Orthogonality from infinitesimal small rotation

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The discussion focuses on understanding the mathematical principles behind vector rotations and their properties. The first equation highlights that vector length remains constant during rotations, while the second equality derives from this using the chain rule, assuming the variation of gik is zero. Participants seek clarification on the chain rule's application and the time dependence of vik, questioning whether the infinitesimal matrix leads to a specific identity. The conversation emphasizes the need for detailed explanations of these mathematical concepts. Overall, the thread aims to clarify the intricacies of orthogonality in the context of infinitesimal rotations.
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Hello buddies,

Could someone please help me to understand where the second and the third equalities came from?
Thanks,

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Um... Ok, it's a little difficult to know what level of detail you want.

The first equation essentially says that the length of a vector does not change under rotations. The second one follows from the first one using the chain rule, and assuming delta of gik is zero.
 
Thanks for answering,

gik is basically the inner product of the base set vector, i.e., <ei,ek>.
- Could you please explicit the chain rule?
- is vik time dependent? And since it is an infinitely small matrix, the ##\delta v^k_i = I##?

Thanks
 
I built a device designed to brake angular velocity which seems to work based on below, i used a flexible shaft that could bow up and down so i could visually see what was happening for the prototypes. If you spin two wheels in opposite directions each with a magnitude of angular momentum L on a rigid shaft (equal magnitude opposite directions), then rotate the shaft at 90 degrees to the momentum vectors at constant angular velocity omega, then the resulting torques oppose each other...

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