3247:
8087:
2878:
3718:) with them along the curve. If the axis of the top points along the tangent to the curve, then it will be observed to rotate about its axis with angular velocity -τ relative to the observer's non-inertial coordinate system. If, on the other hand, the axis of the top points in the binormal direction, then it is observed to rotate with angular velocity -κ. This is easily visualized in the case when the curvature is a positive constant and the torsion vanishes. The observer is then in
4005:
6760:
3703:
6314:
3242:{\displaystyle {\begin{aligned}{\begin{bmatrix}\mathbf {e} _{1}'(s)\\\vdots \\\mathbf {e} _{n}'(s)\\\end{bmatrix}}=\\\end{aligned}}\|\mathbf {r} '(s)\|\cdot {\begin{aligned}{\begin{bmatrix}0&\chi _{1}(s)&&0\\-\chi _{1}(s)&\ddots &\ddots &\\&\ddots &0&\chi _{n-1}(s)\\0&&-\chi _{n-1}(s)&0\\\end{bmatrix}}{\begin{bmatrix}\mathbf {e} _{1}(s)\\\vdots \\\mathbf {e} _{n}(s)\\\end{bmatrix}}\end{aligned}}}
1331:
420:
4576:
1577:
478:
5337:
27:
6554:
1154:
243:
4272:
2517:
5094:
6488:
6068:
1397:
5846:
5313:
6755:{\displaystyle {\frac {\mathrm {d} }{\mathrm {d} t}}{\begin{bmatrix}\mathbf {T} \\\mathbf {N} \\\mathbf {B} \end{bmatrix}}=\|\mathbf {r} '(t)\|{\begin{bmatrix}0&\kappa &0\\-\kappa &0&\tau \\0&-\tau &0\end{bmatrix}}{\begin{bmatrix}\mathbf {T} \\\mathbf {N} \\\mathbf {B} \end{bmatrix}}}
2036:
2711:
2321:
3686:
interpretation. Imagine that an observer moves along the curve in time, using the attached frame at each point as their coordinate system. The Frenet–Serret formulas mean that this coordinate system is constantly rotating as an observer moves along the curve. Hence, this coordinate system is always
945:
1326:{\displaystyle {\begin{aligned}{\frac {\mathrm {d} \mathbf {T} }{\mathrm {d} s}}&=\kappa \mathbf {N} ,\\{\frac {\mathrm {d} \mathbf {N} }{\mathrm {d} s}}&=-\kappa \mathbf {T} +\tau \mathbf {B} ,\\{\frac {\mathrm {d} \mathbf {B} }{\mathrm {d} s}}&=-\tau \mathbf {N} ,\end{aligned}}}
415:{\displaystyle {\begin{aligned}{\frac {\mathrm {d} \mathbf {T} }{\mathrm {d} s}}&=\kappa \mathbf {N} ,\\{\frac {\mathrm {d} \mathbf {N} }{\mathrm {d} s}}&=-\kappa \mathbf {T} +\tau \mathbf {B} ,\\{\frac {\mathrm {d} \mathbf {B} }{\mathrm {d} s}}&=-\tau \mathbf {N} ,\end{aligned}}}
4881:
8073:
4571:{\displaystyle \mathbf {r} (s)=\mathbf {r} (0)+\left(s-{\frac {s^{3}\kappa ^{2}(0)}{6}}\right)\mathbf {T} (0)+\left({\frac {s^{2}\kappa (0)}{2}}+{\frac {s^{3}\kappa '(0)}{6}}\right)\mathbf {N} (0)+\left({\frac {s^{3}\kappa (0)\tau (0)}{6}}\right)\mathbf {B} (0)+o(s^{3}).}
2863:
2327:
6876:
2168:
1808:
6309:{\displaystyle \mathbf {N} (t)={\frac {\mathbf {T} '(t)}{\|\mathbf {T} '(t)\|}}={\frac {\mathbf {r} '(t)\times \left(\mathbf {r} ''(t)\times \mathbf {r} '(t)\right)}{\left\|\mathbf {r} '(t)\right\|\,\left\|\mathbf {r} ''(t)\times \mathbf {r} '(t)\right\|}}}
1572:{\displaystyle {\begin{bmatrix}\mathbf {T'} \\\mathbf {N'} \\\mathbf {B'} \end{bmatrix}}={\begin{bmatrix}0&\kappa &0\\-\kappa &0&\tau \\0&-\tau &0\end{bmatrix}}{\begin{bmatrix}\mathbf {T} \\\mathbf {N} \\\mathbf {B} \end{bmatrix}}.}
5126:
7853:
5695:
4743:
7040:
858:
7423:
7322:
6329:
5902:
Moreover, using the Frenet–Serret frame, one can also prove the converse: any two curves having the same curvature and torsion functions must be congruent by a
Euclidean motion. Roughly speaking, the Frenet–Serret formulas express the
3393:
6053:
1026:
2554:
2200:
723:
847:
1881:
1900:
1088:
3800:
5430:
under congruence, so that if two figures are congruent then they must have the same properties. The Frenet–Serret apparatus presents the curvature and torsion as numerical invariants of a space curve.
3844:
7198:
2512:{\displaystyle {\begin{aligned}{\overline {\mathbf {e} _{j}}}(s)=\mathbf {r} ^{(j)}(s)-\sum _{i=1}^{j-1}\langle \mathbf {r} ^{(j)}(s),\mathbf {e} _{i}(s)\rangle \,\mathbf {e} _{i}(s).\end{aligned}}}
3761:, particularly in models of microbial motion, considerations of the Frenet–Serret frame have been used to explain the mechanism by which a moving organism in a viscous medium changes its direction.
7104:. The converse, however, is false. That is, a regular curve with nonzero torsion must have nonzero curvature. This is just the contrapositive of the fact that zero curvature implies zero torsion.
7490:
3999:
2997:
2883:
2332:
2205:
1159:
248:
3637:
5089:{\displaystyle \mathbf {r} (0)+\left({\frac {s^{2}\kappa (0)}{2}}+{\frac {s^{3}\kappa '(0)}{6}}\right)\mathbf {N} (0)+\left({\frac {s^{3}\kappa (0)\tau (0)}{6}}\right)\mathbf {B} (0)+o(s^{3})}
3937:
2736:
5340:
A ribbon defined by a curve of constant torsion and a highly oscillating curvature. The arc length parameterization of the curve was defined via integration of the Frenet–Serret equations.
4624:
2062:
1702:
536:
3742:
3706:
A top whose axis is situated along the binormal is observed to rotate with angular speed κ. If the axis is along the tangent, it is observed to rotate with angular speed τ.
1094:
7695:
7592:
3764:
In physics, the Frenet–Serret frame is useful when it is impossible or inconvenient to assign a natural coordinate system for a trajectory. Such is often the case, for instance, in
7654:
7551:
4170:
4237:
5841:{\displaystyle {\frac {\mathrm {d} (QM)}{\mathrm {d} s}}(QM)^{\top }={\frac {\mathrm {d} Q}{\mathrm {d} s}}MM^{\top }Q^{\top }={\frac {\mathrm {d} Q}{\mathrm {d} s}}Q^{\top }}
5658:
3458:
3312:
1640:
184:
103:
6771:
4008:
Two helices (slinkies) in space. (a) A more compact helix with higher curvature and lower torsion. (b) A stretched out helix with slightly higher torsion but lower curvature.
4250:
the radius.) In particular, curvature and torsion are complementary in the sense that the torsion can be increased at the expense of curvature by stretching out the slinky.
3480:
3429:
3283:
7616:
5308:{\displaystyle \mathbf {r} (0)+\left(s-{\frac {s^{3}\kappa ^{2}(0)}{6}}\right)\mathbf {T} (0)+\left({\frac {s^{3}\kappa (0)\tau (0)}{6}}\right)\mathbf {B} (0)+o(s^{3})}
4859:
4823:
4783:
7873:
6483:{\displaystyle \mathbf {B} (t)=\mathbf {T} (t)\times \mathbf {N} (t)={\frac {\mathbf {r} '(t)\times \mathbf {r} ''(t)}{\|\mathbf {r} '(t)\times \mathbf {r} ''(t)\|}}}
1354:
798:
7715:
3494:
and the curvature κ, and the third Frenet-Serret formula holds by the definition of the torsion τ. Thus what is needed is to show the second Frenet-Serret formula.
1378:
449:
of the space curve. (Intuitively, curvature measures the failure of a curve to be a straight line, while torsion measures the failure of a curve to be planar.) The
7882:
3320:
2546:
7513:
7446:
7221:
2706:{\displaystyle {\mathbf {e} _{n}}(s)={\mathbf {e} _{1}}(s)\times {\mathbf {e} _{2}}(s)\times \dots \times {\mathbf {e} _{n-2}}(s)\times {\mathbf {e} _{n-1}}(s)}
2316:{\displaystyle {\begin{aligned}\mathbf {e} _{j}(s)={\frac {{\overline {\mathbf {e} _{j}}}(s)}{\|{\overline {\mathbf {e} _{j}}}(s)\|}}{\mbox{, }}\end{aligned}}}
974:
7720:
7327:
7226:
940:{\displaystyle \mathbf {N} :={{\frac {\mathrm {d} \mathbf {T} }{\mathrm {d} s}} \over \left\|{\frac {\mathrm {d} \mathbf {T} }{\mathrm {d} s}}\right\|},}
6891:
3252:
Notice that as defined here, the generalized curvatures and the frame may differ slightly from the convention found in other sources. The top curvature
5972:
643:
5445:
if one can be rigidly moved to the other. A rigid motion consists of a combination of a translation and a rotation. A translation moves one point of
5568:
can all be given as successive derivatives of the parametrization of the curve, each of them is insensitive to the addition of a constant vector to
1052:
5943:, because the arclength is a Euclidean invariant of the curve. In the terminology of physics, the arclength parametrization is a natural choice of
5375:
is the surface traced out by sweeping the line segment generated by the unit normal along the curve. This surface is sometimes confused with the
2031:{\displaystyle {\overline {\mathbf {e} _{2}}}(s)=\mathbf {r} ''(s)-\langle \mathbf {r} ''(s),\mathbf {e} _{1}(s)\rangle \,\mathbf {e} _{1}(s)}
8605:
8201:
4861:. This can be seen from the above Taylor expansion. Thus in a sense the osculating plane is the closest plane to the curve at a given point.
124:, in 1851. Vector notation and linear algebra currently used to write these formulas were not yet available at the time of their discovery.
3852:
The kinematic significance of the curvature is best illustrated with plane curves (having constant torsion equal to zero). See the page on
4016:
in which the helix twists around its central axis. Explicitly, the parametrization of a single turn of a right-handed helix with height 2π
8376:(1974), "On Cartan's method of Lie groups and moving frames as applied to uniqueness and existence questions in differential geometry",
1819:
8352:
3460:, and this change of sign makes the frame positively oriented. As defined above, the frame inherits its orientation from the jet of
3398:(the orientation of the basis) from the usual torsion. The Frenet–Serret formulas are invariant under flipping the sign of both
633:), since many different particle paths may trace out the same geometrical curve by traversing it at different rates. In detail,
8292:
Crenshaw, H.C.; Edelstein-Keshet, L. (1993), "Orientation by
Helical Motion II. Changing the direction of the axis of motion",
7128:
630:
8520:
4183:
to explain the meaning of the torsion and curvature. The slinky, he says, is characterized by the property that the quantity
8172:
can be chosen as the unit vector orthogonal to the span of the others, such that the resulting frame is positively oriented.
105:, or the geometric properties of the curve itself irrespective of any motion. More specifically, the formulas describe the
3768:. Within this setting, Frenet–Serret frames have been used to model the precession of a gyroscope in a gravitational well.
8638:
7451:
3943:
8685:
2858:{\displaystyle \chi _{i}(s)={\frac {\langle \mathbf {e} _{i}'(s),\mathbf {e} _{i+1}(s)\rangle }{\|\mathbf {r} '(s)\|}}}
3887:
2163:{\displaystyle \mathbf {e} _{2}(s)={\frac {{\overline {\mathbf {e} _{2}}}(s)}{\|{\overline {\mathbf {e} _{2}}}(s)\|}}}
1803:{\displaystyle \mathbf {e} _{1}(s)={\frac {{\overline {\mathbf {e} _{1}}}(s)}{\|{\overline {\mathbf {e} _{1}}}(s)\|}}}
116:
in terms of each other. The formulas are named after the two French mathematicians who independently discovered them:
8773:
8710:
8416:
8271:
8862:
8125:
3723:
8595:
500:
8852:
8660:
5912:
4581:
For a generic curve with nonvanishing torsion, the projection of the curve onto various coordinate planes in the
8616:
8611:
5895:
of the curve under
Euclidean motions: if a Euclidean motion is applied to a curve, then the resulting curve has
8847:
5947:. However, it may be awkward to work with in practice. A number of other equivalent expressions are available.
