Component of angular velocity in rigid body motion -- which is right?

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The discussion centers on the angular velocity vector w = (w1, w2, w3) of a rigid body and the confusion surrounding its definitions. One definition states that the rigid body rotates about w at a rate equal to the magnitude of w, while the other suggests each component of w indicates rotation about its respective axis. It is clarified that while angular velocities can be added as vectors, performing rotations about each axis separately does not yield a unique result due to the non-commutative nature of finite rotations. The combined rotation can be viewed as occurring about a single axis at any moment, but this axis and rate of rotation will vary over time unless specific conditions are met. Understanding these concepts is essential for accurately analyzing rigid body motion.
mcheung4
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Let w = (w1, w2, w3) wrt to the body frame of a rigid body, where the body frame is right-handed orthonormal. I have gathered 2 definitions of w from different sources and I am confused at how they connect to one another. One is that the RB rotates about w through its CoM at rate abs(w), the other is that each component of w represents the rate at which the RB rotates about that particular basis axis. Does this mean we can somehow add the 3 rotations (which are about different axes) and get an equivalent rotation about some other (single) axis? Thanks!
 
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mcheung4 said:
Let w = (w1, w2, w3) wrt to the body frame of a rigid body, where the body frame is right-handed orthonormal. I have gathered 2 definitions of w from different sources and I am confused at how they connect to one another. One is that the RB rotates about w through its CoM at rate abs(w), the other is that each component of w represents the rate at which the RB rotates about that particular basis axis. Does this mean we can somehow add the 3 rotations (which are about different axes) and get an equivalent rotation about some other (single) axis? Thanks!
Yes, if there is a simple finite rotation. That is Euler's rotation theorem. See:http://vmm.math.uci.edu/PalaisPapers/EulerFPT.pdf

Where there is continual rotation about more than one axis, one axis of rotation will rotate about another axis, which means the axis will precess. Warning: that analysis of rotational motion can be rather complicated and difficult.

AM
 
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mcheung4 said:
Does this mean we can somehow add the 3 rotations (which are about different axes) and get an equivalent rotation about some other (single) axis?

You can add them as vectors. If you want to "add" them by doing 3 separate rotations, one about each axis, this is a different matter. A velocity is a rate of rotation, not a finite rotation. You'd have to define what it means to "apply each angular velocity component separately about its corresponding axis". I think you can make this definition meaningful if you think in terms of integrating angular velocity to get net displacement. As I recall, it has to do with taking the exponential of matrices.

Finite rotations don't commute. So if you say "perform each rotation separately about its correspondin axis" this doesn't define a unique answer. The order in which you perform them can give different results - i.e. a specific point on the rotating object can end up in different positions depending on the order of rotations. So if you treated the velocity numbers as finite rotations and performed the component rotations, you would not, in general, end up with a rotation equal to their vector sum.
 
At any instant in time, you can view the combined rotation as a rotation about a single axis, but unless the object is spherically symmetric (or has an inertial tensor with just a single eigenvalue), the rotation rate and axis will change over time.
 

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