Tanya Sharma said:
Hi Doc
I am not clear about a few things...
If we apply work energy theorem ,
Work done by non conservative forces=Change in the mechanical energy of the ball
Things get a bit tricky when dealing with deformable bodies such as this ball. In the so-called "work"-energy theorem, the "work" done by the external force of the floor will equal the change in mechanical energy. I put work in quotes, because it's really ∫F.dx where F is the force of the floor and x represents the motion of the center of mass. (So it's not the "real" work done by that force.)
∫F.dx=ΔKE + ΔGPE + ΔEPE ,where ΔEPE is the change in the elastic potential energy of the ball and where dx is the displacement of the center of mass
So, if you mean by ∫F.dx what I described above, then I would say that:
∫F.dx = ΔKE + ΔGPE
I would leave out the elastic PE of the ball, as that is internal. This equation is not particularly useful, since we have no simple way of calculating ∫F.dx.
On the other hand, using conservation of energy you can say:
Real Work done from floor = Δtotal energy
The real work is zero, so the total energy is conserved:
0 = ΔKE + ΔGPE + ΔEPE + other forms of internal energy, such as thermal energy. Now you can apply your analysis to that equation.
Using this, you'll get:
25 J = ΔEPE + other forms of internal energy, such as thermal energy.
When all is said and done, most likely all the mechanical energy lost ends up as internal thermal energy.
Hence,ΔEPE = ∫F.dx + 25J
This ΔEPE is what goes away as thermal energy.
Do I make sense? If not where am I getting it wrong ?
Let me know if my comments make sense.