4789:(0). The osculating plane has the special property that the distance from the curve to the osculating plane is
8512:
489:
vectors at two points on a plane curve, a translated version of the second frame (dotted), and the change in
7659:
7556:
7621:
7518:
4131:
3688:
3734:
about the tangent vector, and similarly the top will rotate in the opposite direction of this precession.
3730:
direction of the circular motion. In the limiting case when the curvature vanishes, the observer's normal
8740:
6493:
An alternative way to arrive at the same expressions is to take the first three derivatives of the curve
6871:{\displaystyle \kappa ={\frac {\|\mathbf {r} '(t)\times \mathbf {r} ''(t)\|}{\|\mathbf {r} '(t)\|^{3}}}}
3881:
of a single turn. The curvature and torsion of a helix (with constant radius) are given by the formulas
8130:
4189:
8596:
Create your own animated illustrations of moving Frenet-Serret frames, curvature and torsion functions
5631:
4738:{\displaystyle \mathbf {r} (0)+s\mathbf {T} (0)+{\frac {s^{2}\kappa (0)}{2}}\mathbf {N} (0)+o(s^{2}).}
3434:
3288:
1616:
160:
79:
8378:
8100:
5939:
depend on the curve being given in terms of the arclength parameter. This is a natural assumption in
117:
5556:
The Frenet–Serret frame is particularly well-behaved with regard to
Euclidean motions. First, since
8803:
8778:
8700:
8263:
8165: − 1 actually need to be linearly independent, as the final remaining frame vector
5462:
8205:
3463:
8750:
8631:
4866:
4258:
Repeatedly differentiating the curve and applying the Frenet–Serret formulas gives the following
3719:
3401:
3255:
952:
8755:
8745:
7597:
5380:
3866:
3853:
4828:
4792:
4752:
8652:
8440:
Iyer, B.R.; Vishveshwara, C.V. (1993), "Frenet-Serret description of gyroscopic precession",
7858:
6882:
1583:
1339:
58:
8538:
8330:
8255:
8068:{\displaystyle \kappa ={\frac {|x'(t)y''(t)-y'(t)x''(t)|}{((x'(t))^{2}+(y'(t))^{2})^{3/2}}}}
3388:{\displaystyle \operatorname {or} \left(\mathbf {r} ^{(1)},\dots ,\mathbf {r} ^{(n)}\right)}
2194:
The remaining vectors in the frame (the binormal, trinormal, etc.) are defined similarly by
566:
of the particle as a function of time. The Frenet–Serret formulas apply to curves which are
8530:
8459:
8351:
Goriely, A.; Robertson-Tessi, M.; Tabor, M.; Vandiver, R. (2006), "Elastic growth models",
8105:
7700:
6518:
4242:
remains constant if the slinky is vertically stretched out along its central axis. (Here 2π
1655:
1363:
454:
121:
8361:
740:) is a strictly monotonically increasing function. Therefore, it is possible to solve for
8:
8793:
8765:
8720:
8256:
7050:
If the curvature is always zero then the curve will be a straight line. Here the vectors
5376:
4259:
3799:
2525:
8463:
7495:
7428:
7203:
1021:{\displaystyle \kappa =\left\|{\frac {\mathrm {d} \mathbf {T} }{\mathrm {d} s}}\right\|}
8725:
8675:
8624:
8483:
8449:
8395:
8309:
8092:
7848:{\displaystyle {\frac {||{\bf {r}}'(t)\times {\bf {r}}''(t)||}{||{\bf {r}}'(t)||^{3}}}}
5940:
5904:
5423:
5414:
are equal to these osculating planes. The Frenet ribbon is in general not developable.
3791:
3669:
8426:
8305:
6529:
frame. This procedure also generalizes to produce Frenet frames in higher dimensions.
5915:
asserts that the curves are congruent. In particular, the curvature and torsion are a
1598:
The Frenet–Serret formulas were generalized to higher-dimensional
Euclidean spaces by
8516:
8487:
8475:
8412:
8373:
8267:
8086:
6522:
5361:
5357:
5353:
3765:
3676:
3661:
1651:
1381:
446:
152:
8399:
8313:
7656:
if, when viewed from above, the curve's trajectory is turning leftward, and will be
7418:{\displaystyle {\displaystyle {\bf {N}}={\frac {{\bf {T}}'(t)}{||{\bf {T}}'(t)||}}}}
7317:{\displaystyle {\displaystyle {\bf {T}}={\frac {{\bf {r}}'(t)}{||{\bf {r}}'(t)||}}}}
3843:
8788:
8690:
8599:
8494:
Jordan, Camille (1874), "Sur la théorie des courbes dans l'espace à n dimensions",
8467:
8387:
8301:
5316:
4606:
3692:
3673:
2179:
1894:, indicates the deviance of the curve from being a straight line. It is defined as
626:
212:
43:
8391:
7035:{\displaystyle \tau ={\frac {}{\|\mathbf {r} '(t)\times \mathbf {r} ''(t)\|^{2}}}}
8857:
8783:
8695:
8646:
8526:
6765:
Explicit expressions for the curvature and torsion may be computed. For example,
5911:
frame. If the
Darboux derivatives of two frames are equal, then a version of the
5426:, one is interested in studying the properties of figures in the plane which are
4013:
563:
559:
74:
20:
6048:{\displaystyle \mathbf {T} (t)={\frac {\mathbf {r} '(t)}{\|\mathbf {r} '(t)\|}}}
5609:
This leaves only the rotations to consider. Intuitively, if we apply a rotation
4116:
Note that these are not the arc length parametrizations (in which case, each of
842:{\displaystyle \mathbf {T} :={\frac {\mathrm {d} \mathbf {r} }{\mathrm {d} s}}.}
718:{\displaystyle s(t)=\int _{0}^{t}\left\|\mathbf {r} '(\sigma )\right\|d\sigma .}
19:"Binormal" redirects here. For the category-theoretic meaning of this word, see
8816:
8811:
8730:
8557:
5097:
3696:
1599:
194:
3826:
At the peaks of the torsion function the rotation of the Frenet–Serret frame (
3636:
8841:
8735:
8471:
8110:
3758:
1038:
222:
204:
8539:"Sur quelques formules relatives à la théorie des courbes à double courbure"
3285:(also called the torsion, in this context) and the last vector in the frame
768:)). The curve is thus parametrized in a preferred manner by its arc length.
8479:
8120:
5944:
3711:
587:
2522:
The last vector in the frame is defined by the cross-product of the first
8821:
7120:
4825:, while the distance from the curve to any other plane is no better than
4611:
4176:
4012:
The sign of the torsion is determined by the right-handed or left-handed
625:
is used to give the curve traced out by the trajectory of the particle a
155:
113:
8427:"Quaternion Frenet Frames: Making Optimal Tubes and Ribbons from Curves"
4004:
1650:
are linearly independent. The vectors in the Frenet–Serret frame are an
8115:
6545:
5625:
vectors of the Frenet–Serret frame changes by the matrix of a rotation
3809:
3683:
610:
106:
8454:
7064:
A curve may have nonzero curvature and zero torsion. For example, the
3490:
The first Frenet-Serret formula holds by the definition of the normal
8670:
8648:
3824:, along with the curvature κ(s), and the torsion τ(s) are displayed.
3715:
1357:
779:), parameterized by its arc length, it is now possible to define the
571:
438:
66:
3753:
The kinematics of the frame have many applications in the sciences.
3702:
8826:
8350:
4746:
3865:
The Frenet–Serret formulas are frequently introduced in courses on
1093:
575:
8562:
A Comprehensive
Introduction to Differential Geometry (Volume Two)
7061:
If the torsion is always zero then the curve will lie in a plane.
1876:{\displaystyle {\overline {\mathbf {e} _{1}}}(s)=\mathbf {r} '(s)}
5344:
The Frenet–Serret apparatus allows one to define certain optimal
3731:
8511:, Student Mathematical Library, vol. 16, Providence, R.I.:
5406:
where these sheets intersect, approach the osculating planes of
5336:
7065:
6536:, the Frenet–Serret formulas pick up an additional factor of ||
4180:
542:
and the curvature describes the speed of rotation of the frame.
5461:′. Such a combination of translation and rotation is called a
3722:. If the top points in the direction of the binormal, then by
1685:
In detail, the unit tangent vector is the first Frenet vector
1083:{\displaystyle \mathbf {B} :=\mathbf {T} \times \mathbf {N} ,}
7108:
3870:
3641:
1098:
614:
555:
127:
The tangent, normal, and binormal unit vectors, often called
70:
8322:
Salas and Hille's
Calculus — One and Several Variables
5352:
centered around a curve. These have diverse applications in
3710:
Concretely, suppose that the observer carries an (inertial)
3545:. Differentiating the last equation with respect to s gives
4878:. The projection of the curve onto this plane has the form:
4621:. The projection of the curve onto this plane has the form:
4266: = 0 if the curve is parameterized by arclength:
3695:
of the observer's coordinate system is proportional to the
477:
5962:
need no longer be arclength. Then the unit tangent vector
5453:′. The rotation then adjusts the orientation of the curve
1391:, and can be stated more concisely using matrix notation:
26:
8291:
7193:{\displaystyle {\bf {r}}(t)=\langle x(t),y(t),0\rangle }
3869:
as a companion to the study of space curves such as the
69:
properties of a particle moving along a differentiable
8320:
Etgen, Garret; Hille, Einar; Salas, Saturnino (1995),
6718:
6649:
6582:
4175:
In his expository writings on the geometry of curves,
3485:
3171:
3005:
2891:
2303:
1532:
1463:
1406:
505:
497:. δs is the distance between the points. In the limit
7885:
7861:
7723:
7703:
7697:
if it is turning rightward. As a result, the torsion
7662:
7624:
7600:
7559:
7521:
7498:
7454:
7431:
7332:
7330:
7231:
7229:
7206:
7131:
6894:
6774:
6557:
6332:
6071:
5975:
5698:
5634:
5390:. This is perhaps because both the Frenet ribbon and
5129:
4884:
4831:
4795:
4755:
4627:
4275:
4192:
4134:
3946:
3890:
3860:
3466:
3437:
3404:
3323:
3291:
3258:
2881:
2739:
2557:
2528:
2330:
2203:
2065:
1903:
1822:
1705:
1619:
1400:
1366:
1342:
1157:
1055:
977:
861:
801:
646:
503:
246:
163:
82:
8082:
7485:{\displaystyle {\bf {B}}={\bf {T}}\times {\bf {N}}}
7100:=0 plane has zero torsion and curvature equal to 1/
5919:set of invariants for a curve in three-dimensions.
4246:is the height of a single twist of the slinky, and
3994:{\displaystyle \tau =\pm {\frac {h}{r^{2}+h^{2}}}.}
8324:(7th ed.), John Wiley & Sons, p. 896
8067:
7867:
7847:
7709:
7689:
7648:
7610:
7586:
7545:
7507:
7484:
7440:
7417:
7316:
7215:
7192:
7034:
6870:
6754:
6482:
6308:
6047:
5840:
5652:
5307:
5088:
4853:
4817:
4777:
4737:
4570:
4231:
4164:
3993:
3931:
3648:The Frenet–Serret frame consisting of the tangent
3626:
3623:This is exactly the second Frenet-Serret formula.
3474:
3452:
3423:
3387:
3306:
3277:
3241:
2857:
2705:
2540:
2511:
2315:
2162:
2030:
1875:
1802:
1634:
1571:
1372:
1348:
1325:
1082:
1020:
939:
841:
717:
530:
414:
197:to the curve, pointing in the direction of motion.
178:
97:
8612:Very nice visual representation for the trihedron
8262:. Englewood Cliffs, N.J., Prentice-Hall. p.
5922:
5123:. The projection of the curve onto this plane is:
8839:
8439:
5410:; the tangent planes of the Frenet ribbon along
3932:{\displaystyle \kappa ={\frac {r}{r^{2}+h^{2}}}}
8319:
5617:frame also rotates. More precisely, the matrix
5398:. Namely, the tangent planes of both sheets of
3873:. A helix can be characterized by the height 2π
3838:) around the tangent vector is clearly visible.
7448:-plane. As a result, the unit binormal vector
8632:
7111:has constant curvature and constant torsion.
3664:of 3-space. At each point of the curve, this
1387:The Frenet–Serret formulas are also known as
570:, which roughly means that they have nonzero
433:is the derivative with respect to arclength,
8546:Journal de Mathématiques Pures et Appliquées
8406:
8342:Journal de Mathématiques Pures et Appliquées
7684:
7663:
7643:
7625:
7581:
7560:
7540:
7522:
7187:
7151:
7020:
6975:
6856:
6833:
6828:
6784:
6641:
6619:
6474:
6430:
6135:
6113:
6039:
6017:
5481:is a composite of the following operations:
2990:
2968:
2849:
2827:
2822:
2765:
2477:
2423:
2296:
2265:
2154:
2123:
2003:
1957:
1794:
1763:
1028:we automatically obtain the first relation.
