Saturday, October 20, 2007

Irodov Problem 1.86

Let the initial angle where the ball was left off from be . The force acting on the ball in the tangential direction of motion will be (as shown in the figure). The acceleration in the tangential direction will thus be . There will be no radial component to the acceleration since the ball is stationary at this position.

The velocity of the ball at the lowest position can be determined by using conservation of energy. As shown in the figure, the height the ball would have fallen is . Thus,




At the lowest point the only acceleration the ball is subjected to is the centripetal acceleration acting radially upwards and is equal to .

If both these accelerations are to be equal then,

Irodov Problem 1.85

The speed of the sphere at a given angle can be determined by the fact the total energy of the system will be conserved.
The potential energy lost will be and this will be converted to the kinetic energy of the sphere given by . In other words,






(a) There are two components of acceleration that the sphere is subject to i) the centripetal acceleration acting radially inwards (towards the pivot) and ii) the tangential acceleration (since the body is not only rotating but also increasing in speed as it moves) .















(3) is not surprising since the only force acting in the tangential direction is the component of gravity given by and thus the acceleration will be . The net acceleration is the Euclidean norm of the tangential and radial accelerations given by,


There are two forces acting on the mass along the radial direction, i) the tension T acting radially inwards and ii) force of gravity acting vertically downwards . The radial acceleration of the mass is directed radially inwards. Thus, we have,



(b) The vertical component of the sphere's velocity is given by as shown in the figure. At its maxima, the first derivative is 0 and the second derivative is negative.








As seen from (6) the second derivative will be negative when (5) is satisfied. The tension at this angle can be calculated using (4) and is given by,





(c)
When the vertical component is 0,