Image
Name
First described
Equation
Comment
circle
r
=
k
{\displaystyle r=k}
The trivial spiral
Archimedean spiral
c. 320 BC
r
=
a
+
b
⋅
θ
{\displaystyle r=a+b\cdot \theta }
Also known as the arithmetic spiral
Euler spiral (also Cornu spiral or polynomial spiral)
x
(
t
)
=
C
(
t
)
,
{\displaystyle x(t)=\operatorname {C} (t),\,}
y
(
t
)
=
S
(
t
)
{\displaystyle y(t)=\operatorname {S} (t)}
using Fresnel integrals [1]
Fermat's spiral (also parabolic spiral)
1636[2]
r
2
=
a
2
⋅
θ
{\displaystyle r^{2}=a^{2}\cdot \theta }
hyperbolic spiral
1704
r
=
a
θ
{\displaystyle r={\frac {a}{\theta ))}
also reciprocal spiral
lituus
1722
r
2
⋅
θ
=
k
{\displaystyle r^{2}\cdot \theta =k}
logarithmic spiral
1638[3]
r
=
a
⋅
e
b
⋅
θ
{\displaystyle r=a\cdot e^{b\cdot \theta ))
Approximations of this are found in nature; also known as the equiangular spiral.
Fibonacci spiral
circular arcs connecting the opposite corners of squares in the Fibonacci tiling
approximation of the golden spiral
golden spiral
r
=
φ
2
⋅
θ
π
{\displaystyle r=\varphi ^{\frac {2\cdot \theta }{\pi ))\,}
special case of the logarithmic spiral
Spiral of Theodorus
Also known as the Pythagorean spiral; an polygonal spiral composed of contiguous right triangles that approximates the Archimedean spiral
involute
1673
helix
r
(
t
)
=
1
,
{\displaystyle r(t)=1,\,}
θ
(
t
)
=
t
,
{\displaystyle \theta (t)=t,\,}
z
(
t
)
=
t
{\displaystyle z(t)=t}
a 3-dimensional spiral
Rhumb line (also loxodrome)
type of spiral drawn on a sphere
Cotes's spiral
1722
1
r
=
{
A
cosh
(
k
θ
+
ε
)
A
exp
(
k
θ
+
ε
)
A
sinh
(
k
θ
+
ε
)
A
(
k
θ
+
ε
)
A
cos
(
k
θ
+
ε
)
{\displaystyle {\frac {1}{r))={\begin{cases}A\cosh(k\theta +\varepsilon )\\A\exp(k\theta +\varepsilon )\\A\sinh(k\theta +\varepsilon )\\A(k\theta +\varepsilon )\\A\cos(k\theta +\varepsilon )\\\end{cases))}
Solution to the two-body problem for an inverse-cube central force
Poinsot's spirals
r
=
a
⋅
csch
(
n
⋅
θ
)
,
{\displaystyle r=a\cdot \operatorname {csch} (n\cdot \theta ),\,}
r
=
a
⋅
sech
(
n
⋅
θ
)
{\displaystyle r=a\cdot \operatorname {sech} (n\cdot \theta )}
Nielsen's spiral
1993[4]
x
(
t
)
=
ci
(
t
)
,
{\displaystyle x(t)=\operatorname {ci} (t),\,}
y
(
t
)
=
si
(
t
)
{\displaystyle y(t)=\operatorname {si} (t)}
A variation of Euler spiral, using sine integral and cosine integrals
Polygonal spiral
special case approximation of logarithmic spiral
Fraser's Spiral
1908
Optical illusion based on spirals
Conchospiral
r
=
μ
t
⋅
a
,
{\displaystyle r=\mu ^{t}\cdot a,\,}
θ
=
t
,
{\displaystyle \theta =t,\,}
z
=
μ
t
⋅
c
{\displaystyle z=\mu ^{t}\cdot c}
three-dimensional spiral on the surface of a cone.
Calkin–Wilf spiral
Ulam spiral (also prime spiral)
1963
Sack's spiral
1994
variant of Ulam spiral and Archimedean spiral.
Seiffert's spiral
2000[5]
r
=
sn
(
s
,
k
)
,
{\displaystyle r=\operatorname {sn} (s,k),\,}
θ
=
k
⋅
s
{\displaystyle \theta =k\cdot s}
z
=
cn
(
s
,
k
)
{\displaystyle z=\operatorname {cn} (s,k)}
spiral curve on the surface of a sphere
using the Jacobi elliptic functions [6]
Tractrix spiral
1704[7]
{
r
=
A
cos
(
t
)
θ
=
tan
(
t
)
−
t
{\displaystyle {\begin{cases}r=A\cos(t)\\\theta =\tan(t)-t\end{cases))}
Pappus spiral
1779
{
r
=
a
θ
ψ
=
k
{\displaystyle {\begin{cases}r=a\theta \\\psi =k\end{cases))}
3D conical spiral studied by Pappus and Pascal [8]
doppler spiral
x
=
a
⋅
(
t
⋅
cos
(
t
)
+
k
⋅
t
)
,
{\displaystyle x=a\cdot (t\cdot \cos(t)+k\cdot t),\,}
y
=
a
⋅
t
⋅
sin
(
t
)
{\displaystyle y=a\cdot t\cdot \sin(t)}
2D projection of Pappus spiral[9]
Atzema spiral
x
=
sin
(
t
)
t
−
2
⋅
cos
(
t
)
−
t
⋅
sin
(
t
)
,
{\displaystyle x={\frac {\sin(t)}{t))-2\cdot \cos(t)-t\cdot \sin(t),\,}
y
=
−
cos
(
t
)
t
−
2
⋅
sin
(
t
)
+
t
⋅
cos
(
t
)
{\displaystyle y=-{\frac {\cos(t)}{t))-2\cdot \sin(t)+t\cdot \cos(t)}
The curve that has a catacaustic forming a circle. Approximates the Archimedean spiral.[10]
Atomic spiral
2002
r
=
θ
θ
−
a
{\displaystyle r={\frac {\theta }{\theta -a))}
This spiral has two asymptotes ; one is the circle of radius 1 and the other is the line
θ
=
a
{\displaystyle \theta =a}
[11]
Galactic spiral
2019
{
d
x
=
R
∗
y
x
2
+
y
2
d
θ
d
y
=
R
∗
[
ρ
(
θ
)
−
x
x
2
+
y
2
]
d
θ
{
x
=
∑
d
x
y
=
∑
d
y
+
R
{\displaystyle {\begin{cases}dx=R*{\frac {y}{\sqrt {x^{2}+y^{2))))d\theta \\dy=R*{\Bigl [}\rho (\theta )-{\frac {x}{\sqrt {x^{2}+y^{2)))){\Bigr ]}d\theta \end{cases)){\begin{cases}x=\sum dx\\\\\\y=\sum dy+R\end{cases))}
The differential spiral equations were developed to simulate the spiral arms of disc galaxies, have 4 solutions with three different cases:
ρ
<
1
,
ρ
=
1
,
ρ
>
1
{\displaystyle \rho <1,\rho =1,\rho >1}
, the spiral patterns are decided by the behavior of the parameter
ρ
{\displaystyle \rho }
. For
ρ
<
1
{\displaystyle \rho <1}
, spiral-ring pattern;
ρ
=
1
,
{\displaystyle \rho =1,}
regular spiral;
ρ
>
1
,
{\displaystyle \rho >1,}
loose spiral. R is the distance of spiral starting point (0, R) to the center. The calculated x and y have to be rotated backward by (
−
θ
{\displaystyle -\theta }
) for plotting.[12]