531:{\displaystyle {\tfrac {d\mathbf {T} }{ds}}}
8581:Lectures on Classical Differential Geometry
8204:. San Jose State University. Archived from
8202:"Watching Flies Fly: Kappatau Space Curves"
2173:The tangent and the normal vector at point
1589:
8639:
8625:
3772:
3631:
8569:
8453:
8372:
8253:
6251:
2480:
2006:
1622:
166:
85:
5335:
4003:
3701:
3635:
1092:
967:, since there is no change in length of
476:
25:
5417:
3640:The Frenet–Serret frame moving along a
1097:The Frenet–Serret frame moving along a
613:which the particle has moved along the
598:) are required not to be proportional.
574:. More formally, in this situation the
8840:
8578:
8556:
8536:
8506:
8493:
8424:
8328:
8218:
8199:
8149:
7690:{\displaystyle \langle 0,0,-1\rangle }
7587:{\displaystyle \langle 0,0,-1\rangle }
7058:and the torsion are not well defined.
2716:The real valued functions used below χ
1109:is represented by the red arrow while
8620:
8193:
7649:{\displaystyle \langle 0,0,1\rangle }
7546:{\displaystyle \langle 0,0,1\rangle }
6881:The torsion may be expressed using a
4165:{\displaystyle {\sqrt {h^{2}+r^{2}}}}
1141:are all perpendicular to each other.
728:Moreover, since we have assumed that
7717:will always be zero and the formula
5331:
4600:have the following interpretations:
215:of the curve, divided by its length.
8434:Indiana University Technical Report
5950:Suppose that the curve is given by
4785:, whose curvature at 0 is equal to
4253:
3682:The Frenet–Serret formulas admit a
3486:Proof of the Frenet-Serret formulas
13:
8686:Radius of curvature (applications)
6567:
6561:
5833:
5818:
5808:
5796:
5786:
5768:
5758:
5746:
5722:
5703:
5465:. In terms of the parametrization
3861:Frenet–Serret formulas in calculus
3778:Example of a moving Frenet basis (
3738:
1288:
1276:
1226:
1214:
1178:
1166:
1113:is represented by the black arrow.
1105:is represented by the blue arrow,
1004:
992:
918:
906:
888:
876:
826:
814:
377:
365:
315:
303:
267:
255:
14:
8874:
8774:Curvature of Riemannian manifolds
8589:
8572:Lectures on Differential Geometry
8360:, Springer-Verlag, archived from
8332:Sur les courbes à double courbure
8258:Lectures on Differential Geometry
7324:and principal unit normal vector
7223:-plane, then its tangent vector
5394:exhibit similar properties along
4232:{\displaystyle A^{2}=h^{2}+r^{2}}
3509:are orthogonal unit vectors with
2872:, stated in matrix language, are
971:. Note that by calling curvature
221:is the binormal unit vector, the
16:Formulas in differential geometry
8294:Bulletin of Mathematical Biology
8126:Tangential and normal components
8085:
7807:
7764:
7740:
7603:
7477:
7467:
7457:
7382:
7349:
7335:
7281:
7248:
7234:
7134:
7045:
7002:
6980:
6953:
6931:
6909:
6838:
6811:
6789:
6740:
6731:
6722:
6624:
6604:
6595:
6586:
6457:
6435:
6411:
6389:
6368:
6351:
6334:
6281:
6259:
6229:
6198:
6176:
6149:
6118:
6094:
6073:
6022:
5998:
5977:
5653:{\displaystyle Q\rightarrow QM.}
5592:frame attached to the new curve
5477:, a general Euclidean motion of
5315:which traces out the graph of a
5270:
5202:
5131:
5051:
4983:
4886:
4697:
4649:
4629:
4530:
4462:
4365:
4294:
4277:
3842:
3798:
3737:The general case is illustrated
3724:conservation of angular momentum
3468:
3453:{\displaystyle \mathbf {e} _{n}}
3440:
3364:
3337:
3307:{\displaystyle \mathbf {e} _{n}}
3294:
3208:
3176:
2973:
2931:
2896:
2832:
2797:
2770:
2677:
2645:
2613:
2587:
2561:
2483:
2458:
2428:
2368:
2339:
2272:
2239:
2210:
2130:
2097:
2068:
2009:
1984:
1962:
1937:
1908:
1856:
1827:
1770:
1737:
1708:
1635:{\displaystyle \mathbb {R} ^{n}}
1554:
1545:
1536:
1439:
1425:
1411:
1312:
1281:
1261:
1250:
1219:
1199:
1171:
1121:is always perpendicular to both
1073:
1065:
1057:
997:
911:
881:
863:
819:
803:
684:
512:
401:
370:
350:
339:
308:
288:
260:
237:The Frenet–Serret formulas are:
179:{\displaystyle \mathbb {R} ^{3}}
98:{\displaystyle \mathbb {R} ^{3}}
8583:, Reading, Mass: Addison-Wesley
8407:Guggenheimer, Heinrich (1977),
7114:
5913:fundamental theorem of calculus
4112:(0 ≤ t ≤ 2 π).
3748:
3627:Applications and interpretation
1129:. Thus, the three unit vectors
207:unit vector, the derivative of
8246:
8237:
8224:
8212:
8184:
8175:
8155:
8143:
8045:
8035:
8031:
8025:
8014:
8002:
7998:
7992:
7981:
7978:
7972:
7968:
7962:
7951:
7945:
7931:
7925:
7914:
7908:
7896:
7832:
7826:
7822:
7816:
7800:
7795:
7788:
7783:
7779:
7773:
7755:
7749:
7733:
7728:
7515:plane and thus must be either
7406:
7401:
7397:
7391:
7375:
7370:
7364:
7358:
7305:
7300:
7296:
7290:
7274:
7269:
7263:
7257:
7178:
7172:
7163:
7157:
7145:
7139:
7016:
7010:
6994:
6988:
6970:
6967:
6961:
6945:
6939:
6923:
6917:
6904:
6852:
6846:
6825:
6819:
6803:
6797:
6638:
6632:
6471:
6465:
6449:
6443:
6425:
6419:
6403:
6397:
6378:
6372:
6361:
6355:
6344:
6338:
6299:
6295:
6289:
6273:
6267:
6253:
6247:
6243:
6237:
6223:
6212:
6206:
6190:
6184:
6163:
6157:
6132:
6126:
6108:
6102:
6083:
6077:
6036:
6030:
6012:
6006:
5987:
5981:
5923:Other expressions of the frame
5861:for the matrix of a rotation.
5742:
5732:
5716:
5707:
5638:
5302:
5289:
5280:
5274:
5256:
5250:
5244:
5238:
5212:
5206:
5187:
5181:
5141:
5135:
5083:
5070:
5061:
5055:
5037:
5031:
5025:
5019:
4993:
4987:
4968:
4962:
4929:
4923:
4896:
4890:
4848:
4835:
4812:
4799:
4772:
4759:
4729:
4716:
4707:
4701:
4687:
4681:
4659:
4653:
4639:
4633:
4562:
4549:
4540:
4534:
4516:
4510:
4504:
4498:
4472:
4466:
4447:
4441:
4408:
4402:
4375:
4369:
4350:
4344:
4304:
4298:
4287:
4281:
4070:and, for a left-handed helix,
4066:(0 ≤ t ≤ 2 π)
3375:
3369:
3348:
3342:
3224:
3218:
3192:
3186:
3150:
3144:
3112:
3106:
3061:
3055:
3029:
3023:
2987:
2981:
2950:
2944:
2915:
2909:
2846:
2840:
2819:
2813:
2789:
2783:
2756:
2750:
2700:
2694:
2668:
2662:
2630:
2624:
2604:
2598:
2578:
2572:
2499:
2493:
2474:
2468:
2450:
2444:
2439:
2433:
2390:
2384:
2379:
2373:
2360:
2354:
2293:
2287:
2260:
2254:
2226:
2220:
2151:
2145:
2118:
2112:
2084:
2078:
2045:, is the second Frenet vector
2025:
2019:
2000:
1994:
1976:
1970:
1951:
1945:
1929:
1923:
1870:
1864:
1848:
1842:
1791:
1785:
1758:
1752:
1724:
1718:
1014:
985:
928:
899:
702:
698:
692:
678:
656:
650:
472:
1:
8513:American Mathematical Society
8392:10.1215/S0012-7094-74-04180-5
8306:10.1016/s0092-8240(05)80070-9
8285:
8190:Iyer and Vishveshwara (1993).
5927:The formulas given above for
5689:is unaffected by a rotation:
5433:Roughly speaking, two curves
963:) is always perpendicular to
947:from which it follows, since
732:′ ≠ 0, it follows that
465:, is called collectively the
120:, in his thesis of 1847, and
111:tangent, normal, and binormal
8606:Rudy Rucker's KappaTau Paper
5552:is the matrix of a rotation.
5386:of the osculating planes of
4128:would need to be divided by
3475:{\displaystyle \mathbf {r} }
2349:
2282:
2249:
2140:
2107:
1918:
1837:
1780:
1747:
1654:constructed by applying the
771:With a non-degenerate curve
453:basis combined with the two
186:and are defined as follows:
7:
8078:
5473:) defining the first curve
3424:{\displaystyle \chi _{n-1}}
3278:{\displaystyle \chi _{n-1}}
1117:from which it follows that
30:A space curve; the vectors
10:
8879:
8570:Sternberg, Shlomo (1964),
8131:Radial, transverse, normal
7118:
6532:In terms of the parameter
5402:, near the singular locus
3820:, and the binormal vector
631:arc-length parametrization
18:
8802:
8764:
8709:
8659:
8564:, Publish or Perish, Inc.
8507:Kühnel, Wolfgang (2002),
8379:Duke Mathematical Journal
8101:Affine geometry of curves
7611:{\displaystyle {\bf {B}}}
7594:. By the right-hand rule
3854:curvature of plane curves
2041:Its normalized form, the
1033:The binormal unit vector
538:will be in the direction
8804:Curvature of connections
8779:Riemann curvature tensor
8701:Total absolute curvature
8579:Struik, Dirk J. (1961),
8472:10.1103/physrevd.48.5706
8136:
7492:is perpendicular to the
6521:. The resulting ordered
5457:to line up with that of
5115:is the plane containing
4870:is the plane containing
4854:{\displaystyle O(s^{2})}
4818:{\displaystyle O(s^{3})}
4778:{\displaystyle O(s^{2})}
791:The tangent unit vector
8863:Curvature (mathematics)
8751:Second fundamental form
8741:Gauss–Codazzi equations
7868:{\displaystyle \kappa }
5958:), where the parameter
5899:curvature and torsion.
5613:to the curve, then the
4179:employs the model of a
3851:
3807:
3773:Graphical Illustrations
3720:uniform circular motion
3632:Kinematics of the frame
1890:, sometimes called the
1613:) is a smooth curve in
1349:{\displaystyle \kappa }
851:The normal unit vector
627:natural parametrization
467:Frenet–Serret apparatus
8853:Multivariable calculus
8756:Third fundamental form
8746:First fundamental form
8711:Differential geometry
8681:Frenet–Serret formulas
8661:Differential geometry
8537:Serret, J. A. (1851),
8496:C. R. Acad. Sci. Paris
8069:
7869:
7849:
7711:
7691:
7650:
7612:
7588:
7547:
7509:
7486:
7442:
7419:
7318:
7217:
7194:
7036:
6872:
6756:
6513:′′′(
6484:
6310:
6049:
5842:
5654:
5341:
5309:
5090:
4855:
4819:
4779:
4739:
4572:
4233:
4166:
4009:
3995:
3933:
3867:multivariable calculus
3726:it must rotate in the
3707:
3660:collectively forms an
3645:
3476:
3454:
3425:
3389:
3308:
3279:
3243:
2870:Frenet–Serret formulas
2859:
2707:
2542:
2513:
2422:
2317:
2164:
2032:
1877:
1804:
1636:
1573:
1374:
1350:
1327:
1146:Frenet–Serret formulas
1114:
1084:
1022:
941:
843:
719:
543:
532:
416:
180:
139:, or collectively the
99:
63:Frenet–Serret formulas
54:
8848:Differential geometry
8653:differential geometry
8509:Differential geometry
8425:Hanson, A.J. (2007),
8409:Differential Geometry
8252:For terminology, see
8200:Rucker, Rudy (1999).
8070:
7870:
7850:
7712:
7710:{\displaystyle \tau }
7692:
7651:
7613:
7589:
7548:
7510:
7487:
7443:
7425:will also lie in the
7420:
7319:
7218:
7195:
7119:Further information:
7037:
6883:scalar triple product
6873:
6757:
6485:
6311:
6050:
5843:
5655:
5588:) is the same as the
5513:is a constant vector.
