Centripetal motion. The objective of this experiment is to verify whether the tension in a centripetal force apparatus is equal to the weight of the mass.

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Physics Laboratory Report

Centripetal motion

Aim of experiment:

The objective of this experiment is to verify whether the tension in a centripetal force apparatus is equal to the weight of the mass.

Theory:

(Fig. 1)

Fig. 2 shows an object of mass m moving with constant velocity v in a circular path of radius r.

By keeping the angular speed of the rubber bung constant and considering the equilibrium of all the applied forces in the system, the theoretical value of the centripetal force F is calculated as follows:

F = mv2/r                or     F = mrω2

where v and ω are the linear and angular speeds of the object respectively.


Nevertheless, some correction should be made in this experiment. In this experiment, the following set-up is used.

(Fig.2)

As shown in Fig.3, in reality, the string is not horizontal and moves in a circle of radius r = l sinθ. The weight of the hanger with slotted mass gives the tension (T) in the string.

(Fig.3)

The horizontal component of the tension provides the net centripetal force. Therefore,

T sinθ = mrω2

T sinθ = m(l sinθ)ω2

T = mlω2


Apparatus:

Rubber bung                        x 1

Glass tube (15cm long)        x 1

Nylon thread (1.5m)        x 1

Slotted mass (50g)                x 4

Hanger (150g)                        x 1

Paper clip                        x 1

Meter rule                        x 1

Stop watch                        x 1

Adhesive tape                        x 1

Balance                                x 1

Procedures:

  1. The mass of the rubber bung (m) was weighed and recorded.
  2. The centripetal force apparatus was constructed following the sequence from A to E as shown in Fig.1. A small rubber bung was attached to the upper end of a nylon thread passing through a thin glass tube. The hanger was first loaded with M = 150g.
  3. The position of the paper clip was fixed about 1cm below the lower end of the glass tube by using adhesive tape. The rubber bung was kept about 80cm (l) from the upper end of the glass tube.
  4. The glass tube was held in a vertical position. The rubber bung was swirled over the head of the one who swirl it in a horizontal plane.
  5. The angular speed of the rubber bung was increased until the paper marker was about 1cm below the glass tube and the speed was kept.
  6. The time taken for 30 revolutions of the rubber bung was measured by an observer. The experiment was repeated to take two more measurements. All the data was recorded.
  7. The experiment was repeated by adding slotted masses to the hanger (0.20, 0.25, 0.30, 0.35kg). The results were recorded.
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Precautions:

  1. When swirling the rubber bung, care should be taken not to let the rubber bung hit anyone nearby.
  2. The angular speed when swirling the rubber bung should be kept constant.
  3. As the presence of wind would add air resistance to the swirling motion, which in turn increase the error in time-taking, the experiment should be carried out in a static environment with little disturbance.
  4. The one who swirl the rubber bung should be the same person throughout the experiment for the sake of minimizing the error in time-taking of this experiment. The one who manipulate the ...

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