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Question: In a Conical pendulum, a string of length \(120cm\) is fixed at rigid support and carries a mass \(1...

In a Conical pendulum, a string of length 120cm120cm is fixed at rigid support and carries a mass 150g150gat the end. If the mass is revolved in a horizontal circle of radius 0.2m0.2m around a vertical axis, Calculate the tension in the string. (g=9.8ms2)(g = 9.8\dfrac{m}{{{s^2}}})

Explanation

Solution

In order to solve this equation, we first have to draw a free body diagram of the body. After that, we have to balance the Net force that is acting on the body. All the forces should be in accordance with Newton's third law. We can easily find the solution after balancing all the forces in all the given directions.

Formula Used:
CentripetalForceCentripetal Force = mV2r\dfrac{{m{V^2}}}{r}
mm is the mass of body
VV is the velocity of body
rr is the radius of circle & Secondly, Net force on a body is equal to 00 i. e. Fnet=0{F_{net}} = 0

Complete step by step answer:
Here, a conical pendulum, a string of length 120cm120cm & mass of 150g150g & given we have to calculate the Tension TT in the String.
In order to understand the Question, Let’s draw a free body diagram of a pendulum.
Free Body Diagram:

Here the mass mm is moving in a circular motion of radius 0.2m0.2m with velocity V.V. The Force acting on a mass mm will be
Fnet=mV2r{F_{net}} = \dfrac{{m{V^2}}}{r}
Here, the Tension TT will be resolved into two components TsinθT\sin \theta (in vertical direction) and cosθ\uparrow \cos \theta (in horizontal direction). Now balancing all forces we get
In Vertical Direction:
Tsinθ=mg(i)T\sin \theta = mg - (i)
Now,
In Horizontal plane,
Tcosθ=T\cos \theta = Horizontal force on a mass mm (i.e. Centripetal force)
So,
Tcosθ=mV2r(ii)T\cos \theta = \dfrac{{m{V^2}}}{r} - (ii)
So, from eq. we get
T=mgsinθT = \dfrac{{mg}}{{\sin \theta }}
Now, In ΔABC\Delta ABC, we get sinθ=PH\sin \theta = \dfrac{P}{H}
So, sinθ=l2R2l\sin \theta = \dfrac{{\sqrt {{l^2} - {R^2}} }}{l}
Putting the value of sinθ\sin \theta in eq. (1)(1) we get
T=mgll2R2T = \dfrac{{mgl}}{{\sqrt {{l^2} - {R^2}} }}
Further,
T=(1501000)(9.8)×120(120)2(20)2T = \left( {\dfrac{{150}}{{1000}}} \right)\dfrac{{(9.8) \times 120}}{{\sqrt {{{(120)}^2} - {{(20)}^2}} }} [1kg=1000g,1m=100cm][1kg = 1000g,1m = 100cm]
T=1.52T = 1.52 Newton.

Hence, the tension on the string will be 1.521.52N.

Note: While solving this question, we have to be very careful with directions. Only forces acting in the same direction will balance each other. Also according to Newton's third law, action and reaction occur on different bodies. So we have to be careful while applying it to anybody. the units for every force should be the same.