Mechanics of Machines by G. H. Ryder, M. D. Bennett (auth.)

By G. H. Ryder, M. D. Bennett (auth.)

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Iii) Since this relative slipping direction is downhill, even though motion is hopefully uphill, the friction force on the tyre will be uphill as shown. There will, of course, be an equal and opposite friction reaction on the road, and it is this force that will cause any loose gravel to be ejected rearwards. N 2 drive is possible. (b) In the second case, the force required up the plane is still 3288 N but now it must be generated at the front wheels. 8 x 3900 = 3120 N and hence front-wheel drive up the hill is not possible.

This can be seen by differentiating the expression for velocity or by noting that the velocity-time graph is a straight line. Such motion is, of course, a special case, but it arises so frequently that it is worth while developing general expressions relating the various quantities. Consider, therefore, a particle moving along a straight line with a constant acceleration a and having an initial velocity Vo at zero time. 2 A city bus has a maximum speed of 90 km/h. 2 m/s2 without discomfort to the passengers.

6 shows the form of the acceleration, velocity and displacement as functions of time. 7. 7 Angular motion of a line a small increment of time t5t, the line PQ moves through a small angle ~() to a new position P'Q'. 2 replacing the linear quantity by the corresponding angular quantity. It is essential that in angular motion problems radian units are used for all angular measures. 6 For tests on an electric motor, the armature is accelerated uniformly from rest to a speed of 1450 rev /min, held at this speed for 10 s, and then decelerated uniformly to rest.

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