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A rotating merry-go-round makes one complete revolution in \(4.0 \mathrm{~s}\) (Fig. \(10-45)\). (a) What is the linear speed of a child seated \(1.2 \mathrm{~m}\) from the center? \((b)\) What is her acceleration (give components)?

Short Answer

Expert verified
Linear speed is approximately 3.77 m/s; acceleration is 2.96 m/s² towards the center.

Step by step solution

01

Determine the Angular Velocity

The angular velocity \( \omega \) is calculated by finding how many radians per second the merry-go-round covers. Since it makes one complete revolution (which is \(2\pi\) radians) in 4.0 seconds, the angular velocity is \(\omega = \frac{2\pi}{4.0} = \frac{\pi}{2} \text{ s}^{-1} \).
02

Calculate the Linear Speed

The linear speed \( v \) of the child can be found using the relationship \( v = r \cdot \omega \), where \( r \) is the distance from the center (1.2 m). Thus, \( v = 1.2 \times \frac{\pi}{2} = 1.2\pi \text{ m/s} \approx 3.77 \text{ m/s} \).
03

Calculate Centripetal Acceleration

The centripetal acceleration \( a_c \) is given by the formula \( a_c = \omega^2 \cdot r \). Substituting the values, we have \( a_c = \left(\frac{\pi}{2}\right)^2 \times 1.2 = \frac{\pi^2}{4} \times 1.2 \approx 2.96 \text{ m/s}^2 \).
04

Determine Components of Acceleration

In circular motion, all acceleration is centripetal, pointing toward the center of the circle, with no tangential acceleration if the speed is constant. Therefore, in this case, the acceleration has no components in directions other than towards the center, with a magnitude calculated as approximately 2.96 m/s².

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Angular Velocity
Angular velocity is a core concept in circular motion that describes how fast an object rotates or revolves around a central point. In this scenario, the merry-go-round completes one full revolution in 4 seconds. It's essential to understand that a full revolution equals a movement of 2\(\pi\) radians, which is the angular distance for a circular path.
To calculate angular velocity \( \omega \), we divide the total angular displacement by the time taken for one complete cycle. Hence, \( \omega = \frac{2\pi}{4.0} = \frac{\pi}{2} \text{ radians/second}\). This measure gives us the rate of rotation and is crucial for finding other aspects of motion, like linear speed and centripetal acceleration. Remember that angular velocity is a vector quantity, with direction typically along the axis of rotation according to the right-hand rule.
Linear Speed
Linear speed in circular motion is the path distance traveled per unit of time. It can be envisioned as how fast a child moves along the edge of the merry-go-round.
The formula to link linear speed \(v\) with angular velocity is \(v = r \cdot \omega\), where \(r\) is the radius (distance from the rotation axis to the edge).
  • The radius in this scenario is 1.2 meters.
  • The angular velocity, as calculated previously, is \(\frac{\pi}{2} \text{ rad/s}\).
Thus, \(v = 1.2 \times \frac{\pi}{2} = 1.2\pi \text{ m/s} \). This equation illustrates how the linear speed increases with either a longer radius or faster angular velocity. In simpler terms, the further out you are from the center, the faster you have to travel to complete one revolution in the same time.
Centripetal Acceleration
Centripetal acceleration is a key concept in the study of circular motion that refers to the acceleration directed towards the center of the circle along which the body is moving. This acceleration keeps the object in circular motion rather than moving in a straight line.
It can be calculated using the formula \( a_c = \omega^2 \cdot r \). This equation indicates that centripetal acceleration depends on both the square of the angular velocity and the radius of the circle.
In our problem:
  • The angular velocity \(\omega = \frac{\pi}{2} \text{ rad/s}\).
  • The radius \(r = 1.2 \text{ m}\).
Substituting these values, we find \( a_c = \left(\frac{\pi}{2}\right)^2 \times 1.2 = \frac{\pi^2}{4} \times 1.2 \approx 2.96 \text{ m/s}^2\).
This resultant acceleration keeps the child securely moving in a circle, always pointing inward toward the center of rotation. This type of acceleration is constant in magnitude but continuously changes direction as the child rides around the merry-go-round.

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Most popular questions from this chapter

Determine the moment of inertia of a \(19-\mathrm{kg}\) door that is \(2.5 \mathrm{~m}\) high and \(1.0 \mathrm{~m}\) wide and is hinged along one side. Ignore the thickness of the door.

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(II) Two uniform solid spheres of mass \(M\) and radius \(r_{0}\) are connected by a thin (massless) rod of length \(r_{0}\) so that the centers are 3\(r_{0}\) apart. (a) Determine the moment of inertia of this system about an axis perpendicular to the rod at its center. \((b)\) What would be the percentage error if the masses of each sphere were assumed to be concentrated at their centers and a very simple calculation made?

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