In mathematics, the concept of a **curve** tries to capture the intuitive idea of a geometrical **one-dimensional** and **continuous** object. A simple example is the circle. In everyday use of the term "curve," a straight line is not curved, but in mathematical parlance curves include straight lines and line segments. A large number of other curves have been studied in geometry.

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The term * curve* is also used in ways making it almost synonymous with mathematical function (as in

It is important to distinguish between a *curve* and its *image*. Two distinct curves may have the same image. For example, a line segment can be traced out at different speeds, or a circle can be traversed a different number of times. Often, however, we are just interested in the image of the curve. It is important to pay attention to context and convention when reading about curves.

Terminology is also not uniform. Topologists often use the term "path" for what we call a curve, and "curve" for what we call the image of a curve. The term "curve" is more common in vector calculus and differential geometry.

A curve may be a locus, or a path. That is, it may be a graphical representation of some property of points; or it may be traced out, for example by a stick in the sand on a beach. Of course, if one says curved in ordinary language, it means bent (not straight), so refers to a locus. This leads to the general idea of curvature. Since the formulation of Newtonian dynamics, we have come to understand that for an object to follow a curved path, it must experience acceleration. This understanding is important because major examples of curves are the orbits of planets. One reason for the use of the Ptolemaic system of epicycles and deferents was the special status accorded to the circle as curve.

The conic sections had been studied in depth by Apollonius of Perga. They were applied in astronomy by Kepler. The Greek geometers had studied many other kinds of curves. One reason was their interest in geometric constructions, going beyond compass and straightedge. In that way, the intersection of curves could be used to solve some polynomial equations, such as that involved in trisecting an angle.

Newton also worked on an early example in the calculus of variations. Solutions to variational problems, such as the brachistochrone and tautochrone questions, introduced properties of curves in new ways (in this case, the cycloid). The catenary gets its name as the solution to the problem of a hanging chain, the sort of question that became routinely accessible by means of differential calculus.

In the eighteenth century came the beginnings of the theory of plane algebraic curves, in general. Newton had studied the cubic curves, in the general description of the real points into "ovals." The statement of Bézout's theorem showed a number of aspects that were not directly accessible to the geometry of the time, to do with singular points and complex solutions.

From the nineteenth century, there is not a separate curve theory, but rather the appearance of curves as the one-dimensional aspect of projective geometry, and differential geometry; and later topology, when for example the Jordan curve theorem was understood to lie quite deep, as well as being required in complex analysis. The era of the space-filling curves finally provoked the modern definitions of curve.

In mathematics, a (topological) **curve** is defined as follows. Let be an interval of real numbers (i.e. a non-empty connected subset of ). Then a curve is a continuous mapping , where is a topological space. The curve is said to be **simple** if it is injective, i.e. if for all , in , we have . If is a closed bounded interval , we also allow the possibility (this convention makes it possible to talk about closed simple curve). If for some (other than the extremities of ), then is called a **double** (or **multiple**) **point** of the curve.

A curve is said to be **closed** or **a loop** if and if . A closed curve is thus a continuous mapping of the circle ; a **simple closed curve** is also called a **Jordan curve**.

A **plane curve** is a curve for which *X* is the Euclidean plane — these are the examples first encountered—or in some cases the projective plane. A **space curve** is a curve for which *X* is of three dimensions, usually Euclidean space; a **skew curve** is a space curve which lies in no plane. These definitions also apply to algebraic curves (see below). However, in the case of algebraic curves it is very common not to restrict the curve to having points only defined over the real numbers.

This definition of curve captures our intuitive notion of a curve as a connected, continuous geometric figure that is "like" a line, without thickness and drawn without interruption, although it also includes figures that can hardly be called curves in common usage. For example, the image of a curve can cover a square in the plane (space-filling curve). The image of simple plane curve can have Hausdorff dimension bigger than one (see Koch snowflake) and even positive Lebesgue measure (the last example can be obtained by small variation of the Peano curve construction). The dragon curve is yet another weird example.

