The Moments of Inertia: Difference between revisions
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The expression for the moment of inertia of a solid cylinder can be built up from the moment of inertia of thin cylindrical shells. | The expression for the moment of inertia of a solid cylinder can be built up from the moment of inertia of thin cylindrical shells. | ||
Because only the perpendicular distances of atoms from the axis matter( | Because only the perpendicular distances of atoms from the axis matter(<math>r_\perp</math>), the moment of inertia for rotation about the axis of a long cylinder has exactly the same form as that of a disk. | ||
==Examples== | ==Examples== | ||
Revision as of 02:22, 1 December 2015
claimed by san47
Definition
Moment of inertia, denoted by the letter I, is another name for rotational inertia. It is associated with an object that is rotating about its center, or an axis. The moment of inertia for any rotating objects must be specified with respect to a chosen axis of rotation due to the varying distance r. The moment of inertia corresponds to mass for translational/linear motion. [1] [2]
A Mathematical Model
The moment of inertia is the sum of mass times the square of perpendicular distance to the rotation axis, that is [math]\displaystyle{ I=\Sigma mr^2 }[/math]for all point mass components. This relationship is the basis for all other moments of inertia since any object can be built up from a collection of point masses. [3] Note that I has units of mass multiplied by distance squared (kg⋅m2), as we might expect from its definition.
Moments of Inertia of Different Shapes
Hoop
The moment of inertia of a hoop or thin hollow cylinder of negligible thickness about its central axis is a straightforward extension of the moment of inertia of a point mass since all of the mass is at the same distance R from the central axis.[4]
Shpere
The moment of inertia of a sphere can be expressed as the summation of moments of infinitesimally thin disks about the z axis.
[5]
Cylinder
The expression for the moment of inertia of a solid cylinder can be built up from the moment of inertia of thin cylindrical shells.
Because only the perpendicular distances of atoms from the axis matter([math]\displaystyle{ r_\perp }[/math]), the moment of inertia for rotation about the axis of a long cylinder has exactly the same form as that of a disk.
Examples
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