| Not that I'm about to solve the problem, but I think a successful solution
will involve inventing at least two more pieces of information. You might
want to invent names for them, rather than making people come up with
them and making the solutions slightly harder to compare.
1. The radius of the torus, measured from the center of the hole to the
center of a circular cross-section. (Two times pi times this number
will determine the distance that the propeller's hub travels in one
trip around the torus). Without this information, you couldn't distinguish
between a normal sized donut and a garden hose wrapped around the Earth.
2. The angular speed of the propeller. Either the spin or the "forward"
speed will suffice, since they are related by TR and PR. Without knowing
this, I could state that Ct=C0,Ct'=C0' is a solution, by assuming that
the angular speeds are zero.
Also, do you have a preference for the kind of coordinate system you want
the answer expressed in? Spherical or cylindrical coordinates centered on
the toroid's axis are probably easier than rectangular coordinates.
/AHM/THX
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| Let the toroid be centered at the origin (in cartesian coordinates),
sortof in the xy-plane.
The circular cross-section of the toroid is R, the distance from
the origin to the center of this cross-section is S.
At time t, the center of the propeller is at (S sin(Kt+L),S cos(Kt+L),0).
At time t, the end-points of the propeller are at:
(S sin(Kt+L) +/- R sin(Mt+N) cos(Kt+L),
S cos(Kt+L) +/- R sin(Mt+N) sin(Kt+L),
-/+ R cos(Mt+N))
Or the same thing, with the -/+ replaced by +/-, since the propellor
might be turning counter-clockwise.
Since the propeller rotates PR radians as it moves TR radians around
the inside of the toroid, we have M/K = PR/TR.
The initial conditions impose constraints on L and N. These can be
solved by a couple of inverse trigonometric functions (hint: use
the z-coordinate first).
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