130 Higher Engineering Mathematics
n=1500
πrev/min=1500
60 π=rev/s, thenangular velocityω= 2 π(
1500
60 π)
=50rad/sThe linear velocity of a point on the rim,v=ωr,where
ris the radius of the wheel, i.e.
540
2mm=0. 54
2m= 0 .27m.Thuslinear velocity v=ωr=( 50 )( 0. 27 )
=13.5m/sProblem 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. 8km
h× 1000m
km×1
3600h
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/sFrom equation (4), angular velocity,ω= 2 πn,
wherenis in rev/s.Hence angular speedn=ω
2 π=60
2 πrev/s= 60 ×60
2 πrev/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=80sSince a wheel is rotating at 573rev/min, then in
80/60minutes it makes573rev/min×80
60min=764revolutionsNow try the following exerciseExercise 59 Further problems on linear
and angular velocity- 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] - 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] - 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.