Consider a uniform rod of length b . One half of this rod has a linear mass density of λ 1 = 9 while the other half has a linear mass density of λ 2 = 1 . The rod is initially placed horizontally in a smooth, fixed hemispherical bowl and the denser side is on the left. It is then released from rest at this initial position. The rod undergoes some motion but eventually comes to rest due to the presence of other dissipative forces. The angle θ that the rod makes with the horizontal when it is in equilibrium is given by:
tan θ = n m ⎝ ⎜ ⎜ ⎛ ( b p R ) q − 1 1 ⎠ ⎟ ⎟ ⎞
Here, m , n , p , q are positive integers and m and n are co-prime. FInd m n p q .
Note:
This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try
refreshing the page, (b) enabling javascript if it is disabled on your browser and,
finally, (c)
loading the
non-javascript version of this page
. We're sorry about the hassle.
Solving the force balance equations along the horizontal and vertical directions, and the moment balance equation about the lower end of the rod, we get tan θ = 2 × ( λ 1 + λ 2 ) × 4 R 2 − b 2 b × ( λ 1 − λ 2 ) . So m = 2 , n = 5 , p = 2 , q = 2 and m n p q = 4 0
Problem Loading...
Note Loading...
Set Loading...
It is an easy calculation that the centre of mass G of the rod is such that A G = 1 0 3 b .
In equilibrium, the three forces acting on the rod (gravity and the two normal reactions) must have concurrent lines of action. Thus the centre of mass G must be vertically beneath the centre O of the circle. Thus R cos ( θ + cos − 1 2 R b ) tan θ = 1 0 3 b cos θ = 5 2 ( ( b 2 R ) 2 − 1 ) − 2 1 so that m = 2 , n = 5 , p = q = 2 , making the answer 4 0 .