5339:
5310:
5091:
4856:
4820:
4780:
4749:up to terms of order
4740:
4593:coordinate system at
4573:
4234:
4167:
4007:
3996:
3934:
3812:, the tangent vector
3705:
3639:
3477:
3455:
3426:
3390:
3309:
3280:
3244:
2860:
2728:generalized curvature
2708:
2543:
2514:
2396:
2318:
2165:
2033:
1878:
1805:
1642:, and that the first
1637:
1574:
1389:Frenet–Serret theorem
1375:
1373:{\displaystyle \tau }
1351:
1328:
1096:
1085:
1023:
942:
844:
720:
533:
480:
417:
181:
100:
73:in three-dimensional
59:differential geometry
29:
8721:Principal curvatures
8106:Differentiable curve
7883:
7859:
7721:
7701:
7660:
7622:
7598:
7557:
7519:
7496:
7452:
7429:
7328:
7227:
7204:
7200:is contained in the
7129:
6892:
6772:
6555:
6519:Gram-Schmidt process
6517:), and to apply the
6330:
6069:
5973:
5696:
5632:
5576:). Intuitively, the
5418:Congruence of curves
5127:
4882:
4829:
4793:
4753:
4625:
4273:
4260:Taylor approximation
4190:
4132:
3944:
3888:
3816:, the normal vector
3808:On the example of a
3741:. There are further
3464:
3435:
3402:
3321:
3289:
3256:
2879:
2737:
2555:
2526:
2328:
2201:
2063:
1901:
1820:
1703:
1696:) and is defined as
1656:Gram-Schmidt process
1617:
1398:
1364:
1340:
1155:
1053:
975:
859:
799:
748:, and thus to write
644:
629:by arc length (i.e.
501:
244:
211:with respect to the
161:
151:), together form an
122:Joseph Alfred Serret
118:Jean Frédéric Frenet
80:
8794:Sectional curvature
8766:Riemannian geometry
8647:Various notions of
8464:1993PhRvD..48.5706I
8329:Frenet, F. (1847),
8208:on 15 October 2004.
6544:)|| because of the
5621:whose rows are the
5377:tangent developable
3314:, differ by a sign
2943:
2908:
2782:
2730:and are defined as
2541:{\displaystyle n-1}
781:Frenet–Serret frame
676:
562:, representing the
213:arclength parameter
193:is the unit vector
141:Frenet–Serret frame
8726:Gaussian curvature
8676:Torsion of a curve
8374:Griffiths, Phillip
8254:Sternberg (1964).
8093:Mathematics portal
8065:
7865:
7855:for the curvature
7845:
7707:
7687:
7646:
7608:
7584:
7543:
7508:{\displaystyle xy}
7505:
7482:
7441:{\displaystyle xy}
7438:
7415:
7413:
7314:
7312:
7216:{\displaystyle xy}
7213:
7190:
7032:
6868:
6752:
6746:
6707:
6610:
6480:
6306:
6058:The normal vector
6045:
5966:may be written as
5941:Euclidean geometry
5905:Darboux derivative
5864:Hence the entries
5838:
5650:
5580:frame attached to
5424:Euclidean geometry
5342:
5305:
5086:
4851:
4815:
4775:
4735:
4568:
4262:to the curve near
4229:
4162:
4010:
3991:
3929:
3708:
3670:frame of reference
3646:
3472:
3450:
3421:
3385:
3304:
3275:
3239:
3237:
3229:
3160:
2966:
2955:
2929:
2894:
2855:
2768:
2703:
2538:
2509:
2507:
2313:
2311:
2307:
2160:
2043:unit normal vector
2028:
1873:
1800:
1632:
1569:
1560:
1521:
1449:
1370:
1346:
1323:
1321:
1115:
1080:
1037:is defined as the
1018:
937:
839:
715:
662:
544:
528:
526:
412:
410:
176:
95:
55:
8835:
8834:
8522:978-0-8218-2656-0
8448:(12): 5706–5720,
8338:, Thèse, Toulouse
8063:
7843:
7411:
7310:
7030:
6866:
6575:
6525:is precisely the
6523:orthonormal basis
6478:
6304:
6139:
6043:
5826:
5776:
5730:
5362:computer graphics
5358:elasticity theory
5354:materials science
5332:Ribbons and tubes
5263:
5194:
5044:
4975:
4936:
4694:
4523:
4454:
4415:
4357:
4160:
3986:
3927:
3790:in purple) along
3766:relativity theory
3677:coordinate system
3662:orthonormal basis
2853:
2352:
2306:
2300:
2285:
2252:
2158:
2143:
2110:
2056:) and defined as
1921:
1840:
1798:
1783:
1750:
1652:orthonormal basis
1296:
1234:
1186:
1012:
932:
926:
896:
834:
744:as a function of
525:
385:
323:
275:
153:orthonormal basis
109:of the so-called
8870:
8789:Scalar curvature
8691:Affine curvature
8641:
8634:
8627:
8618:
8617:
8584:
8575:
8565:
8552:
8543:
8533:
8503:
8490:
8457:
8436:
8431:
8421:
8402:
8368:
8366:
8359:
8339:
8337:
8325:
8316:
8279:
8277:
8261:
8250:
8244:
8241:
8235:
8228:
8222:
8216:
8210:
8209:
8197:
8191:
8188:
8182:
8181:Crenshaw (1993).
8179:
8173:
8159:
8153:
8147:
8095:
8090:
8089:
8074:
8072:
8071:
8066:
8064:
8062:
8061:
8060:
8056:
8043:
8042:
8024:
8010:
8009:
7991:
7976:
7975:
7961:
7944:
7924:
7907:
7899:
7893:
7874:
7872:
7871:
7866:
7854:
7852:
7851:
7846:
7844:
7842:
7841:
7840:
7835:
7829:
7815:
7811:
7810:
7803:
7798:
7792:
7791:
7786:
7772:
7768:
7767:
7748:
7744:
7743:
7736:
7731:
7725:
7716:
7714:
7713:
7708:
7696:
7694:
7693:
7688:
7655:
7653:
7652:
7647:
7617:
7615:
7614:
7609:
7607:
7606:
7593:
7591:
7590:
7585:
7552:
7550:
7549:
7544:
7514:
7512:
7511:
7506:
7491:
7489:
7488:
7483:
7481:
7480:
7471:
7470:
7461:
7460:
7447:
7445:
7444:
7439:
7424:
7422:
7421:
7416:
7414:
7412:
7410:
7409:
7404:
7390:
7386:
7385:
7378:
7373:
7367:
7357:
7353:
7352:
7344:
7339:
7338:
7323:
7321:
7320:
7315:
7313:
7311:
7309:
7308:
7303:
7289:
7285:
7284:
7277:
7272:
7266:
7256:
7252:
7251:
7243:
7238:
7237:
7222:
7220:
7219:
7214:
7199:
7197:
7196:
7191:
7138:
7137:
7041:
7039:
7038:
7033:
7031:
7029:
7028:
7027:
7009:
7005:
6987:
6983:
6973:
6960:
6956:
6938:
6934:
6916:
6912:
6902:
6877:
6875:
6874:
6869:
6867:
6865:
6864:
6863:
6845:
6841:
6831:
6818:
6814:
6796:
6792:
6782:
6761:
6759:
6758:
6753:
6751:
6750:
6743:
6734:
6725:
6712:
6711:
6631:
6627:
6615:
6614:
6607:
6598:
6589:
6576:
6574:
6570:
6564:
6559:
6489:
6487:
6486:
6481:
6479:
6477:
6464:
6460:
6442:
6438:
6428:
6418:
6414:
6396:
6392:
6385:
6371:
6354:
6337:
6315:
6313:
6312:
6307:
6305:
6303:
6302:
6298:
6288:
6284:
6266:
6262:
6250:
6246:
6236:
6232:
6220:
6219:
6215:
6205:
6201:
6183:
6179:
6156:
6152:
6145:
6140:
6138:
6125:
6121:
6111:
6101:
6097:
6090:
6076:
6054:
6052:
6051:
6046:
6044:
6042:
6029:
6025:
6015:
6005:
6001:
5994:
5980:
5887:
5885:
5884:
5879:
5876:
5860:
5847:
5845:
5844:
5839:
5837:
5836:
5827:
5825:
5821:
5815:
5811:
5805:
5800:
5799:
5790:
5789:
5777:
5775:
5771:
5765:
5761:
5755:
5750:
5749:
5731:
5729:
5725:
5719:
5706:
5700:
5685:
5683:
5682:
5677:
5674:
5659:
5657:
5656:
5651:
5605:
5463:Euclidean motion
5360:, as well as to
5317:cubic polynomial
5314:
5312:
5311:
5306:
5301:
5300:
5273:
5268:
5264:
5259:
5234:
5233:
5223:
5205:
5200:
5196:
5195:
5190:
5180:
5179:
5170:
5169:
5159:
5134:
5113:rectifying plane
5095:
5093:
5092:
5087:
5082:
5081:
5054:
5049:
5045:
5040:
5015:
5014:
5004:
4986:
4981:
4977:
4976:
4971:
4961:
4953:
4952:
4942:
4937:
4932:
4919:
4918:
4908:
4889:
4860:
4858:
4857:
4852:
4847:
4846:
4824:
4822:
4821:
4816:
4811:
4810:
4784:
4782:
4781:
4776:
4771:
4770:
4744:
4742:
4741:
4736:
4728:
4727:
4700:
4695:
4690:
4677:
4676:
4666:
4652:
4632:
4607:osculating plane
4599:
4577:
4575:
4574:
4569:
4561:
4560:
4533:
4528:
4524:
4519:
4494:
4493:
4483:
4465:
4460:
4456:
4455:
4450:
4440:
4432:
4431:
4421:
4416:
4411:
4398:
4397:
4387:
4368:
4363:
4359:
4358:
4353:
4343:
4342:
4333:
4332:
4322:
4297:
4280:
4254:Taylor expansion
4238:
4236:
4235:
4230:
4228:
4227:
4215:
4214:
4202:
4201:
4171:
4169:
4168:
4163:
4161:
4159:
4158:
4146:
4145:
4136:
4000:
3998:
3997:
3992:
3987:
3985:
3984:
3983:
3971:
3970:
3957:
3938:
3936:
3935:
3930:
3928:
3926:
3925:
3924:
3912:
3911:
3898:
3846:
3802:
3693:angular momentum
3481:
3479:
3478:
3473:
3471:
3459:
3457:
3456:
3451:
3449:
3448:
3443:
3430:
3428:
3427:
3422:
3420:
3419:
3394:
3392:
3391:
3386:
3384:
3380:
3379:
3378:
3367:
3352:
3351:
3340:
3313:
3311:
3310:
3305:
3303:
3302:
3297:
3284:
3282:
3281:
3276:
3274:
3273:
3248:
3246:
3245:
3240:
3238:
3234:
3233:
3217:
3216:
3211:
3185:
3184:
3179:
3165:
3164:
3143:
3142:
3123:
3105:
3104:
3078:
3075:
3054:
3053:
3033:
3022:
3021:
2980:
2976:
2967:
2960:
2959:
2939:
2934:
2904:
2899:
2864:
2862:
2861:
2856:
2854:
2852:
2839:
2835:
2825:
2812:
2811:
2800:
2778:
2773:
2763:
2749:
2748:
2712:
2710:
2709:
2704:
2693:
2692:
2691:
2680:
2661:
2660:
2659:
2648:
2623:
2622:
2621:
2616:
2597:
2596:
2595:
2590:
2571:
2570:
2569:
2564:
2547:
2545:
2544:
2539:
2518:
2516:
2515:
2510:
2508:
2492:
2491:
2486:
2467:
2466:
2461:
2443:
2442:
2431:
2421:
2410:
2383:
2382:
2371:
2353:
2348:
2347:
2342:
2336:
2322:
2320:
2319:
2314:
2312:
2308:
2304:
2301:
2299:
2286:
2281:
2280:
2275:
2269:
2263:
2253:
2248:
2247:
2242:
2236:
2233:
2219:
2218:
2213:
2180:osculating plane
2169:
2167:
2166:
2161:
2159:
2157:
2144:
2139:
2138:
2133:
2127:
2121:
2111:
2106:
2105:
2100:
2094:
2091:
2077:
2076:
2071:
2037:
2035:
2034:
2029:
2018:
2017:
2012:
1993:
1992:
1987:
1969:
1965:
1944:
1940:
1922:
1917:
1916:
1911:
1905:
1892:curvature vector
1882:
1880:
1879:
1874:
1863:
1859:
1841:
1836:
1835:
1830:
1824:
1809:
1807:
1806:
1801:
1799:
1797:
1784:
1779:
1778:
1773:
1767:
1761:
1751:
1746:
1745:
1740:
1734:
1731:
1717:
1716:
1711:
1658:to the vectors (
1641:
1639:
1638:
1633:
1631:
1630:
1625:
1578:
1576:
1575:
1570:
1565:
1564:
1557:
1548:
1539:
1526:
1525:
1454:
1453:
1446:
1445:
1432:
1431:
1418:
1417:
1379:
1377:
1376:
1371:
1355:
1353:
1352:
1347:
1332:
1330:
1329:
1324:
1322:
1315:
1297:
1295:
1291:
1285:
1284:
1279:
1273:
1264:
1253:
1235:
1233:
1229:
1223:
1222:
1217:
1211:
1202:
1187:
1185:
1181:
1175:
1174:
1169:
1163:
1089:
1087:
1086:
1081:
1076:
1068:
1060:
1027:
1025:
1024:
1019:
1017:
1013:
1011:
1007:
1001:
1000:
995:
989:
951:always has unit
946:
944:
943:
938:
933:
931:
