1. The moment of inertia (sometimes referred to as a “swing
weight”) is a measure of the resistance to rotation about a
particular axis. It is often expressed as Ia = mka2 where m is the
mass of the object and ka is the radius of gyration about the axis
of rotation.
The radius of gyration ka for the arm about its COM = 0.368*(arm
length). Compute the moment of inertia of the arm in the extended
position about its own COG. The mass of the human is 70 kg
total.
| Joint | X (cm) | Y (cm) |
| Shoulder | 0 | 0 |
| Wrist | 58 | 0 |
The arm weighs 5% of the body mass and the COM of the arm is 53% from the proximal joint.
2. Compute the moment of inertia of the arm about the shoulder joint using the parallel axes theorem. Parallel axes theorem Ia = Icg + mr2
1. mass = 0.05 M = 0.05 x 70 = 3.5 kg
Icm = m K^2
= (3.5)(0.368 x 0.58)^2
= 0.16 kg m^2 .......Ans
2. I = Icm + m d^2
d = 0.53 x 0.58 m = 0.3074 m
I = (0.16) + (3.5)(0.3074^2)
I = 0.49 kg m^2
1. The moment of inertia (sometimes referred to as a “swing weight”) is a measure of...
Definitions and Equations: Moment of Inertia (D): Tendency to resist angular acceleration; the angular equivalent of mass. In practical terms it is a measure of how hard it is to rotate an object or segment, like a baseball bat or a body segment. It is the sum of the products of the mass (m) with the square of its distance from the axis of rotation (ka). SEE FINAL TWO PAGES OF THIS LAB EOR CHARTS NEEDED TO CALCULATE L. 1...
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The parallel axis theorem provides a useful way to calculate the moment of inertia I about an arbitrary axis. The theorem states that I = Icm + Mh2, where Icm is the moment of inertia of the object relative to an axis that passes through the center of mass and is parallel to the axis of interest, M is the total mass of the object, and h is the perpendicular distance between the two axes. Use this theorem and information...
The Parallel-Axis Theorem allows one to find the moment of inertia of an object if the moment of inertia through the center of mass (c.o.m.) is known and the second axis is parallel to the axis through the c.o.m.. The equation is given by I= Icom +md2, where Icom is the moment of inertia about an axis through the c.o.m., m is the mass of the object, d is the perpendicular distance from the axis through the c.o.m. to the...
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10.24 ** (a) If Icm denotes the moment of inertia tensor of a rigid body (mass M) about its CM, and I the corresponding tensor about a point P displaced from the C M by Δ (ξ, η, ζ), prove that and 1ImMnt, (10.117) yz and so forth. (These results, which generalize the parallel-axis theorem that you probably learned in introductory physics, mean that once you know the inertia tensor for rotation about the CM, calculating it for any other...
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1) The parallel axis theorem provides a useful way to calculate the moment of inertia I about an arbitrary axis. The theorem states that I = Icm + Mh2, where Icm is the moment of inertia of the object relative to an axis that passes through the center of mass and is parallel to the axis of interest, M is the total mass of the object, and h is the perpendicular distance between the two axes. Use this theorem and...