English

Deutsch

Español

Français

Hrvatski

Italiano

Polski

Türkçe

Русский

中文

日本語

한국어

powered by CADENAS

Go to Article

Licensed under Creative Commons Attribution-Share Alike 3.0 (Sun Ladder).

For other uses, see Cylinder (disambiguation).

A **cylinder** (from Greek κύλινδρος – *kulindros*, "roller, tumbler"^{[1]}), has traditionally been a three-dimensional solid, one of the most basic of curvilinear geometric shapes. It is the idealized version of a solid physical tin can having lids on top and bottom.

This traditional view is still used in elementary treatments of geometry, but the advanced mathematical viewpoint has shifted to the infinite curvilinear surface and this is how a cylinder is now defined in various modern branches of geometry and topology.

The shift in the basic meaning (solid versus surface) has created some ambiguity with terminology. It is generally hoped that context makes the meaning clear. In this article both points of view are presented and distinguished by referring to *solid cylinders* and *cylindrical surfaces*, but keep in mind that in the literature the unadorned term cylinder could refer to either of these or to an even more specialized object, the *right circular cylinder*.

The definitions and results in this section are taken from the 1913 text, *Plane and Solid Geometry* by George Wentworth and David Eugene Smith (Wentworth & Smith 1913).

A *cylindrical surface* is a surface consisting of all the points on all the lines which are parallel to a given line and which pass through a fixed plane curve in a plane not parallel to the given line. Any line in this family of parallel lines is called an *element* of the cylindrical surface. From a kinematics point of view, given a plane curve, called the *directrix*, a cylindrical surface is that surface traced out by a line, called the *generatrix*, not in the plane of the directrix, moving parallel to itself and always passing through the directrix. Any particular position of the generatrix is an element of the cylindrical surface.

A solid bounded by a cylindrical surface and two parallel planes is called a (solid) *cylinder*. The line segments determined by an element of the cylindrical surface between the two parallel planes is called an *element of the cylinder*. All the elements of a cylinder have equal lengths. The region bounded by the cylindrical surface in either of the parallel planes is called a *base* of the cylinder. The two bases of a cylinder are congruent figures. If the elements of the cylinder are perpendicular to the planes containing the bases, the cylinder is a *right cylinder*, otherwise it is called an *oblique cylinder*. If the bases are disks (regions whose boundary is a circle) the cylinder is called a *circular cylinder*. In some elementary treatments, a cylinder always means a circular cylinder.^{[2]}

The *height* (or altitude) of a cylinder is the perpendicular distance between its bases.

The cylinder obtained by rotating a line segment about a fixed line that it is parallel to is a *cylinder of revolution*. A cylinder of revolution is a right circular cylinder. The height of a cylinder of revolution is the length of the generating line segment. The line that the segment is revolved about is called the *axis* of the cylinder and it passes through the centers of the two bases.

The unmodified term *cylinder* often refers to a solid cylinder with circular ends perpendicular to the axis, that is, a right circular cylinder, as shown in the figure. If the ends are missing, it is called an *open cylinder*. The formulae for the surface area and the volume of a right circular cylinder have been known from early antiquity.

A right circular cylinder can also be thought of as the solid of revolution generated by rotating a rectangle about one of its sides. These cylinders are used in an integration technique (the "disk method") for obtaining volumes of solids of revolution.^{[3]}

Cylindric sections are the intersections of cylinders with planes. They are, in general, curves and are special types of *plane sections*. The cylindric section of a plane that contains two elements of a cylinder is a parallelogram.^{[4]} Such a cylindric section of a right cylinder is a rectangle.^{[4]}

A cylindric section in which the intersecting plane intersects and is perpendicular to all the elements of the cylinder is called a *right section*.^{[5]} If a right section of a cylinder is a circle then the cylinder is a circular cylinder. In more generality, if a right section of a cylinder is a conic section (parabola, ellipse, hyperbola) then the solid cylinder is said to be parabolic, elliptic or hyperbolic respectively.

For a right circular cylinder, there are four possibilities for planes that meet a cylinder. A plane is tangent to the cylinder if it meets the cylinder in a single element. A plane containing two elements has a rectangle as a cylindric section. The right sections are circles and all other planes intersect the cylinder in an ellipse.^{[6]}

In the case of a right circular cylinder with a cylindric section that is an ellipse, the eccentricity *e* of the cylindric section and semi-major axis *a* of the cylindric section depend on the radius of the cylinder *r* and the angle *α* between the secant plane and cylinder axis, in the following way:

- $e=\cos \alpha ,$

- $a={\frac {r}{\sin \alpha }}.$

If the base of a circular cylinder has a radius *r* and the cylinder has height h, then its volume is given by

*V*= π*r*^{2}*h*.