927:
925:
921:
915:
914:
909:
903:
897:
895:
891:
885:
884:
879:
873:
871:
866:
848:
846:
845:
840:
835:
833:
829:
823:
822:
817:
811:
806:
724:
722:
721:
716:
705:
701:
691:
687:
675:
670:
609:) represent the
537:
535:
534:
529:
527:
524:
516:
515:
506:
421:
419:
418:
413:
411:
404:
386:
384:
380:
374:
373:
368:
362:
353:
342:
324:
322:
318:
312:
311:
306:
300:
291:
276:
274:
270:
264:
263:
258:
252:
185:
183:
182:
177:
175:
174:
169:
104:
102:
101:
96:
94:
93:
88:
44:osculating plane
8878:
8877:
8873:
8872:
8871:
8869:
8868:
8867:
8838:
8837:
8836:
8831:
8798:
8784:Ricci curvature
8760:
8712:
8705:
8696:Total curvature
8662:
8655:
8645:
8592:
8574:, Prentice-Hall
8558:Spivak, Michael
8541:
8523:
8429:
8419:
8364:
8357:
8335:
8288:
8283:
8282:
8274:
8251:
8247:
8242:
8238:
8229:
8225:
8217:
8213:
8198:
8194:
8189:
8185:
8180:
8176:
8171:
8161:Only the first
8160:
8156:
8148:
8144:
8139:
8091:
8084:
8081:
8052:
8048:
8044:
8038:
8034:
8017:
8005:
8001:
7984:
7977:
7971:
7954:
7937:
7917:
7900:
7895:
7894:
7892:
7884:
7881:
7880:
7876:
7860:
7857:
7856:
7836:
7831:
7830:
7825:
7806:
7805:
7804:
7799:
7794:
7793:
7787:
7782:
7763:
7762:
7761:
7739:
7738:
7737:
7732:
7727:
7726:
7724:
7722:
7719:
7718:
7702:
7699:
7698:
7661:
7658:
7657:
7623:
7620:
7619:
7602:
7601:
7599:
7596:
7595:
7558:
7555:
7554:
7520:
7517:
7516:
7497:
7494:
7493:
7476:
7475:
7466:
7465:
7456:
7455:
7453:
7450:
7449:
7430:
7427:
7426:
7405:
7400:
7381:
7380:
7379:
7374:
7369:
7368:
7348:
7347:
7346:
7345:
7343:
7334:
7333:
7331:
7329:
7326:
7325:
7304:
7299:
7280:
7279:
7278:
7273:
7268:
7267:
7247:
7246:
7245:
7244:
7242:
7233:
7232:
7230:
7228:
7225:
7224:
7205:
7202:
7201:
7133:
7132:
7130:
7127:
7126:
7123:
7117:
7048:
7023:
7019:
7001:
7000:
6979:
6978:
6974:
6952:
6951:
6930:
6929:
6908:
6907:
6903:
6901:
6893:
6890:
6889:
6859:
6855:
6837:
6836:
6832:
6810:
6809:
6788:
6787:
6783:
6781:
6773:
6770:
6769:
6745:
6744:
6739:
6736:
6735:
6730:
6727:
6726:
6721:
6714:
6713:
6706:
6705:
6700:
6692:
6686:
6685:
6680:
6675:
6666:
6665:
6660:
6655:
6645:
6644:
6623:
6622:
6609:
6608:
6603:
6600:
6599:
6594:
6591:
6590:
6585:
6578:
6577:
6566:
6565:
6560:
6558:
6556:
6553:
6552:
6505:′′(
6456:
6455:
6434:
6433:
6429:
6410:
6409:
6388:
6387:
6386:
6384:
6367:
6350:
6333:
6331:
6328:
6327:
6280:
6279:
6258:
6257:
6256:
6252:
6228:
6227:
6226:
6222:
6221:
6197:
6196:
6175:
6174:
6173:
6169:
6148:
6147:
6146:
6144:
6117:
6116:
6112:
6093:
6092:
6091:
6089:
6072:
6070:
6067:
6066:
6062:takes the form
6021:
6020:
6016:
5997:
5996:
5995:
5993:
5976:
5974:
5971:
5970:
5925:
5880:
5877:
5872:
5871:
5869:
5852:
5832:
5828:
5817:
5816:
5807:
5806:
5804:
5795:
5791:
5785:
5781:
5767:
5766:
5757:
5756:
5754:
5745:
5741:
5721:
5720:
5702:
5701:
5699:
5697:
5694:
5693:
5678:
5675:
5670:
5669:
5667:
5633:
5630:
5629:
5593:
5441:′ in space are
5420:
5379:, which is the
5334:
5296:
5292:
5269:
5229:
5225:
5224:
5222:
5218:
5201:
5175:
5171:
5165:
5161:
5160:
5158:
5151:
5147:
5130:
5128:
5125:
5124:
5077:
5073:
5050:
5010:
5006:
5005:
5003:
4999:
4982:
4954:
4948:
4944:
4943:
4941:
4914:
4910:
4909:
4907:
4906:
4902:
4885:
4883:
4880:
4879:
4842:
4838:
4830:
4827:
4826:
4806:
4802:
4794:
4791:
4790:
4766:
4762:
4754:
4751:
4750:
4723:
4719:
4696:
4672:
4668:
4667:
4665:
4648:
4628:
4626:
4623:
4622:
4594:
4556:
4552:
4529:
4489:
4485:
4484:
4482:
4478:
4461:
4433:
4427:
4423:
4422:
4420:
4393:
4389:
4388:
4386:
4385:
4381:
4364:
4338:
4334:
4328:
4324:
4323:
4321:
4314:
4310:
4293:
4276:
4274:
4271:
4270:
4256:
4223:
4219:
4210:
4206:
4197:
4193:
4191:
4188:
4187:
4154:
4150:
4141:
4137:
4135:
4133:
4130:
4129:
3979:
3975:
3966:
3962:
3961:
3956:
3945:
3942:
3941:
3920:
3916:
3907:
3903:
3902:
3897:
3889:
3886:
3885:
3863:
3825:
3792:Viviani's curve
3775:
3751:
3656:, and binormal
3634:
3629:
3587:, this becomes
3521:, one also has
3488:
3467:
3465:
3462:
3461:
3444:
3439:
3438:
3436:
3433:
3432:
3409:
3405:
3403:
3400:
3399:
3368:
3363:
3362:
3341:
3336:
3335:
3334:
3330:
3322:
3319:
3318:
3298:
3293:
3292:
3290:
3287:
3286:
3263:
3259:
3257:
3254:
3253:
3236:
3235:
3228:
3227:
3212:
3207:
3206:
3203:
3202:
3196:
3195:
3180:
3175:
3174:
3167:
3166:
3159:
3158:
3153:
3132:
3128:
3122:
3116:
3115:
3094:
3090:
3088:
3083:
3076:
3074:
3069:
3064:
3049:
3045:
3039:
3038:
3032:
3017:
3013:
3011:
3001:
3000:
2996:
2972:
2971:
2965:
2964:
2954:
2953:
2935:
2930:
2926:
2925:
2919:
2918:
2900:
2895:
2887:
2886:
2882:
2880:
2877:
2876:
2831:
2830:
2826:
2801:
2796:
2795:
2774:
2769:
2764:
2762:
2744:
2740:
2738:
2735:
2734:
2721:
2681:
2676:
2675:
2674:
2649:
2644:
2643:
2642:
2617:
2612:
2611:
2610:
2591:
2586:
2585:
2584:
2565:
2560:
2559:
2558:
2556:
2553:
2552:
2527:
2524:
2523:
2506:
2505:
2487:
2482:
2481:
2462:
2457:
2456:
2432:
2427:
2426:
2411:
2400:
2372:
2367:
2366:
2343:
2338:
2337:
2335:
2331:
2329:
2326:
2325:
2310:
2309:
2302:
2276:
2271:
2270:
2268:
2264:
2243:
2238:
2237:
2235:
2234:
2232:
2214:
2209:
2208:
2204:
2202:
2199:
2198:
2134:
2129:
2128:
2126:
2122:
2101:
2096:
2095:
2093:
2092:
2090:
2072:
2067:
2066:
2064:
2061:
2060:
2051:
2013:
2008:
2007:
1988:
1983:
1982:
1961:
1960:
1936:
1935:
1912:
1907:
1906:
1904:
1902:
1899:
1898:
1855:
1854:
1831:
1826:
1825:
1823:
1821:
1818:
1817:
1774:
1769:
1768:
1766:
1762:
1741:
1736:
1735:
1733:
1732:
1730:
1712:
1707:
1706:
1704:
1701:
1700:
1691:
1670:′′(
1646:derivatives of
1626:
1621:
1620:
1618:
1615:
1614:
1596:
1582:This matrix is
1559:
1558:
1553:
1550:
1549:
1544:
1541:
1540:
1535:
1528:
1527:
1520:
1519:
1514:
1506:
1500:
1499:
1494:
1489:
1480:
1479:
1474:
1469:
1459:
1458:
1448:
1447:
1438:
1437:
1434:
1433:
1424:
1423:
1420:
1419:
1410:
1409:
1402:
1401:
1399:
1396:
1395:
1365:
1362:
1361:
1341:
1338:
1337:
1320:
1319:
1311:
1298:
1287:
1286:
1280:
1275:
1274:
1272:
1269:
1268:
1260:
1249:
1236:
1225:
1224:
1218:
1213:
1212:
1210:
1207:
1206:
1198:
1188:
1177:
1176:
1170:
1165:
1164:
1162:
1158:
1156:
1153:
1152:
1072:
1064:
1056:
1054:
1051:
1050:
1003:
1002:
996:
991:
990:
988:
984:
976:
973:
972:
959:(the change of
917:
916:
910:
905:
904:
902:
898:
887:
886:
880:
875:
874:
872:
870:
862:
860:
857:
856:
825:
824:
818:
813:
812:
810:
802:
800:
797:
796:
683:
682:
681:
677:
671:
666:
645:
642:
641:
621:. The quantity
594:′′(
564:position vector
560:Euclidean space
517:
511:
507:
504:
502:
499:
498:
475:
409:
408:
400:
387:
376:
375:
369:
364:
363:
361:
358:
357:
349:
338:
325:
314:
313:
307:
302:
301:
299:
296:
295:
287:
277:
266:
265:
259:
254:
253:
251:
247:
245:
242:
241:
170:
165:
164:
162:
159:
158:
89:
84:
83:
81:
78:
77:
75:Euclidean space
24:
21:normal morphism
17:
12:
11:
5:
8876:
8866:
8865:
8860:
8855:
8850:
8833:
8832:
8830:
8829:
8824:
8819:
8817:Torsion tensor
8814:
8812:Curvature form
8808:
8806:
8800:
8799:
8797:
8796:
8791:
8786:
8781:
8776:
8770:
8768:
8762:
8761:
8759:
8758:
8753:
8748:
8743:
8738:
8733:
8731:Mean curvature
8728:
8723:
8717:
8715:
8707:
8706:
8704:
8703:
8698:
8693:
8688:
8683:
8678:
8673:
8667:
8665:
8657:
8656:
8644:
8643:
8636:
8629:
8621:
8615:
8614:
8609:
8603:
8591:
8590:External links
8588:
8587:
8586:
8576:
8567:
8554:
8534:
8521:
8504:
8491:
8437:
8422:
8417:
8404:
8386:(4): 775–814,
8370:
8348:
8340:. Abstract in
8326:
8317:
8300:(1): 213–230,
8287:
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8211:
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7479:
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7212:
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7136:
7116:
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7047:
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6999:
6996:
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6704:
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6659:
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6408:
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6383:
6380:
6377:
6374:
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6360:
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6340:
6336:
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6297:
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6000:
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5774:
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5709:
5705:
5661:
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5649:
5646:
5643:
5640:
5637:
5554:
5553:
5514:
5449:to a point of
5419:
5416:
5371:along a curve
5333:
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5299:
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5262:
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5211:
5208:
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5168:
5164:
5157:
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5146:
5143:
5140:
5137:
5133:
5109:
5098:cuspidal cubic
5085:
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4110:
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4085:
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3990:
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3839:
3806:
3796:
3795:
3774:
3771:
3770:
3769:
3762:
3750:
3747:
3745:on Wikimedia.
3699:of the frame.
