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If the body's center of mass were not placed on the rotational axis of the turntable, how would the person's measured moment of inertia compare to the moment of inertia for rotation about the center of mass? (a) The measured moment of inertia would be too large; (b) the measured moment of inertia would be too small; (c) the two moments of inertia would be the same; (d) it depends on where the body's center of mass is placed relative to the center of the turntable.

Short Answer

Expert verified
The measured moment of inertia would be too large (option a).

Step by step solution

01

Understand the Concept of Moment of Inertia

The moment of inertia is a measure of an object's resistance to changes in its rotation. It depends on the mass distribution relative to the axis of rotation. If mass is farther from the axis, the moment of inertia increases.
02

Apply the Parallel Axis Theorem

The parallel axis theorem states that the moment of inertia about any axis parallel to one through the center of mass is given by: \( I = I_{cm} + Md^2 \), where \( I_{cm} \) is the moment of inertia through the center of mass, \( M \) is the mass, and \( d \) is the distance between the axes.
03

Analyze the Problem

In this problem, the body's center of mass is away from the rotational axis of the turntable. According to the parallel axis theorem, the moment of inertia measured around the turntable's axis will be \( I = I_{cm} + Md^2 \), which is greater than \( I_{cm} \) since \( Md^2 > 0 \).
04

Conclusion

The measured moment of inertia is greater when the axis of rotation is not through the center of mass. Therefore, the correct answer is (a) The measured moment of inertia would be too large.

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Key Concepts

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

Center of Mass
The center of mass (COM) of an object is a critical point where the entire mass seems to be concentrated. It is the average location of all the mass in a body. Imagine it as the balancing point of an object where it would stay level if supported.
This concept is crucial in understanding rotational movements and balance.
  • If a force is applied at the center of mass, the object will move without rotating.
  • If the force is applied elsewhere, it will cause the object to rotate around the center of mass.
Understanding the center of mass is essential when discussing the moment of inertia, as it affects how easily an object can be spun around an axis.
Parallel Axis Theorem
The parallel axis theorem is a fundamental concept in rotational dynamics. It provides a way to calculate an object's moment of inertia when the rotational axis is not through the center of mass. According to this theorem:
  • The moment of inertia about an axis parallel to one through the center of mass can be calculated with the equation: \[ I = I_{cm} + Md^2 \]
  • \( I_{cm} \) is the moment of inertia through the center of mass.
  • \( M \) is the total mass of the object.
  • \( d \) is the distance between the two axes.
This theorem shows that the moment of inertia increases when the axis is farther from the center of mass. Hence, the farther the rotational axis is from the center of mass, the larger the contribution of \( Md^2 \) to the total moment of inertia.
Rotational Axis
The rotational axis is the line around which an object rotates. The position of this axis plays a significant role in the rotational dynamics of the body.
  • It can pass through the center of mass, leading to minimal resistance to rotation.
  • Or it can be offset, causing increased resistance due to the need for more force to rotate the object.
Choosing the right axis of rotation is crucial in engineering and design, as it affects the effort needed to spin or rotate objects. If the axis does not pass through the center of mass, the object will experience a larger moment of inertia, making it more resistant to changes in its rotational motion.
Mass Distribution
Mass distribution refers to how mass is spread throughout an object. It has a direct impact on the moment of inertia. The further the mass is from the rotational axis, the greater the moment of inertia will be.
  • For a concentrated mass closer to the rotational axis, the moment of inertia is lower.
  • For a spread-out mass farther from the axis, the moment of inertia increases significantly.
This idea is essential in understanding why the moment of inertia can change with different mass arrangements. Engineers and designers must consider mass distribution in their work, especially when designing rotating systems like wheels or turbines.

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Most popular questions from this chapter

A block with mass m is revolving with linear speed \(v_1\) in a circle of radius \(r_1\) on a frictionless horizontal surface (see Fig. E10.40). The string is slowly pulled from below until the radius of the circle in which the block is revolving is reduced to \(r_2\). (a) Calculate the tension \(T\) in the string as a function of \(r\), the distance of the block from the hole. Your answer will be in terms of the initial velocity \(v_1\) and the radius \(r_1\). (b) Use \(W = \int_{r1}^{r2} \overrightarrow{T} (r) \cdot d\overrightarrow{r}\) to calculate the work done by \(\overrightarrow{T}\) when \(r\) changes from \(r_1\) to \(r_2\). (c) Compare the results of part (b) to the change in the kinetic energy of the block.

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