Solveeit Logo

Question

Question: A particle is given an initial speed \(u\) inside a smooth spherical shell of radius \(R = 1m\) such...

A particle is given an initial speed uu inside a smooth spherical shell of radius R=1mR = 1m such that it is just able to complete the circle. Acceleration of the particle when its velocity is vertical is:

A) g10g\sqrt {10}
B) gg
C) g2g\sqrt 2
D) g6g\sqrt 6

Explanation

Solution

To solve this question, we have to calculate the resultant of the tangential and centripetal acceleration. We all know the value of tangential acceleration which is equal to the value of acceleration due to gravity. The centripetal acceleration can be calculated by using velocity and the radius of the circle.

Formulae used:
vl=5gl{v_l} = \sqrt {5gl}
Here vl{v_l} is the velocity at the lowest point, gg is the acceleration due to gravity and ll is distance from center.
a=v2ra = \dfrac{{{v^2}}}{r}
Here aa is the centripetal acceleration, vv is the tangential velocity at point B and rr is the radius of the circle.

Complete step by step solution:
We know that in a circle the velocity at the lowest most position will be,
vl=5gl{v_l} = \sqrt {5gl}
Here vl{v_l} is the velocity at the lowest point, gg is the acceleration due to gravity and ll is the distance.
So, u=5glu = \sqrt {5gl}

Applying conservation of energy at points A and B, we get
12mu2=12mv2+m()gl\Rightarrow \dfrac{1}{2}m{u^2} = \dfrac{1}{2}m{v^2} + m\left( - \right)gl
Here uu is the velocity at point A, vv is the velocity at point B, mm is the mass of the box, gg is the acceleration due to gravity and ll is the distance from the center.
The negative sign in gravity is because of its downwards action.
Simplifying the equation, we get,
u2=v22gl\Rightarrow {u^2} = {v^2} - 2gl
Putting the value of uu, we get
v2=(5gl)22gl\Rightarrow {v^2} = {\left( {\sqrt {5gl} } \right)^2} - 2gl
v2=3gl\Rightarrow {v^2} = 3gl
v=3gl\Rightarrow v = \sqrt {3gl}
So the value of tangential velocity at point B is 3gl\sqrt {3gl} .
We know that,
a=v2r\Rightarrow a = \dfrac{{{v^2}}}{r}
Here aa is the centripetal acceleration, vv is the tangential velocity at point B and rr is the radius of the circle.
Putting the values of vv and rr, we get
a=3g\Rightarrow a = 3g

From the above diagram, the resultant acceleration acting on the body will be,
anet=a2+g2+2agcos90\Rightarrow {a_{net}} = \sqrt {{a^2} + {g^2} + 2ag\cos 90^\circ }
anet=a2+g2\Rightarrow {a_{net}} = \sqrt {{a^2} + {g^2}}
Putting the value of a=3ga = 3g we get,
anet=9g2+g2=g10\Rightarrow {a_{net}} = \sqrt {9{g^2} + {g^2}} = g\sqrt {10}
So the net acceleration acting on the body will be g10g\sqrt {10} .

Hence option (A) is the correct option.

Note: In a vertical circle,
1. The velocity at the lower most position is v=5glv = \sqrt {5gl}
2. The velocity at the horizontal position is v=3glv = \sqrt {3gl}
3. The velocity at the top most position is v=glv = \sqrt {gl}
Here gg is the acceleration due to gravity and ll is the distance from the centre. Also for particles in a vertical circle, both centripetal acceleration and acceleration due to gravity acts on it.