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Timeline for Angular position vector?

Current License: CC BY-SA 3.0

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Nov 9, 2013 at 8:32 vote accept Henry Swanson
Nov 8, 2013 at 18:19 comment added John Alexiou There are several ways to represent a rigid body rotation. a) A unit vector direction $\hat{z}$ and an angle $\theta$ b) A 3d vector whose magnitude is the angle and direction is the rotation axis c) A 3x3 rotation matrix, representing the local axes coordinates d) Using quarternions e) Using Euler angles.
Nov 8, 2013 at 16:42 answer added John Alexiou timeline score: 0
Nov 8, 2013 at 15:20 answer added stachyra timeline score: 1
Nov 7, 2013 at 6:10 review Suggested edits
Nov 7, 2013 at 7:29
Nov 7, 2013 at 2:45 history edited Henry Swanson CC BY-SA 3.0
winding numbers seem to be related?
Nov 6, 2013 at 23:34 comment added Henry Swanson Why do we know that $\vec{x}(t) = R(t) \vec{x}(0)$?
Nov 6, 2013 at 19:02 comment added joshphysics For a discussion of defining angular velocity in a mathematically precise, general way, see Step 1. here physics.stackexchange.com/a/74014/19976
Nov 6, 2013 at 16:41 comment added Henry Swanson I'm not sure I understand your comment; there seem to be two things going on. One is that perhaps this is not equal at all points on a rigid body. This is fine, because that's also true of the conventional definition of $\omega$. The other seems to be about 2D vs 3D, and I'm not quite sure what you mean. (Rotation is always in a plane)
Nov 6, 2013 at 14:16 comment added Sandesh Kalantre The general relationship for a rigid body undergoing rotation in space is $\vec{v_i}=\vec{\omega} \times\vec{r_i} $ where $i$ denotes a point in the body.So you can't really define $\vec{\omega}=\vec{r} \times \vec{v}$ as that is valid only in the special case when the rotation is in a plane.
Nov 6, 2013 at 10:49 history asked Henry Swanson CC BY-SA 3.0