The figure shows a conical pendulum, in which the bob (the small object at the lower end of the cord) moves in a horizontal circle at constant speed

The figure shows a conical pendulum, in which the bob (the small object at the lower end of the cord) moves in a horizontal circle at constant speed. (The cord sweeps out a cone as the bob rotates.) The bob has a mass of 0.040 kg, the string has length L = 1.1 m and negligible mass, and the bob follows a circular path of circumference 1.0 m. What are (a) the tension in the string and (b) the period of the motion?

The correct answer and explanation is :

A conical pendulum consists of a mass (bob) attached to the end of a string, moving in a horizontal circular path while the string traces out a cone. In this scenario, the bob has a mass of 0.040 kg, the string length (L) is 1.1 m, and the bob follows a circular path with a circumference of 1.0 m. We aim to determine (a) the tension in the string and (b) the period of the motion.

(a) Tension in the String

First, we calculate the radius (r) of the circular path:

[ \text{Circumference} = 2\pi r ]

[ 1.0\, \text{m} = 2\pi r ]

[ r = \frac{1.0\, \text{m}}{2\pi} \approx 0.159\, \text{m} ]

The angle θ between the string and the vertical can be found using:

[ \sin\theta = \frac{r}{L} = \frac{0.159\, \text{m}}{1.1\, \text{m}} \approx 0.145 ]

[ \theta = \arcsin(0.145) \approx 8.33^\circ ]

In the vertical direction, the vertical component of the tension (T) balances the gravitational force:

[ T\cos\theta = mg ]

[ T = \frac{mg}{\cos\theta} ]

Substituting the known values:

[ T = \frac{0.040\, \text{kg} \times 9.8\, \text{m/s}^2}{\cos(8.33^\circ)} \approx 0.393\, \text{N} ]

(b) Period of the Motion

The centripetal force required for circular motion is provided by the horizontal component of the tension:

[ T\sin\theta = \frac{mv^2}{r} ]

Using the previously calculated tension and angle:

[ 0.393\, \text{N} \times \sin(8.33^\circ) = \frac{0.040\, \text{kg} \times v^2}{0.159\, \text{m}} ]

[ 0.393\, \text{N} \times 0.145 = \frac{0.040\, \text{kg} \times v^2}{0.159\, \text{m}} ]

[ 0.057\, \text{N} = \frac{0.040\, \text{kg} \times v^2}{0.159\, \text{m}} ]

Solving for v:

[ v^2 = \frac{0.057\, \text{N} \times 0.159\, \text{m}}{0.040\, \text{kg}} ]

[ v^2 \approx 0.226\, \text{m}^2/\text{s}^2 ]

[ v \approx 0.475\, \text{m/s} ]

The period (T) is the time taken for one complete revolution:

[ T = \frac{\text{Circumference}}{v} = \frac{1.0\, \text{m}}{0.475\, \text{m/s}} \approx 2.11\, \text{s} ]

Thus, the tension in the string is approximately 0.393 N, and the period of the motion is approximately 2.11 seconds.

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