Problem 74
Question
Moments of inertia of solid circular eylinder Find the moment of inertia of a solid circular cylinder of radius 1 and height 2 (a) about the axis of the cylinder and (b) about a line through the centroid perpendicular to the axis of the cylinder. (Take \(\delta=1 . )\)
Step-by-Step Solution
Verified Answer
Moment of inertia about the axis is \( \pi \); perpendicular to the axis is \( \frac{7}{6} \pi \).
1Step 1: Identify Cylinder Properties
We have a solid circular cylinder with radius \( R = 1 \) and height \( h = 2 \). The density \( \delta = 1 \). These properties will be used in our calculations.
2Step 2: Calculate Mass of Cylinder
The mass \( M \) of the cylinder is calculated using the formula \( M = \delta \times \text{Volume} = \delta \times \pi R^2 h \). With \( \delta = 1 \), \( R = 1 \), and \( h = 2 \), we have \( M = \pi \times 1^2 \times 2 = 2\pi \).
3Step 3: Moment of Inertia about the Axis of the Cylinder
For a solid cylinder, the moment of inertia \( I_z \) about its axis is given by \( I_z = \frac{1}{2} M R^2 \). Substituting \( M = 2\pi \) and \( R = 1 \), we get \( I_z = \frac{1}{2} \times 2\pi \times 1^2 = \pi \).
4Step 4: Moment of Inertia about Centroid Perpendicular to Axis
The moment of inertia \( I_y \) about a line through the centroid and perpendicular to the axis is given by \( I_y = \frac{1}{4} M R^2 + \frac{1}{12} M h^2 \). Substituting \( M = 2\pi \), \( R = 1 \), and \( h = 2 \), we calculate: \( I_y = \frac{1}{4} \times 2\pi \times 1^2 + \frac{1}{12} \times 2\pi \times 2^2 = \frac{1}{2} \pi + \frac{2}{3} \pi = \frac{7}{6} \pi \).
Key Concepts
Understanding the CylinderDefining Mass in ContextCentroid - The Center of MassAxis and Its Role in Rotational Dynamics
Understanding the Cylinder
A cylinder is a three-dimensional geometric shape that consists of two parallel circular bases connected by a curved surface. Imagine a soup can; that is a perfect example of a cylinder.
Key characteristics of a cylinder include:
These properties are essential when calculating mass and moment of inertia, both of which are necessary to understand the dynamics of a cylinder in motion.
Key characteristics of a cylinder include:
- Radius (\( R \)): The distance from the center to the edge of the base circle. In this case, it is 1 unit.
- Height (\( h \)): The distance between the two bases. Here, it is 2 units.
- Volume: Calculated as \( \pi R^2 h \), which tells us how much space it occupies.
These properties are essential when calculating mass and moment of inertia, both of which are necessary to understand the dynamics of a cylinder in motion.
Defining Mass in Context
Mass is a measure of the amount of matter in an object. For solid objects like cylinders, we determine the mass using density and volume.
For the given cylinder:
For the given cylinder:
- Density (\( \delta \)): This is given as 1 unit, simplifying calculations.
- Volume: Found by \( \pi \times R^2 \times h \)
- Formula for Mass: \( M = \delta \times \text{Volume} \)
Centroid - The Center of Mass
The centroid of a shape is its geometric center or balance point. For simple symmetrical shapes like a cylinder, the centroid lies along its axis of symmetry, midway between its top and bottom surfaces.
The centroid is essential because:
The centroid is essential because:
- It helps locate where the mass is concentrated.
- For a cylinder, it is located at a height of \( \frac{h}{2} \).
- It determines the rotational characteristics related to moments of inertia.
Axis and Its Role in Rotational Dynamics
An axis provides a point or line around which the body rotates. In the context of a cylinder, different axes can provide varying resistance to rotation, measured by the moment of inertia.
Considerations for a cylinder:
Considerations for a cylinder:
- Axis along the cylinder: Usually runs through the center, parallel to the height, making rotation straightforward.
- Perpendicular through centroid: Another critical axis is when it passes through the centroid but perpendicular to the height, which provides information on different rotational dynamics.
Other exercises in this chapter
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