| written 9.5 years ago by | modified 3.8 years ago by |
Indian Institute of Science Education and Research > Physics > Sem 2 > Classical Mechanics
Marks : 20M
Year : April 2015
| written 9.5 years ago by | modified 3.8 years ago by |
Indian Institute of Science Education and Research > Physics > Sem 2 > Classical Mechanics
Marks : 20M
Year : April 2015
| written 9.5 years ago by |
Let $N$ be the normal force between stick and circle and let $F_f$ be the friction between ground and circle (see figure below). Then we immadiatly see that the friction force between stick and circle is also $F_f$, because the torques from the two friction forces on the circle must …
That circle isn't in horiz equilibrium because Nsin@, Fcos@ and F all point to the left.
N (on the circle) points to the circle's centre, equal & opposite to N (on the stick). F (on the circle) is equal & opposite to F (on the stick).
Note the 'N' in your diagram is infact N (on the stick), which was used in taking moments.
Also tan@ doesn't equal sin@/(1 + cos@), this re-arranges to tan@ + sin@ = sin@, which is wrong. Its tan(@/2) = sin@/(1 + cos@).