvatdx0 0 0 )(

tvatx 0

2

2

1

Remark: The equation used for design is , where the

deceleration rate has a positive value.

a

vvx

2

220

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Dr. Lina Shbeeb 17

Braking Distance

ag

w

w

sinw

u

coswf

Db

G

1.0

Distance to stop vehicle

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Braking on Grades

sincos WWfag

W

a

vvx

2

220

x

Db

cos2

cos22

0

a

vvxDb

bDvva

2

cos)( 22

0

cos

sincos2

cos)(

1 220

f

Dvv

g b

cos

sin

2

1)(

1 220

f

Dvv

g b

G

tan

cos

sin)(2

220

Gfg

vvDb

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Dr. Lina Shbeeb 19

Braking distance

• Braking Distance (Db)

• Db = distance from brakes enact to final speed

• Db = f(velocity, grade, friction)

• Db = (V02 – V2)/[30(f +/- G)]

• or

• Db = (V02 – V2)/[254(f +/- G)] metric

– Db = braking distance (feet or meters)

– V0 = initial velocity (mph or kph)

– V = final velocity (mph or kph)

– f = coefficient of friction

– G = Grade (decimal) 30 or 254 = conversion coefficient

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Braking Distance

Db = braking distance

u = initial velocity when brakes are

applied

a = vehicle acceleration

g = acceleration of gravity (32.2 ft/sec2)

G = grade (decimal), level roads G=zero

• AASHTO represents friction as a/g which is a function

of the roadway, tires, etc

• Can use when deceleration is known (usually not) or

use previous equation with friction

Db = _____u2_____

30({a/g} ± G)

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Vehicle Braking Distance

• Factors

• Braking System

• Tire Condition

• Roadway Surface

• Initial Speed

• Grade

• Braking Distance Equation

• db = (V2 - U2) / 30( f + g )

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Coefficient of friction

Pavement condition Maximum Slide

Good, dry 1.00 0.80

Good, wet 0.90 0.60

Poor, dry 0.80 0.55

Poor, wet 0.60 0.30

Packed snow and

Ice

0.25 0.10

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Dr. Lina Shbeeb 23

Motion on Circular Curves

dt

dvat

R

van

2

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Dr. Lina Shbeeb 24

coscossin ns amWfW

coscos)(cossin

2

WR

v

g

WWfW s

e

tan

cos

sin

gR

vfe s

2

Motion on

Circular

Curves

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Minimum Radius of a Circular Curve

• where u = vehicle velocity (mph)

• e = tan (rate of superelevation)

• fs = coefficient of side friction (depends on design speed)

• Example

– design speed = 65 mph

– rate of superelevation = 0.05

– coefficient of side friction = 0.11

• Solution

– minimum radius

– R = (65)2/[15(0.05+0.11)] = 1760 ft

)(15

2

sfe

uR

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Dr. Lina Shbeeb 26

Relative Motion • It is common to examine the motion of one

object in relation to another, for example the

motion of vehicles on a highway may be studies

from the point of view of the driver of a moving

vehicle.

• The simplest case of relative motion involves the

motion of one object B relative to a coordinate

system (x, y, z) that is translating but not rotating

with respect to a fixed coordinate system (X, Y,

Z)

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Dr. Lina Shbeeb 27

Relative Motion • The relationship between the position vectors of the two objects in relation to the fixed

system, RA and RB and the position vector rB/A with respect to the moving object A is

Y

Z

y

X

x

z

RA

RB

RA/B

ABAB

ABAB

ABAB

aaa

and

vvv

givestimetorespectwithatingDifferenti

rrr

/

/

/


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