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Question: A mass of \(0.2kg\) is whirled in a horizontal circle of radius \(0.5m\) by a string inclined at \(3...

A mass of 0.2kg0.2kg is whirled in a horizontal circle of radius 0.5m0.5m by a string inclined at 3030^\circ to the vertical. Calculate the tension in the string and the speed of the mass in the horizontal circle?

Explanation

Solution

This question utilizes the concept of mechanics and free body diagrams. We need to draw the free body diagram of the mass which is whirled and then equate the forces acting on them in the vertical and horizontal direction.

Formulae used :
Fc=mv2r{F_c} = \dfrac{{m{v^2}}}{r} where Fc{F_c} is the centripetal force acting on the body, mm is the mass of the body and vv is the velocity of the body and rr is the radius of the circle.
Acceleration due to gravity g=9.8ms2g = 9.8m{s^{ - 2}}

Complete step by step answer:
Let the body which is whirled around be AA . Let it be spinning from a point BB with a rope with tension TT in it .
According to the question, it is inclined at 3030^\circ to the vertical.
Then, the angle it will make with the horizontal will be
θ=9030 θ=60  \Rightarrow \theta = 90^\circ - 30^\circ \\\ \Rightarrow \theta = 60^\circ \\\
Mass of the body AA is m=0.2kgm = 0.2kg
Radius of the circle which is made when AA is whirled r=0.5mr = 0.5m
Now, a free body diagram is made to understand better.

First, we balance out the vertical forces acting on AA .
We have a component of the tension of the string, which is pushing the body upwards. Then we have the weight of the body which is pulling it downwards.
Since the body is in equilibrium, these two forces must be equal to each other.
Thus, we have

Tsinθ=mg \Rightarrow T\sin \theta = mg
Putting in the respective values, we have
Tsin60=0.2kg×9.8ms2 T=0.2×9.8sin60N T=1.960.866N T=2.26N  \Rightarrow T\sin 60^\circ = 0.2kg \times 9.8m{s^{ - 2}} \\\ \Rightarrow T = \dfrac{{0.2 \times 9.8}}{{\sin 60^\circ }}N \\\ \Rightarrow T = \dfrac{{1.96}}{{0.866}}N \\\ \Rightarrow T = 2.26N \\\
Therefore, the tension on the string is 2.26N2.26N
Now, while balancing out the horizontal forces, we see that the centripetal force is balanced out by the horizontal component of tension. Thus we have
Fc=Tcosθ\Rightarrow {F_c} = T\cos \theta
mv2r=Tcosθ\Rightarrow \dfrac{{m{v^2}}}{r} = T\cos \theta
Putting in the respective values, we get
0.2kg×v20.5m=2.26N×cos60 v2=2.26×0.5×0.50.2(ms1)2 v2=(11.3×0.5×0.5)(ms1)2  \Rightarrow \dfrac{{0.2kg \times {v^2}}}{{0.5m}} = 2.26N \times \cos 60^\circ \\\ \Rightarrow {v^2} = \dfrac{{2.26 \times 0.5 \times 0.5}}{{0.2}}{\left( {m{s^{ - 1}}} \right)^2} \\\ \Rightarrow {v^2} = \left( {11.3 \times 0.5 \times 0.5} \right){\left( {m{s^{ - 1}}} \right)^2} \\\
Now, using square root on both the sides, we get
v=3.36×0.5ms1 v=1.68ms1  \Rightarrow v = 3.36 \times 0.5m{s^{ - 1}} \\\ \Rightarrow v = 1.68m{s^{ - 1}} \\\
Therefore, the speed of the mass in the horizontal circle is 1.68ms11.68m{s^{ - 1}}.

Note: Students usually get confused when resolving a vector into two parts. Just remember that the vertical component of the vector is the vector multiplied by sinθ\sin \theta and the horizontal component is the vector multiplied by cosθ\cos \theta . Here, θ\theta is the angle between the vector and the xx axis.