In mathematics, a conical spiral, also known as a conical helix,[1] is a space curve on a right circular cone, whose floor projection is a plane spiral. If the floor projection is a logarithmic spiral, it is called conchospiral (from conch).
In the
x
y
x=r(\varphi)\cos\varphi , y=r(\varphi)\sin\varphi
a third coordinate
z(\varphi)
m2(x2+y
2 , m>0 | |
0) |
x=r(\varphi)\cos\varphi , y=r(\varphi)\sin\varphi , \color{red}{z=z0+mr(\varphi)} .
Such curves are called conical spirals.[2] They were known to Pappos.
Parameter
m
x
y
A conical spiral can instead be seen as the orthogonal projection of the floor plan spiral onto the cone.
1) Starting with an archimedean spiral
r(\varphi)=a\varphi
x=a\varphi\cos\varphi , y=a\varphi\sin\varphi , z=z0+ma\varphi , \varphi\ge0 .
In this case the conical spiral can be seen as the intersection curve of the cone with a helicoid.
2) The second diagram shows a conical spiral with a Fermat's spiral
r(\varphi)=\pma\sqrt{\varphi}
3) The third example has a logarithmic spiral
r(\varphi)=aek\varphi
Introducing the abbreviation
K=ek
r(\varphi)=aK\varphi
4) Example 4 is based on a hyperbolic spiral
r(\varphi)=a/\varphi
\varphi\to0
The following investigation deals with conical spirals of the form
r=a\varphin
r=aek\varphi
The slope at a point of a conical spiral is the slope of this point's tangent with respect to the
x
y
\tan\beta=
z' | |
\sqrt{(x')2+(y')2 |
A spiral with
r=a\varphin
\tan\beta= | mn |
\sqrt{n2+\varphi2 |
For an archimedean spiral is
n=1
\tan\beta=\tfrac{m}{\sqrt{1+\varphi2}} .
r=aek\varphi
\tan\beta=\tfrac{mk}{\sqrt{1+k2}}
\color{red}{constant!
Because of this property a conchospiral is called an equiangular conical spiral.
The length of an arc of a conical spiral can be determined by
\varphi2 | |
L=\int | |
\varphi1 |
\sqrt{(x')2+(y')2+(z')2}d\varphi =
\varphi2 | |
\int | |
\varphi1 |
\sqrt{(1+m2)(r')2+r2}d\varphi .
For an archimedean spiral the integral can be solved with help of a table of integrals, analogously to the planar case:
L=
a | |
2 |
\left[\varphi\sqrt{(1+m2)+\varphi2}+(1+m2)ln\left(\varphi+\sqrt{(1+m2)+\varphi2}\right)\right
\varphi2 | |
] | |
\varphi1 |
.
For a logarithmic spiral the integral can be solved easily:
L= | \sqrt{(1+m2)k2+1 |
In other cases elliptical integrals occur.
For the development of a conical spiral[3] the distance
\rho(\varphi)
(x,y,z)
(0,0,z0)
\varphi
\psi
\rho=\sqrt{x2+y
2}=\sqrt{1+m | |
0) |
2} r ,
\varphi=\sqrt{1+m2}\psi .
Hence the polar representation of the developed conical spiral is:
\rho(\psi)=\sqrt{1+m2} r(\sqrt{1+m2}\psi)
In case of
r=a\varphin
\rho=a\sqrt{1+m2}n+1\psin,
which describes a spiral of the same type.
In case of a hyperbolic spiral (
n=-1
In case of a logarithmic spiral
r=aek\varphi
\rho=a\sqrt{1+m2} e
k\sqrt{1+m2 | |
\psi} .
The collection of intersection points of the tangents of a conical spiral with the
x
y
For the conical spiral
(r\cos\varphi,r\sin\varphi,mr)
the tangent vector is
(r'\cos\varphi-r\sin\varphi,r'\sin\varphi+r\cos\varphi,mr')T
and the tangent:
x(t)=r\cos\varphi+t(r'\cos\varphi-r\sin\varphi) ,
y(t)=r\sin\varphi+t(r'\sin\varphi+r\cos\varphi) ,
z(t)=mr+tmr' .
The intersection point with the
x
y
t=-r/r'
\left(
r2 | |
r' |
\sin\varphi,-
r2 | |
r' |
\cos\varphi,0\right) .
r=a\varphin
\tfrac{r2}{r'}=\tfrac{a}{n}\varphin+1
n=-1
a
r=aek\varphi
\tfrac{r2}{r'}=\tfrac{r}{k}