Roger N. answered 08/05/21
. BE in Civil Engineering . Senior Structural/Civil Engineer
Solution:
This is an example of physical body rotation where ω = √( m g r / I) with r being the distance from the pivot of rotation to the center of gravity of the rotating object, In this case and for a bar attached to a massless string it will be the length of the string plus the length from the end of the string to the center of gravity of the rotating bar. r = 70 cm + ( 30 cm/2) = 85 cm = 0.85 m
I is the moment of inertia of a long bar = 1/3 m L2 where L is the bar length = 30 cm =0.3 m
then ω = √( m g r / 1/3 m L2) simplifying ω = √ ( 3 g r / L2) = √ ( 3 . 9.8 m/s2 . 0.85 m / ( 0.3 m)2 ) =
√ ( 25 m2/ s2 / 0.09 m2) = 16.7 /s
= 16.7 s-1 = 16.7 rad/s
The Kinetic energy is KE = 1/2 m Vt2 where Vt is the tangential velocity and
Vt = ω r = 16.7 rad / s ( 0.85 m) = 14.2 m/s/
KE = 1/2 ( 12 g x kg/ 1000 g)( 14.2 m/s)2 = 1.21 kg.m2/ s2 = 1.21 J ( joules) = 1.21 X 107 ergs
note that 1 J = 107 ergs or 1 erg = 10-7 J
or KE = 1/2 ( 12 g) ( 14.2 m/s x 100 cm/m) = 1/2 ( 12 g) ( 1420 cm/s)2 = 12,100,000 g.cm2/s2 = 1.21 x 107 ergs