3697:Darboux vector
3633:
3630:
3628:
3625:
3487:
3484:
3470:
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3418:
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3408:
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3333:
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3250:
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2016:
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1629:
1624:
1600:Camille Jordan
1595:
1588:
1584:skew-symmetric
1580:
1579:
1568:
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1552:
1551:
1547:
1543:
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920:
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901:
894:
890:
883:
878:
869:
865:
855:is defined as
849:
838:
832:
828:
821:
816:
809:
805:
795:is defined as
726:
725:
714:
711:
708:
704:
700:
697:
694:
690:
686:
680:
674:
669:
665:
661:
658:
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649:
568:non-degenerate
523:
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510:
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407:
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92:
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15:
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3:
2:
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8809:
8807:
8805:
8801:
8795:
8792:
8790:
8787:
8785:
8782:
8780:
8777:
8775:
8772:
8771:
8769:
8767:
8763:
8757:
8754:
8752:
8749:
8747:
8744:
8742:
8739:
8737:
8736:Darboux frame
8734:
8732:
8729:
8727:
8724:
8722:
8719:
8718:
8716:
8714:
8708:
8702:
8699:
8697:
8694:
8692:
8689:
8687:
8684:
8682:
8679:
8677:
8674:
8672:
8669:
8668:
8666:
8664:
8658:
8654:
8650:
8642:
8637:
8635:
8630:
8628:
8623:
8622:
8619:
8613:
8610:
8607:
8604:
8601:
8597:
8594:
8593:
8582:
8577:
8573:
8568:
8563:
8559:
8555:
8551:
8547:
8540:
8535:
8532:
8528:
8524:
8518:
8514:
8510:
8505:
8501:
8497:
8492:
8489:
8485:
8481:
8477:
8473:
8469:
8465:
8461:
8456:
8455:gr-qc/9310019
8451:
8447:
8443:
8438:
8435:
8428:
8423:
8420:
8418:0-486-63433-7
8414:
8410:
8405:
8401:
8397:
8393:
8389:
8385:
8381:
8380:
8375:
8371:
8367:on 2006-12-29
8363:
8356:
8355:
8349:
8346:
8343:
8334:
8333:
8327:
8323:
8318:
8315:
8311:
8307:
8303:
8299:
8295:
8290:
8289:
8275:
8273:9780135271506
8269:
8265:
8260:
8259:
8249:
8240:
8233:
8227:
8220:
8215:
8207:
8203:
8196:
8187:
8178:
8168:
8164:
8158:
8151:
8146:
8142:
8132:
8129:
8127:
8124:
8122:
8119:
8117:
8114:
8112:
8111:Darboux frame
8109:
8107:
8104:
8102:
8099:
8098:
8094:
8088:
8083:
8057:
8053:
8049:
8039:
8028:
8021:
8018:
8011:
8006:
7995:
7988:
7985:
7965:
7958:
7955:
7948:
7941:
7938:
7934:
7928:
7921:
7918:
7911:
7904:
7901:
7889:
7886:
7879:
7878:
7877:
7862:
7837:
7819:
7812:
7776:
7769:
7758:
7752:
7745:
7704:
7681:
7678:
7675:
7672:
7669:
7666:
7640:
7637:
7634:
7631:
7628:
7578:
7575:
7572:
7569:
7566:
7563:
7537:
7534:
7531:
7528:
7525:
7502:
7499:
7472:
7462:
7435:
7432:
7394:
7387:
7361:
7354:
7340:
7293:
7286:
7260:
7253:
7239:
7210:
7207:
7184:
7181:
7175:
7169:
7166:
7160:
7154:
7148:
7142:
7122:
7112:
7110:
7105:
7103:
7099:
7095:
7091:
7087:
7083:
7079:
7075:
7071:
7067:
7062:
7059:
7057:
7053:
7046:Special cases
7024:
7013:
7006:
6997:
6991:
6984:
6964:
6957:
6948:
6942:
6935:
6926:
6920:
6913:
6898:
6895:
6888:
6887:
6886:
6884:
6860:
6849:
6842:
6822:
6815:
6806:
6800:
6793:
6778:
6775:
6768:
6767:
6766:
6747:
6715:
6708:
6702:
6697:
6694:
6689:
6682:
6677:
6672:
6669:
6662:
6657:
6652:
6646:
6635:
6628:
6616:
6611:
6579:
6571:
6551:
6550:
6549:
6547:
6543:
6539:
6535:
6530:
6528:
6524:
6520:
6516:
6512:
6508:
6504:
6500:
6496:
6468:
6461:
6452:
6446:
6439:
6422:
6415:
6406:
6400:
6393:
6381:
6375:
6364:
6358:
6347:
6341:
6326:
6325:
6324:
6322:
6319:The binormal
6292:
6285:
6276:
6270:
6263:
6240:
6233:
6216:
6209:
6202:
6193:
6187:
6180:
6170:
6166:
6160:
6153:
6141:
6129:
6122:
6105:
6098:
6086:
6080:
6065:
6064:
6063:
6061:
6033:
6026:
6009:
6002:
5990:
5984:
5969:
5968:
5967:
5965:
5961:
5957:
5953:
5948:
5946:
5942:
5938:
5934:
5930:
5920:
5918:
5914:
5910:
5906:
5900:
5898:
5894:
5890:
5883:
5875:
5867:
5862:
5859:
5855:
5829:
5822:
5812:
5801:
5792:
5782:
5778:
5772:
5762:
5751:
5738:
5735:
5726:
5713:
5710:
5692:
5691:
5690:
5688:
5681:
5673:
5666:, the matrix
5665:
5647:
5644:
5641:
5635:
5628:
5627:
5626:
5624:
5620:
5616:
5612:
5607:
5604:
5600:
5596:
5591:
5587:
5583:
5579:
5575:
5571:
5567:
5563:
5559:
5551:
5547:
5543:
5539:
5535:
5531:
5527:
5523:
5519:
5515:
5512:
5508:
5504:
5500:
5496:
5492:
5488:
5484:
5483:
5482:
5480:
5476:
5472:
5468:
5464:
5460:
5456:
5452:
5448:
5444:
5440:
5436:
5431:
5429:
5425:
5422:In classical
5415:
5413:
5409:
5405:
5401:
5397:
5393:
5389:
5385:
5382:
5378:
5374:
5370:
5369:Frenet ribbon
5365:
5363:
5359:
5355:
5351:
5347:
5338:
5326:
5322:
5318:
5297:
5293:
5286:
5283:
5277:
5265:
5260:
5253:
5247:
5241:
5235:
5230:
5226:
5219:
5215:
5209:
5197:
5191:
5184:
5176:
5172:
5166:
5162:
5155:
5152:
5148:
5144:
5138:
5122:
5118:
5114:
5110:
5107:
5103:
5099:
5078:
5074:
5067:
5064:
5058:
5046:
5041:
5034:
5028:
5022:
5016:
5011:
5007:
5000:
4996:
4990:
4978:
4972:
4965:
4958:
4955:
4949:
4945:
4938:
4933:
4926:
4920:
4915:
4911:
4903:
4899:
4893:
4877:
4873:
4869:
4868:
4863:
4843:
4839:
4832:
4807:
4803:
4796:
4788:
4767:
4763:
4756:
4748:
4732:
4724:
4720:
4713:
4710:
4704:
4691:
4684:
4678:
4673:
4669:
4662:
4656:
4645:
4642:
4636:
4620:
4616:
4613:
4610:is the plane
4609:
4608:
4603:
4602:
4601:
4597:
4592:
4588:
4584:
4565:
4557:
4553:
4546:
4543:
4537:
4525:
4520:
4513:
4507:
4501:
4495:
4490:
4486:
4479:
4475:
4469:
4457:
4451:
4444:
4437:
4434:
4428:
4424:
4417:
4412:
4405:
4399:
4394:
4390:
4382:
4378:
4372:
4360:
4354:
4347:
4339:
4335:
4329:
4325:
4318:
4315:
4311:
4307:
4301:
4290:
4284:
4269:
4268:
4267:
4265:
4261:
4251:
4249:
4245:
4224:
4220:
4216:
4211:
4207:
4203:
4198:
4194:
4186:
4185:
4184:
4182:
4178:
4173:
4155:
4151:
4147:
4142:
4138:
4127:
4123:
4119:
4111:
4109:
4106:
4102:
4099:
4097:
4093:
4089:
4086:
4084:
4080:
4076:
4073:
4072:
4071:
4065:
4063:
4060:
4056:
4053:
4051:
4047:
4043:
4040:
4038:
4034:
4030:
4027:
4026:
4025:
4023:
4019:
4015:
4006:
3988:
3980:
3976:
3972:
3967:
3963:
3958:
3953:
3950:
3947:
3940:
3921:
3917:
3913:
3908:
3904:
3899:
3894:
3891:
3884:
3883:
3882:
3880:
3876:
3872:
3868:
3855:
3849:
3848:
3847:
3845:
3837:
3833:
3829:
3823:
3819:
3815:
3811:
3805:
3804:
3803:
3801:
3793:
3789:
3785:
3781:
3777:
3776:
3767:
3763:
3760:
3759:life sciences
3756:
3755:
3754:
3746:
3744:
3743:illustrations
3740:
3735:
3733:
3729:
3725:
3721:
3717:
3713:
3704:
3700:
3698:
3694:
3690:
3685:
3680:
3679:(see image).
