Figured it out. Use of center mass was an idea which helped me a lot.
$$(m_2−m_1)gr=Iε=(m_2+m_1)r^2\varepsilon$$Force ##F## and accelaration ##a_c=\varepsilon x## at center of mass:
$$F=Ma_c=(m_1+m_2)a_c$$Forces acting:$$F=(m_1+m_2)g−N$$Assume ##m_2>m_1## and center of mass is at distance x from...
@jbriggs444 & @etotheipi : Thanks for actually not giving me solution because I really want to solve it myself.
Will try your suggestions little later and let you know.
Thanks!
@etotheipi : I really was thinking about this problem, and all your points are valid.
But I don't see a motion in this problem - better say I don't see how to introduce it.
Neither do I understand how to introduce acceleration.
Any suggestion will help.
Summary:: What is the force N which acts on a support point at the moment just after system is released?
[Thread moved from the technical forums, so no Homework Template is shown]
A light bar with m1 and m2 masses (m1≠m2) at the ends placed on the support point (in the middle of the bar)...