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144 GEOMETRY AND TRIGONOMETRY<br />

(a) Determine the angular velocity of the<br />

wheels in both rad/s and rev/min.<br />

(b) If the speed remains constant for 2.70 km,<br />

determine the number of revolutions<br />

made by a wheel, assuming no slipping<br />

occurs. [ ]<br />

(a) 75 rad/s, 716.2rev/min<br />

(b) 1074 revs<br />

Since θ = ωt then<br />

t = θ ω<br />

Dividing equation (1) by equation (2) gives:<br />

V<br />

t<br />

=<br />

2v sin (θ/2)<br />

(θ/ω)<br />

=<br />

vω sin (θ/2)<br />

(θ/2)<br />

(2)<br />

14.7 Centripetal force<br />

When an object moves in a circular path at constant<br />

speed, its direction of motion is continually changing<br />

and hence its velocity (which depends on both magnitude<br />

and direction) is also continually changing.<br />

Since acceleration is the (change in velocity)/(time<br />

taken), the object has an acceleration. Let the object<br />

be moving with a constant angular velocity of ω and a<br />

tangential velocity of magnitude v and let the change<br />

of velocity for a small change of angle of θ (=ωt)<br />

be V in Fig. 14.12. Then v 2 − v 1 = V. The vector<br />

diagram is shown in Fig. 14.12(b) and since the magnitudes<br />

of v 1 and v 2 are the same, i.e. v, the vector<br />

diagram is an isosceles triangle.<br />

For small angles<br />

hence<br />

V<br />

t<br />

However, ω = v r<br />

thus<br />

sin (θ/2)<br />

(θ/2)<br />

≈ 1,<br />

change of velocity<br />

=<br />

change of time<br />

= acceleration a = vω<br />

vω = v · v<br />

r = v2<br />

r<br />

(from Section 14.6)<br />

i.e. the acceleration a is v2<br />

and is towards the centre<br />

of the circle of motion (along V). It is called the<br />

r<br />

centripetal acceleration. If the mass of the rotating<br />

object is m, then by Newton’s second law, the centripetal<br />

force is mv2 and its direction is towards the<br />

r<br />

centre of the circle of motion.<br />

Problem 16. A vehicle of mass 750 kg travels<br />

around a bend of radius 150 m, at 50.4 km/h.<br />

Determine the centripetal force acting on the<br />

vehicle.<br />

Figure 14.12<br />

Bisecting the angle between v 2 and v 1 gives:<br />

sin θ 2 = V/2<br />

v 2<br />

i.e. V = 2v sin θ 2<br />

= V 2v<br />

(1)<br />

The centripetal force is given by mv2 and its<br />

r<br />

direction is towards the centre of the circle.<br />

Mass m = 750 kg, v = 50.4km/h<br />

50.4 × 1000<br />

= m/s<br />

60 × 60<br />

= 14 m/s<br />

and radius r = 150 m,<br />

thus centripetal force = 750(14)2<br />

150<br />

= 980 N.

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