Ibix
Science Advisor
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If you spin up the propellor arbitrarily slowly (i.e. ##d\omega/dt \rightarrow 0##) then you can treat the propellor as rigid, I think, in the usual sense of "transients die away quickly". Alternatively one could attach rockets along the length of the blades and adjust their thrust to maintain uniform (in some inertial frame) rotational motion. However, there is an upper limit to the angular velocity you can achieve like this - namely ##\omega<c/r## if r is the radius of the propellor. But there is nothing stopping you spinning the boss up to a greater angular speed than this - which is what is baking the OP's noodle, I think.
At that point, you can't treat the material as rigid, infinitely or otherwise. To maintain rigidity would require the propellor tips to force the boss to stay below the critical angular velocity, and that is problematic. What must happen is that the blades flex so that the tips (and indeed the entire blades) are contained in a radius ##r'##, ##r'<r##, so that ##\omega r' <c##. Either that or they disintegrate - which is much more plausible.
At that point, you can't treat the material as rigid, infinitely or otherwise. To maintain rigidity would require the propellor tips to force the boss to stay below the critical angular velocity, and that is problematic. What must happen is that the blades flex so that the tips (and indeed the entire blades) are contained in a radius ##r'##, ##r'<r##, so that ##\omega r' <c##. Either that or they disintegrate - which is much more plausible.