circular helix (original) (raw)
The space curve traced out by the parameterization
𝜸(t)=[acos(t)asin(t)bt],t∈ℝ,a,b∈ℝ |
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is called a circular helix (plur. helices).
A circular helix can be conceived of as a space curve with constant, non-zero curvature, and constant, non-zero torsion. Indeed, one can show that if a space curve satisfies the above constraints, then there exists a system of Cartesian coordinates in which the curve has a parameterization of the form shown above.
Figure 1: A plot of a circular helix with a=b=1, and κ=τ=1/2.
An important property of the circular helix is that for any point of it, the angle φ between its tangent and the helix axis is constant. Indeed, if we consider the position vector of that arbitrary point, we have (where 𝐤 is the unit vector parallel to helix axis)
d𝜸dt⋅𝐤=[-asintacostb][0 0 1]=b≡∥d𝜸dt∥cosφ=a2+b2cosφ. |
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Therefore,
as was to be shown.
There is also another parameter, the so-called pitch of the helix P which is the separation between two consecutive turns. (It is mostly used in the manufacture of screws.) Thus,
P=γ3(t+2π)-γ3(t)=b(t+2π)-bt=2πb, |
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and P is also a constant.