3678:
3675:
3671:
3667:
3663:
3659:
3655:
3651:
3643:
3638:
3624:
3621:
3620:
3616:
3611:
3609:
3605:
3601:
3597:
3593:
3588:
3586:
3582:
3578:
3574:
3569:
3567:
3563:
3559:
3555:
3551:
3546:
3544:
3540:
3536:
3532:
3528:
3524:
3520:
3516:
3512:
3508:
3504:
3500:
3495:
3493:
3483:
3445:
3416:
3413:
3410:
3406:
3381:
3372:
3359:
3356:
3353:
3345:
3331:
3327:
3324:
3317:
3316:
3315:
3299:
3270:
3267:
3264:
3260:
3230:
3221:
3213:
3199:
3189:
3181:
3168:
3161:
3155:
3147:
3139:
3136:
3133:
3129:
3125:
3119:
3109:
3101:
3098:
3095:
3091:
3085:
3080:
3071:
3066:
3058:
3050:
3046:
3042:
3035:
3026:
3018:
3014:
3008:
3002:
2993:
2984:
2977:
2961:
2956:
2947:
2940:
2936:
2922:
2912:
2905:
2901:
2888:
2875:
2874:
2873:
2871:
2843:
2836:
2816:
2808:
2805:
2802:
2792:
2786:
2779:
2775:
2759:
2753:
2745:
2741:
2733:
2732:
2731:
2729:
2726:) are called
2725:
2720:
2697:
2688:
2685:
2682:
2671:
2665:
2656:
2653:
2650:
2639:
2636:
2633:
2627:
2618:
2607:
2601:
2592:
2581:
2575:
2566:
2551:
2550:
2549:
2535:
2532:
2529:
2502:
2496:
2488:
2471:
2463:
2453:
2447:
2436:
2418:
2415:
2412:
2407:
2404:
2401:
2397:
2393:
2387:
2376:
2363:
2357:
2344:
2324:
2290:
2277:
2257:
2244:
2229:
2223:
2215:
2197:
2196:
2195:
2192:
2190:
2186:
2182:
2181:
2176:
2148:
2135:
2115:
2102:
2087:
2081:
2073:
2059:
2058:
2057:
2055:
2048:
2044:
2022:
2014:
1997:
1989:
1979:
1973:
1966:
1954:
1948:
1941:
1932:
1926:
1913:
1897:
1896:
1895:
1893:
1889:
1888:normal vector
1867:
1860:
1851:
1845:
1832:
1816:
1815:
1814:
1788:
1775:
1755:
1742:
1727:
1721:
1713:
1699:
1698:
1697:
1695:
1688:
1683:
1681:
1677:
1673:
1669:
1665:
1661:
1657:
1653:
1649:
1645:
1627:
1612:
1608:
1605:Suppose that
1603:
1601:
1593:
1587:
1585:
1566:
1561:
1529:
1522:
1516:
1511:
1508:
1503:
1496:
1491:
1486:
1483:
1476:
1471:
1466:
1460:
1455:
1450:
1442:
1428:
1414:
1403:
1394:
1393:
1392:
1390:
1385:
1383:
1367:
1359:
1343:
1316:
1308:
1305:
1302:
1300:
1292:
1265:
1257:
1254:
1246:
1243:
1240:
1238:
1230:
1203:
1195:
1192:
1190:
1182:
1151:
1150:
1149:
1147:
1142:
1140:
1136:
1132:
1128:
1124:
1120:
1112:
1108:
1104:
1100:
1095:
1077:
1069:
1061:
1048:
1044:
1040:
1039:cross product
1036:
1032:
1031:
1008:
981:
978:
970:
966:
962:
958:
954:
950:
934:
922:
892:
867:
854:
850:
836:
830:
807:
794:
790:
789:
788:
786:
782:
778:
774:
769:
767:
763:
759:
755:
751:
747:
743:
739:
735:
731:
712:
709:
706:
695:
688:
672:
667:
663:
659:
653:
647:
640:
639:
638:
636:
632:
628:
624:
620:
616:
612:
608:
604:
599:
597:
593:
589:
585:
581:
577:
573:
569:
565:
561:
557:
553:
549:
541:
521:
518:
508:
496:
492:
488:
484:
479:
470:
468:
464:
460:
456:
452:
448:
444:
440:
436:
432:
428:
405:
397:
394:
391:
389:
381:
354:
346:
343:
335:
332:
329:
327:
319:
292:
284:
281:
279:
271:
240:
239:
238:
232:
228:
224:
223:cross product
220:
217:
214:
210:
206:
202:
199:
196:
192:
189:
188:
187:
171:
157:
154:
150:
146:
142:
138:
134:
130:
125:
123:
119:
115:
112:
108:
90:
76:
72:
68:
65:describe the
64:
60:
53:
49:
45:
41:
37:
33:
28:
22:
8680:
8580:
8571:
8561:
8549:
8545:
8508:
8499:
8495:
8445:
8441:
8433:
8408:
8383:
8377:
8362:the original
8353:
8344:
8341:
8331:
8321:
8297:
8293:
8257:
8248:
8239:
8231:
8226:
8221:, p. 19
8214:
8206:the original
8195:
8186:
8177:
8166:
8162:
8157:
8145:
8121:Moving frame
7124:
7115:Plane curves
7106:
7101:
7097:
7096:, 0) in the
7093:
7089:
7085:
7081:
7077:
7073:
7069:
7063:
7060:
7055:
7051:
7049:
6885:as follows,
6880:
6764:
6541:
6537:
6533:
6531:
6526:
6514:
6510:
6506:
6502:
6498:
6494:
6492:
6320:
6318:
6059:
6057:
5963:
5959:
5955:
5951:
5949:
5936:
5932:
5928:
5926:
5916:
5908:
5901:
5896:
5892:
5888:
5881:
5873:
5865:
5863:
5857:
5853:
5850:
5686:
5679:
5671:
5663:
5662:
5622:
5618:
5614:
5610:
5608:
5602:
5598:
5594:
5589:
5585:
5581:
5577:
5573:
5569:
5565:
5561:
5557:
5555:
5549:
5545:
5541:
5537:
5533:
5529:
5525:
5521:
5517:
5510:
5506:
5502:
5498:
5494:
5490:
5486:
5478:
5474:
5470:
5466:
5458:
5454:
5450:
5446:
5442:
5438:
5434:
5432:
5427:
5421:
5411:
5407:
5403:
5399:
5395:
5391:
5387:
5383:
5372:
5368:
5366:
5349:
5345:
5343:
5324:
5320:
5120:
5116:
5112:
5105:
5101:
4875:
4871:
4867:normal plane
4865:
4786:
4618:
4614:
4605:
4595:
4590:
4586:
4582:
4580:
4263:
4257:
4247:
4243:
4241:
4174:
4125:
4121:
4117:
4115:
4107:
4104:
4100:
4095:
4091:
4087:
4082:
4078:
4074:
4069:
4061:
4058:
4054:
4049:
4045:
4041:
4036:
4032:
4028:
4021:
4017:
4011:
3878:
3874:
3864:
3841:
3835:
3831:
3827:
3821:
3817:
3813:
3797:
3787:
3783:
3779:
3752:
3749:Applications
3736:
3727:
3709:
3689:non-inertial
3681:
3665:
3657:
3653:
3649:
3647:
3622:
3618:
3614:
3612:
3607:
3603:
3599:
3595:
3591:
3589:
3584:
3580:
3576:
3572:
3571:Using that ∂
3570:
3565:
3561:
3557:
3553:
3549:
3547:
3542:
3538:
3534:
3530:
3526:
3522:
3518:
3514:
3510:
3506:
3502:
3498:
3496:
3491:
3489:
3397:
3251:
2869:
2867:
2727:
2723:
2718:
2715:
2521:
2193:
2188:
2184:
2178:
2174:
2172:
2053:
2046:
2042:
2040:
1891:
1887:
1885:
1812:
1693:
1686:
1684:
1679:
1675:
1671:
1667:
1663:
1659:
1647:
1643:
1610:
1606:
1604:
1597:
1591:
1590:Formulas in
1581:
1388:
1386:
1335:
1145:
1143:
1138:
1134:
1130:
1126:
1122:
1118:
1116:
1110:
1106:
1102:
1046:
1042:
1034:
968:
964:
960:
956:
948:
852:
792:
784:
780:
776:
772:
770:
765:
761:
757:
753:
749:
745:
741:
737:
733:
729:
727:
637:is given by
634:
622:
618:
606:
602:
600:
595:
591:
588:acceleration
583:
579:
567:
551:
547:
545:
539:
494:
490:
486:
482:
466:
462:
458:
450:
442:
434:
430:
426:
424:
236:
230:
226:
218:
208:
200:
190:
148:
144:
140:
136:
132:
128:
126:
114:unit vectors
110:
62:
56:
51:
47:
39:
35:
31:
8822:Cocurvature
8713:of surfaces
8651:defined in
8354:BIOMAT-2006
8219:Kühnel 2002
8150:Kühnel 2002
7125:If a curve
7121:Plane curve
5487:Translation
5096:which is a
4177:Rudy Rucker
4020:and radius
3877:and radius
3674:rectilinear
3594:/ ∂s = -τ (
2177:define the
473:Definitions
107:derivatives
46:spanned by
8842:Categories
8602:Worksheet)
8442:Phys. Rev.
8286:References
8116:Kinematics
7068:of radius
6546:chain rule
5893:invariants
5664:A fortiori
4745:This is a
4612:containing
3810:torus knot
3786:in green,
1594:dimensions
611:arc length
586:) and the
42:; and the
8671:Curvature
8663:of curves
8649:curvature
8502:: 795–797
8488:119458843
8411:, Dover,
7935:−
7887:κ
7863:κ
7759:×
7705:τ
7685:⟩
7679:−
7664:⟨
7644:⟩
7626:⟨
7582:⟩
7576:−
7561:⟨
7541:⟩
7523:⟨
7473:×
7188:⟩
7152:⟨
7072:given by
7021:‖
6998:×
6976:‖
6896:τ
6857:‖
6834:‖
6829:‖
6807:×
6785:‖
6776:κ
6698:τ
6695:−
6683:τ
6673:κ
6670:−
6658:κ
6642:‖
6620:‖
6475:‖
6453:×
6431:‖
6407:×
6365:×
6277:×
6194:×
6167:×
6136:‖
6114:‖
6040:‖
6018:‖
5868:and τ of
5834:⊤
5797:⊤
5787:⊤
5747:⊤
5639:→
5548:), where
5443:congruent
5428:invariant
5319:to order
5248:τ
5236:κ
5173:κ
5156:−
5100:to order
5029:τ
5017:κ
4956:κ
4921:κ
4679:κ
4508:τ
4496:κ
4435:κ
4400:κ
4336:κ
4319:−
4090:= −
3954:±
3948:τ
3892:κ
3782:in blue,
3732:precesses
3716:gyroscope
3684:kinematic
3652:, normal
3575:/ ∂s = -τ
3552:/ ∂s = (∂
3414:−
3407:χ
3357:…
3328:
3268:−
3261:χ
3200:⋮
3137:−
3130:χ
3126:−
3099:−
3092:χ
3081:⋱
3072:⋱
3067:⋱
3047:χ
3043:−
3015:χ
2994:⋅
2991:‖
2969:‖
2923:⋮
2850:‖
2828:‖
2823:⟩
2766:⟨
2742:χ
2686:−
2672:×
2654:−
2640:×
2637:⋯
2634:×
2608:×
2548:vectors:
2533:−
2478:⟩
2424:⟨
2416:−
2398:∑
2394:−
2350:¯
2297:‖
2283:¯
2266:‖
2250:¯
2183:at point
2155:‖
2141:¯
2124:‖
2108:¯
2004:⟩
1958:⟨
1955:−
1919:¯
1838:¯
1795:‖
1781:¯
1764:‖
1748:¯
1602:in 1874.
1512:τ
1509:−
1497:τ
1487:κ
1484:−
1472:κ
1368:τ
1358:curvature
1344:κ
1309:τ
1306:−
1258:τ
1247:κ
1244:−
1196:κ
1070:×
979:κ
953:magnitude
785:TNB frame
710:σ
696:σ
664:∫
572:curvature
439:curvature
398:τ
395:−
347:τ
336:κ
333:−
285:κ
149:TNB basis
145:TNB frame
67:kinematic
8827:Holonomy
8560:(1999),
8480:10016237
8400:12966544
8314:50734771
8230:Goriely
8079:See also
8022:′
7989:′
7959:″
7942:′
7922:″
7905:′
7875:becomes
7813:′
7770:″
7746:′
7618:will be
7388:′
7355:′
7287:′
7254:′
7007:″
6985:′
6958:‴
6936:″
6914:′
6843:′
6816:″
6794:′
6629:′
6540:′(
6497:′(
6462:″
6440:′
6416:″
6394:′
6323:is then
6300:‖
6286:′
6264:″
6254:‖
6248:‖
6234:′
6224:‖
6203:′
6181:″
6154:′
6123:′
6099:′
6027:′
6003:′
5917:complete
5897:the same
5518:Rotation
5509:, where
5381:envelope
4959:′
4747:parabola
4438:′
3728:opposite
3666:attaches
3644:in space
3583:/ ∂s = κ
3556:/ ∂s) ×
2978:′
2941:′
2906:′
2837:′
2780:′
1967:″
1942:″
1861:′
1674:), ...,
1662:′(
1443:′
1429:′
1415:′
1015:‖
986:‖
929:‖
900:‖
703:‖
689:′
679:‖
617:in time
582:′(
576:velocity
156:spanning
8531:1882174
8460:Bibcode
8347:, 1852.
8243:Hanson.
8234:(2006).
5907:of the
5886:
5870:
5684:
5668:
5346:ribbons
3757:In the
3602:) + κ (
2305:,
1382:torsion
1380:is the
1356:is the
955:, that
590:vector
578:vector
554:) be a
455:scalars
447:torsion
445:is the
437:is the
203:is the
195:tangent
8858:Curves
8529:
8519:
8486:
8478:
8415:
8398:
8312:
8270:
8266:-254.
8232:et al.
8152:, §1.9
7066:circle
5935:, and
5851:since
5564:, and
4181:slinky
4124:, and
3691:. The
3568:/ ∂s)
3505:, and
3497:Since
1813:where
1336:where
1137:, and
1101:. The
441:, and
425:where
205:normal
135:, and
61:, the
8600:Maple
8542:(PDF)
8484:S2CID
8450:arXiv
8444:, D,
8430:(PDF)
8396:S2CID
8365:(PDF)
8358:(PDF)
8336:(PDF)
8310:S2CID
8137:Notes
7109:helix
5945:gauge
5350:tubes
4014:sense
3871:helix
3739:below
3642:helix
3579:and ∂
1148:are:
1099:helix
615:curve
556:curve
71:curve
8517:ISBN
8476:PMID
8413:ISBN
8268:ISBN
7553:or
7092:sin
7084:cos
5891:are
5601:) +
5544:) +
5528:) +
5505:) +
5497:) →
5437:and
5367:The
5356:and
5348:and
5119:and
5111:The
4874:and
4864:The
4617:and
4604:The
4094:sin
4081:cos
4048:sin
4035:cos
3714:(or
3564:× (∂
3533:and
3431:and
2868:The
1886:The
1682:)).
1360:and
1144:The
1125:and
1045:and
783:(or
756:) =
601:Let
546:Let
485:and
481:The
461:and
229:and
50:and
38:and
8468:doi
8388:doi
8302:doi
8264:252
7080:)=(
6527:TNB
6509:),
6501:),
5909:TNB
5623:TNB
5615:TNB
5590:TNB
5578:TNB
5520:)
5489:)
4598:= 0
4172:.)
4024:is
3712:top
3672:or
3617:- κ
3613:= τ
2191:).
1666:),
1041:of
787:):
558:in
493:: δ
451:TNB
225:of
147:or
57:In
8844::
8550:16
8548:,
8544:,
8527:MR
8525:,
8515:,
8500:79
8498:,
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8466:,
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8432:,
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8384:41
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8308:,
8298:55
8296:,
7107:A
7088:,
7054:,
6548::
5931:,
5882:ds
5874:dQ
5856:=
5854:MM
5680:ds
5672:dQ
5606:.
5560:,
5532:→
5364:.
5327:).
5108:).
4589:,
4585:,
4120:,
4103:=
4077:=
4057:=
4044:=
4031:=
3668:a
3610:)
3606:×
3598:×
3560:+
3541:×
3537:=
3529:×
3525:=
3517:×
3513:=
3501:,
3482:.
3325:or
1586:.
1384:.
1133:,
1062::=
1049::
868::=
808::=
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469:.
