- #1
davieddy
- 181
- 0
Consider the flexible string under tension T passing through a
fixed wiggly tube at speed v.
At any point, the tube's wiggly curve has a well-defined centre of curvature,
and associated radius r.
The acceleration of the string is v^2/r, and the force due to tension T is
T*dl/r where dl is the length of an element of string. Both directed towards the
centre of curvature.
If T*dl/r = m*dl*v^2/r (m being mass/unit length) then there is no need for
the tube!
v^2 = T/m and there is no restriction on the waveform.
Comments?
David
fixed wiggly tube at speed v.
At any point, the tube's wiggly curve has a well-defined centre of curvature,
and associated radius r.
The acceleration of the string is v^2/r, and the force due to tension T is
T*dl/r where dl is the length of an element of string. Both directed towards the
centre of curvature.
If T*dl/r = m*dl*v^2/r (m being mass/unit length) then there is no need for
the tube!
v^2 = T/m and there is no restriction on the waveform.
Comments?
David