Length of the pendulum, \(\text I\) = \(1.5 \,m\)
Mass of the bob = \(m\)
Energy dissipated = \(5\)%
According to the law of conservation of energy, the total energy of the system remains constant.
At the horizontal position:
Potential energy of the bob, \(E_p\) = \(mgl\)
Kinetic energy of the bob, \(E_k\) = \(0\)
Total energy = \(mgl\) … (i)
At the lowermost point (mean position): Potential energy of the bob, \(E_p\) = \(0\)
Kinetic energy of the bob, \(E_k\)= \(\frac{1}{2}mv^2\)
Total energy \(E_x\)= \(\frac{1}{2}mv^2\) … (ii)
As the bob moves from the horizontal position to the lowermost point, \(5\)% of its energy gets dissipated. The total energy at the lowermost point is equal to \(95\)% of the total energy at the horizontal point, i.e.,
\(\frac{1}{2}\) \(mv^2\) = \(\frac{95}{100}\times\,mgl\)
\(\therefore\) \(v\) = \(\sqrt{\frac{2\times 95\times 1.5\times 9.8}{100}}\)=
\(5.28\;m/s\)
Two identical ball bearings in contact with each other and resting on a frictionless table are hit head-on by another ball bearing of the same mass moving initially with a speed V. If the collision is elastic, which of the following (Fig. 5.14) is a possible result after collision ?

The bob A of a pendulum released from 30o to the vertical hits another bob B of the same mass at rest on a table as shown in Fig. 5.15. How high does the bob A rise after the collision ? Neglect the size of the bobs and assume the collision to be elastic.

Find the mean deviation about the mean for the data 38, 70, 48, 40, 42, 55, 63, 46, 54, 44.
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