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An explanation of mass moments of inertia, including its definition, the parallel axis theorem, and examples of mass moments of inertia for common shapes such as a solid sphere, slender rod, solid circular cylinder, thin disk, thin rectangular plate, and brick. It also covers the concept of the radius of gyration.
What you will learn
Typology: Schemes and Mind Maps
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In this appendix I will tell you all you need to know about mass moments of inertia (at least for this class).
The mass moment of inertia is a measure of an objects resistance to rotation, similar to mass being a measure of an objects resistance to translation. It depends on the distribution of mass of an object and the axis about which the mass moment of inertia is to be calculated. The mass moment of inertia is defined to be:
I = r dm 2
The mass moments of inertia for some common shapes are shown on the following
page.
Parallel Axis Theorem
Given the mass moment of inertia about an axis passing through the center of
gravity, the mass moment of inertia about an axis passing through any other point
may be determined using the parallel axis theorem as shown below:
2 I (^) O =IG+mr
where
r = the distance between G and O
I (^) O = mass moment of inertia about an axis passing though O
I (^) G = mass moment of inertial about the center of gravity.
Radius of Gyration
The radius of the gyration is the quantity that when squared and multiplied by the
mass you get the mass moment of inertia. That is
2 I (^) O =mkO
where
k (^) O = the radius of gyration about point O
m = mass of the object
I (^) O = mass moment of inertia of the object about an axis passing through O.
It is basically just an alternative way of giving you the mass moment of inertia.
Mass moment of Inertia of some Common Shapes
Solid Sphere
2 x y z mr 5
Slender Rod
2 y z mL 12
Solid Circular Cylinder
2 2 y z
2 x
mL 3 r 12
mr 2
Thin Disk
2 y z
2 x
mr 4
mr 2
Thin Rectangular Plate
2 z
2 y
2 2 x
mb 12
mh 12
mb h 12
Brick
2 2 z
2 2 y
2 2 x
mb d 12
mh d 12
mb h 12
x
y
z
L
G
r
z
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x
G
r
z
y
x
G
r
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y
x
G
L
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b
h
y
x
G
h
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G
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