*Main article: arc length*

If is a metric space with metric , then we can define the *length* of a curve by

A **rectifiable curve** is a curve with finite length. A parametrization of is called **natural** (or **unit speed** or **parametrised by arc length**) if for any , in , we have

If is a Lipschitz-continuous function, then it is automatically rectifiable. Moreover, in this case, one can define speed of at as

and then

In particular, if is Euclidean space and is differentiable then

While the first examples of curves that are met are mostly plane curves (that is, in everyday words, *curved lines* in *two-dimensional space*), there are obvious examples such as the helix which exist naturally in three dimensions. The needs of geometry, and also for example classical mechanics are to have a notion of curve in space of any number of dimensions. In general relativity, a world line is a curve in spacetime.

If is a differentiable manifold, then we can define the notion of *differentiable curve* in . This general idea is enough to cover many of the applications of curves in mathematics. From a local point of view one can take to be Euclidean space. On the other hand it is useful to be more general, in that (for example) it is possible to define the tangent vectors to by means of this notion of curve.

If is a smooth manifold, a *smooth curve* in is a smooth map

This is a basic notion. There are less and more restricted ideas, too. If is a manifold (i.e., a manifold whose charts are times continuously differentiable), then a curve in is such a curve which is only assumed to be (i.e. times continuously differentiable). If is an analytic manifold (i.e. infinitely differentiable and charts are expressible as power series), and is an analytic map, then is said to be an *analytic curve*.

A differentiable curve is said to be *regular* if its derivative never vanishes. (In words, a regular curve never slows to a stop or backtracks on itself.) Two differentiable curves

- and

are said to be *equivalent* if there is a bijective map

such that the inverse map

is also , and

for all . The map is called a *reparametrisation* of ; and this makes an equivalence relation on the set of all differentiable curves in . A *arc* is an equivalence class of curves under the relation of reparametrisation.

Algebraic curves are the curves considered in algebraic geometry. A plane algebraic curve is the locus of points *f*(*x*, *y*) = 0, where *f*(*x*, *y*) is a polynomial in two variables defined over some field *F*. Algebraic geometry normally looks at such curves in the context of algebraically closed fields. If *K* is the algebraic closure of *F*, and *C* is a curve defined by a polynomial *f*(*x*, *y*) defined over *F*, the points of the curve defined over *F*, consisting of pairs (*a*, *b*) with *a* and *b* in *F*, can be denoted *C*(*F*); the full curve itself being *C*(*K*).

Algebraic curves can also be space curves, or curves in even higher dimensions, obtained as the intersection (common solution set) of more than one polynomial equation in more than two variables. By eliminating variables by means of the resultant, these can be reduced to plane algebraic curves, which, however, may introduce singularities such as cusps or double points. We may also consider these curves to have points defined in the projective plane; if *f*(*x*, *y*) = 0 then if *x* = *u*/*w* and *y* = *v*/*w*, and *n* is the total degree of *f*, then by expanding out *w*^{n}*f*(*u*/*w*, *v*/*w*) = 0 we obtain *g*(*u*, *v*, *w*) = 0, where *g* is homogeneous of degree *n*. An example is the Fermat curve **u**^{n} + **v**^{n} = **w**^{n}, which has an affine form **x**^{n} + **y**^{n} = 1.

Important examples of algebraic curves are the conics, which are nonsingular curves of degree two and genus zero, and elliptic curves, which are nonsingular curves of genus one studied in number theory and which have important applications to cryptography. Because algebraic curves in fields of characteristic zero are most often studied over the complex numbers, algbebraic curves in algebraic geometry look like real surfaces. Looking at them projectively, if we have a nonsingular curve in *n* dimensions, we obtain a picture in the complex projective space of dimension *n*, which corresponds to a real manifold of dimension 2*n*, in which the curve is an embedded smooth and compact surface with a certain number of holes in it, the genus. In fact, non-singular complex projective algebraic curves are compact Riemann surfaces.

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*Math Made Nice-n-Easy Books #7: Trigonometric Identities & Equations, Straight Lines, Conic Sections*. Piscataway, N.J.: Research & Education Association. ISBN 0878912061.

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All links retrieved November 22, 2017.

- Rectifiable curve. – SpringerLink. This text originally appeared in
*Encyclopaedia of Mathematics*. ISBN 1402006098.

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