Higher Engineering Mathematics, Sixth Edition

(Nancy Kaufman) #1

130 Higher Engineering Mathematics


n=

1500
π

rev/min=

1500
60 π

=rev/s, then

angular velocityω= 2 π

(
1500
60 π

)
=50rad/s

The linear velocity of a point on the rim,v=ωr,where
ris the radius of the wheel, i.e.
540
2

mm=

0. 54
2

m= 0 .27m.

Thuslinear velocity v=ωr=( 50 )( 0. 27 )
=13.5m/s

Problem 19. A car is travelling at 64.8km/h and
has wheels of diameter 600mm.
(a) Find the angular velocity of the wheels in both
rad/s and rev/min.
(b) If the speed remains constant for 1.44km,
determine the number of revolutions made by
the wheel, assuming no slipping occurs.

(a) Linear velocityv= 64 .8km/h
= 64. 8

km
h

× 1000

m
km

×

1
3600

h
s

=18m/s.

The radius of a wheel=

600
2

=300mm

= 0 .3m.

From equation (5),v=ωr, from which,

angular velocityω=

v
r

=

18
0. 3
=60rad/s

From equation (4), angular velocity,ω= 2 πn,
wherenis in rev/s.

Hence angular speedn=

ω
2 π

=

60
2 π

rev/s

= 60 ×

60
2 π

rev/min

=573rev/min

(b) From equation (1), sincev=s/tthen the time
taken to travel 1.44km, i.e. 1440m at a constant
speed of 18m/s is given by:

timet=

s
v

=

1440m
18m/s

=80s

Since a wheel is rotating at 573rev/min, then in
80/60minutes it makes

573rev/min×

80
60

min=764revolutions

Now try the following exercise

Exercise 59 Further problems on linear
and angular velocity


  1. A pulley driving a belt has a diameter of
    300mm and is turning at 2700/πrevolutions
    per minute. Find the angular velocity of the
    pulley and the linear velocity of the belt
    assuming that no slip occurs.
    [ω=90rad/s,v= 13 .5m/s]

  2. Abicycleistravellingat36km/handthediam-
    eter of the wheels of the bicycle is 500mm.
    Determine the linear velocity of a point on the
    rim of one of the wheels of the bicycle, and
    the angular velocity of the wheels.
    [v=10m/s,ω=40rad/s]

  3. Atrainistravellingat108km/handhaswheels
    of diameter 800mm.
    (a) Determine the angular velocity of the
    wheels in both rad/s and rev/min.
    (b) If the speed remains constant for 2.70km,
    determine the number of revolutions
    made by a wheel, assuming no slipping
    occurs. [
    (a)75rad/s, 716 .2rev/min
    (b)1074revs


]

13.7 Centripetal force


When an object moves in a circular path at constant
speed, its direction of motion is continually changing
and hence its velocity (which depends on both magni-
tude and direction) is also continually changing. Since
acceleration is the (change in velocity)/(timetaken), the
object has an acceleration. Let the object be moving
with a constant angular velocity ofωand a tangential
velocity of magnitudevand let the change of veloc-
ity for a small change of angle ofθ(=ωt)beV in
Fig. 13.17. Thenv 2 −v 1 =V. The vector diagram is
shown in Fig. 13.17(b) and since the magnitudes ofv 1
andv 2 are the same, i.e.v, the vector diagram is an
isosceles triangle.
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