In physics and geometry, the troposkein (from Greek, Ancient (to 1453);: [[wikt:τρόπος#Ancient Greek|τρόπος]]|trópos|turn Greek, Ancient (to 1453);: [[wikt:σχοῖνος#Ancient Greek|σχοῖνος]]|skhoînos|rope|label=and)[1] is the curve an idealized rope assumes when anchored at its ends and spun around its long axis at a constant angular velocity. This shape is similar to the shape assumed by a skipping rope, and is independent of rotational speed in the absence of gravity, but varies with respect to rotational speed in the presence of gravity. The troposkein does not have a closed-form representation; in the absence of gravity, though, it can be approximated by a pair of line segments spanned by a circular arc (tangential to the line segments at its endpoints). The form of a troposkein can be approximated for a given gravitational acceleration, rope density and angular velocity by iterative approximation. This shape is also useful for decreasing the stress experienced by the blades of a Darrieus vertical axis wind turbine.