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431:ds
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8470::
8462::
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7979:(
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7890:=
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7833:|
7827:|
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7820:t
7817:(
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7564:0
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7526:0
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7468:T
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7436:y
7433:x
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7350:T
7341:=
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7301:|
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7291:(
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7270:|
7264:)
7261:t
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7240:=
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7158:(
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7149:=
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7143:t
7140:(
7135:r
7102:R
7098:z
7094:t
7090:R
7086:t
7082:R
7078:t
7076:(
7074:r
7070:R
7056:B
7052:N
7025:2
7017:)
7014:t
7011:(
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6995:)
6992:t
6989:(
6981:r
6971:]
6968:)
6965:t
6962:(
6954:r
6949:,
6946:)
6943:t
6940:(
6932:r
6927:,
6924:)
6921:t
6918:(
6910:r
6905:[
6899:=
6861:3
6853:)
6850:t
6847:(
6839:r
6826:)
6823:t
6820:(
6812:r
6804:)
6801:t
6798:(
6790:r
6779:=
6748:]
6741:B
6732:N
6723:T
6716:[
6709:]
6703:0
6690:0
6678:0
6663:0
6653:0
6647:[
6639:)
6636:t
6633:(
6625:r
6617:=
6612:]
6605:B
6596:N
6587:T
6580:[
6572:t
6568:d
6562:d
6542:t
6538:r
6534:t
6515:t
6511:r
6507:t
6503:r
6499:t
6495:r
6472:)
6469:t
6466:(
6458:r
6450:)
6447:t
6444:(
6436:r
6426:)
6423:t
6420:(
6412:r
6404:)
6401:t
6398:(
6390:r
6382:=
6379:)
6376:t
6373:(
6369:N
6362:)
6359:t
6356:(
6352:T
6348:=
6345:)
6342:t
6339:(
6335:B
6321:B
6296:)
6293:t
6290:(
6282:r
6274:)
6271:t
6268:(
6260:r
6244:)
6241:t
6238:(
6230:r
6217:)
6213:)
6210:t
6207:(
6199:r
6191:)
6188:t
6185:(
6177:r
6171:(
6164:)
6161:t
6158:(
6150:r
6142:=
6133:)
6130:t
6127:(
6119:T
6109:)
6106:t
6103:(
6095:T
6087:=
6084:)
6081:t
6078:(
6074:N
6060:N
6037:)
6034:t
6031:(
6023:r
6013:)
6010:t
6007:(
5999:r
5991:=
5988:)
5985:t
5982:(
5978:T
5964:T
5960:t
5956:t
5954:(
5952:r
5937:B
5933:N
5929:T
5889:Q
5878:/
5866:κ
5858:I
5830:Q
5823:s
5819:d
5813:Q
5809:d
5802:=
5793:Q
5783:M
5779:M
5773:s
5769:d
5763:Q
5759:d
5752:=
5743:)
5739:M
5736:Q
5733:(
5727:s
5723:d
5717:)
5714:M
5711:Q
5708:(
5704:d
5687:Q
5676:/
5648:.
5645:M
5642:Q
5636:Q
5619:Q
5611:M
5603:v
5599:t
5597:(
5595:r
5586:t
5584:(
5582:r
5574:t
5572:(
5570:r
5566:B
5562:N
5558:T
5550:M
5546:v
5542:t
5540:(
5538:r
5536:(
5534:M
5530:v
5526:t
5524:(
5522:r
5516:(
5511:v
5507:v
5503:t
5501:(
5499:r
5495:t
5493:(
5491:r
5485:(
5479:C
5475:C
5471:t
5469:(
5467:r
5459:C
5455:C
5451:C
5447:C
5439:C
5435:C
5412:C
5408:C
5404:C
5400:E
5396:C
5392:E
5388:C
5384:E
5373:C
5325:s
5323:(
5321:o
5303:)
5298:3
5294:s
5290:(
5287:o
5284:+
5281:)
5278:0
5275:(
5271:B
5266:)
5261:6
5257:)
5254:0
5251:(
5245:)
5242:0
5239:(
5231:3
5227:s
5220:(
5216:+
5213:)
5210:0
5207:(
5203:T
5198:)
5192:6
5188:)
5185:0
5182:(
5177:2
5167:3
5163:s
5153:s
5149:(
5145:+
5142:)
5139:0
5136:(
5132:r
5121:B
5117:T
5106:s
5104:(
5102:o
5084:)
5079:3
5075:s
5071:(
5068:o
5065:+
5062:)
5059:0
5056:(
5052:B
5047:)
5042:6
5038:)
5035:0
5032:(
5026:)
5023:0
5020:(
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5008:s
5001:(
4997:+
4994:)
4991:0
4988:(
4984:N
4979:)
4973:6
4969:)
4966:0
4963:(
4950:3
4946:s
4939:+
4934:2
4930:)
4927:0
4924:(
4916:2
4912:s
4904:(
4900:+
4897:)
4894:0
4891:(
4887:r
4876:B
4872:N
4849:)
4844:2
4840:s
4836:(
4833:O
4813:)
4808:3
4804:s
4800:(
4797:O
4787:κ
4773:)
4768:2
4764:s
4760:(
4757:O
4733:.
4730:)
4725:2
4721:s
4717:(
4714:o
4711:+
4708:)
4705:0
4702:(
4698:N
4692:2
4688:)
4685:0
4682:(
4674:2
4670:s
4663:+
4660:)
4657:0
4654:(
4650:T
4646:s
4643:+
4640:)
4637:0
4634:(
4630:r
4619:N
4615:T
4596:s
4591:B
4587:N
4583:T
4566:.
4563:)
4558:3
4554:s
4550:(
4547:o
4544:+
4541:)
4538:0
4535:(
4531:B
4526:)
4521:6
4517:)
4514:0
4511:(
4505:)
4502:0
4499:(
4491:3
4487:s
4480:(
4476:+
4473:)
4470:0
4467:(
4463:N
4458:)
4452:6
4448:)
4445:0
4442:(
4429:3
4425:s
4418:+
4413:2
4409:)
4406:0
4403:(
4395:2
4391:s
4383:(
4379:+
4376:)
4373:0
4370:(
4366:T
4361:)
4355:6
4351:)
4348:0
4345:(
4340:2
4330:3
4326:s
4316:s
4312:(
4308:+
4305:)
4302:0
4299:(
4295:r
4291:=
4288:)
4285:s
4282:(
4278:r
4264:s
4248:r
4244:h
4225:2
4221:r
4217:+
4212:2
4208:h
4204:=
4199:2
4195:A
4156:2
4152:r
4148:+
4143:2
4139:h
4126:z
4122:y
4118:x
4108:t
4105:h
4101:z
4096:t
4092:r
4088:y
4083:t
4079:r
4075:x
4062:t
4059:h
4055:z
4050:t
4046:r
4042:y
4037:t
4033:r
4029:x
4022:r
4018:h
3989:.
3981:2
3977:h
3973:+
3968:2
3964:r
3959:h
3951:=
3922:2
3918:h
3914:+
3909:2
3905:r
3900:r
3895:=
3879:r
3875:h
3856:.
3836:B
3834:,
3832:N
3830:,
3828:T
3822:B
3818:N
3814:T
3794:.
3788:B
3784:N
3780:T
3658:B
3654:N
3650:T
3619:T
3615:B
3608:N
3604:B
3600:T
3596:N
3592:N
3590:∂
3585:N
3581:T
3577:N
3573:B
3566:T
3562:B
3558:T
3554:B
3550:N
3548:∂
3543:T
3539:B
3535:N
3531:B
3527:N
3523:T
3519:N
3515:T
3511:B
3507:B
3503:N
3499:T
3492:N
3469:r
3446:n
3441:e
3417:1
3411:n
3382:)
3376:)
3373:n
3370:(
3365:r
3360:,
3354:,
3349:)
3346:1
3343:(
3338:r
3332:(
3300:n
3295:e
3271:1
3265:n
3231:]
3225:)
3222:s
3219:(
3214:n
3209:e
3193:)
3190:s
3187:(
3182:1
3177:e
3169:[
3162:]
3156:0
3151:)
3148:s
3145:(
3140:1
3134:n
3120:0
3113:)
3110:s
3107:(
3102:1
3096:n
3086:0
3062:)
3059:s
3056:(
3051:1
3036:0
3030:)
3027:s
3024:(
3019:1
3009:0
3003:[
2988:)
2985:s
2982:(
2974:r
2962:=
2957:]
2951:)
2948:s
2945:(
2937:n
2932:e
2916:)
2913:s
2910:(
2902:1
2897:e
2889:[
2847:)
2844:s
2841:(
2833:r
2820:)
2817:s
2814:(
2809:1
2806:+
2803:i
2798:e
2793:,
2790:)
2787:s
2784:(
2776:i
2771:e
2760:=
2757:)
2754:s
2751:(
2746:i
2724:s
2722:(
2719:i
2701:)
2698:s
2695:(
2689:1
2683:n
2678:e
2669:)
2666:s
2663:(
2657:2
2651:n
2646:e
2631:)
2628:s
2625:(
2619:2
2614:e
2605:)
2602:s
2599:(
2593:1
2588:e
2582:=
2579:)
2576:s
2573:(
2567:n
2562:e
2536:1
2530:n
2503:.
2500:)
2497:s
2494:(
2489:i
2484:e
2475:)
2472:s
2469:(
2464:i
2459:e
2454:,
2451:)
2448:s
2445:(
2440:)
2437:j
2434:(
2429:r
2419:1
2413:j
2408:1
2405:=
2402:i
2391:)
2388:s
2385:(
2380:)
2377:j
2374:(
2369:r
2364:=
2361:)
2358:s
2355:(
2345:j
2340:e
2294:)
2291:s
2288:(
2278:j
2273:e
2261:)
2258:s
2255:(
2245:j
2240:e
2230:=
2227:)
2224:s
2221:(
2216:j
2211:e
2189:s
2187:(
2185:r
2175:s
2152:)
2149:s
2146:(
2136:2
2131:e
2119:)
2116:s
2113:(
2103:2
2098:e
2088:=
2085:)
2082:s
2079:(
2074:2
2069:e
2054:s
2052:(
2050:2
2047:e
2026:)
2023:s
2020:(
2015:1
2010:e
2001:)
1998:s
1995:(
1990:1
1985:e
1980:,
1977:)
1974:s
1971:(
1963:r
1952:)
1949:s
1946:(
1938:r
1933:=
1930:)
1927:s
1924:(
1914:2
1909:e
1871:)
1868:s
1865:(
1857:r
1852:=
1849:)
1846:s
1843:(
1833:1
1828:e
1792:)
1789:s
1786:(
1776:1
1771:e
1759:)
1756:s
1753:(
1743:1
1738:e
1728:=
1725:)
1722:s
1719:(
1714:1
1709:e
1694:s
1692:(
1690:1
1687:e
1680:s
1678:(
1676:r
1672:s
1668:r
1664:s
1660:r
1648:r
1644:n
1628:n
1623:R
1611:s
1609:(
1607:r
1592:n
1567:.
1562:]
1555:B
1546:N
1537:T
1530:[
1523:]
1517:0
1504:0
1492:0
1477:0
1467:0
1461:[
1456:=
1451:]
1440:B
1426:N
1412:T
1404:[
1317:,
1313:N
1303:=
1293:s
1289:d
1282:B
1277:d
1266:,
1262:B
1255:+
1251:T
1241:=
1231:s
1227:d
1220:N
1215:d
1204:,
1200:N
1193:=
1183:s
1179:d
1172:T
1167:d
1139:B
1135:N
1131:T
1127:N
1123:T
1119:B
1111:B
1107:N
1103:T
1078:,
1074:N
1066:T
1058:B
1047:N
1043:T
1035:B
1009:s
1005:d
998:T
993:d
982:=
969:T
965:T
961:T
957:N
949:T
935:,
923:s
919:d
912:T
907:d
893:s
889:d
882:T
877:d
864:N
853:N
837:.
831:s
827:d
820:r
815:d
804:T
793:T
777:s
775:(
773:r
766:s
764:(
762:t
760:(
758:r
754:s
752:(
750:r
746:s
742:t
738:t
736:(
734:s
730:r
713:.
707:d
699:)
693:(
685:r
673:t
668:0
660:=
657:)
654:t
651:(
648:s
635:s
623:s
619:t
607:t
605:(
603:s
596:t
592:r
584:t
580:r
552:t
550:(
548:r
540:N
522:s
519:d
513:T
509:d
491:T
487:N
483:T
463:τ
459:κ
443:τ
435:κ
429:/
427:d
406:,
402:N
392:=
382:s
378:d
371:B
366:d
355:,
351:B
344:+
340:T
330:=
320:s
316:d
309:N
304:d
293:,
289:N
282:=
272:s
268:d
261:T
256:d
233:.
231:N
227:T
219:B
209:T
201:N
191:T
172:3
167:R
143:(
137:B
133:N
129:T
91:3
86:R
52:N
48:T
40:B
36:N
32:T
23:.
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