This formula holds whether or not the cylinder is a right cylinder.^{[7]}

This formula may be established by using Cavalieri's principle.

In more generality, by the same principle, the volume of any cylinder is the product of the area of a base and the height. For example, an elliptic cylinder with a base having semi-major axis a, semi-minor axis b and height h has a volume *V* = *Ah*, where A is the area of the base ellipse (= π*ab*). This result for right elliptic cylinders can also be obtained by integration, where the axis of the cylinder is taken as the positive x-axis and *A*(*x*) = *A* the area of each elliptic cross-section, thus:

- $V=\int _{0}^{h}A(x)dx=\int _{0}^{h}\pi abdx=\pi ab\int _{0}^{h}dx=\pi abh.$

Using cylindrical coordinates, the volume of a right circular cylinder can be calculated by integration over

- $=\int _{0}^{h}\int _{0}^{2\pi }\int _{0}^{r}s\,\,ds\,d\phi \,dz$
- $=\pi \,r^{2}\,h.$

Having radius *r* and altitude (height) h, the surface area of a right circular cylinder, oriented so that its axis is vertical, consists of three parts:

- the area of the top base: π
*r*^{2} - the area of the bottom base: π
*r*^{2} - the area of the side: 2π
*rh*

The area of the top and bottom bases is the same, and is called the *base area*, *B*. The area of the side is known as the *lateral area*, *L*.

An *open cylinder* does not include either top or bottom elements, and therefore has surface area (lateral area)

*L*= 2π*rh*.

The surface area of the solid right circular cylinder is made up the sum of all three components: top, bottom and side. Its surface area is therefore,

*A*=*L*+2*B*= 2π*rh*+ 2π*r*^{2}= 2π*r*(*h*+*r*) = π*d*(*r*+*h*),

where *d* = 2*r* is the diameter of the circular top or bottom.

For a given volume, the right circular cylinder with the smallest surface area has *h* = 2*r*. Equivalently, for a given surface area, the right circular cylinder with the largest volume has *h* = 2*r*, that is, the cylinder fits snugly in a cube of side length = altitude ( = diameter of base circle).^{[8]}

The lateral area, L, of a circular cylinder, which need not be a right cylinder, is more generally given by:

*L*=*e*×*p*,

where e is the length of an element and p is the perimeter of a right section of the cylinder.^{[9]} This produces the previous formula for lateral area when the cylinder is a right circular cylinder.

A *right circular hollow cylinder* (or *cylindrical shell*) is a three-dimensional region bounded by two right circular cylinders having the same axis and two parallel annular bases perpendicular to the cylinders' common axis, as in the diagram.

Let the height be *h*, internal radius *r*, and external radius *R*. The volume is given by

- $V=\pi (R^{2}-r^{2})h=2\pi \left({\frac {R+r}{2}}\right)h(R-r).$.

Thus, the volume of a cylindrical shell equals 2π(average radius)(altitude)(thickness).^{[10]}

The surface area, including the top and bottom, is given by

- $A=2\pi (R+r)h+2\pi (R^{2}-r^{2}).$.

Cylindrical shells are used in a common integration technique for finding volumes of solids of revolution.^{[11]}

Main article: On the Sphere and Cylinder

In the treatise by this name, written c. 225 BCE, Archimedes obtained the result of which he was most proud, namely obtaining the formulas for the volume and surface area of a sphere by exploiting the relationship between a sphere and its circumscribed right circular cylinder of the same height and diameter. The sphere has a volume two-thirds that of the circumscribed cylinder and a surface area two-thirds that of the cylinder (including the bases). Since the values for the cylinder were already known, he obtained, for the first time, the corresponding values for the sphere. The volume of a sphere of radius r is 4/3π*r*^{3} = 2/3 (2π*r*^{3}). The surface area of this sphere is 4π*r*^{2} = 2/3 (6π*r*^{2}). A sculpted sphere and cylinder were placed on the tomb of Archimedes at his request.

In some areas of geometry and topology the term *cylinder* refers to what we have called a cylindrical surface. To repeat, throughout this section a cylinder is defined as a surface consisting of all the points on all the lines which are parallel to a given line and which pass through a fixed plane curve in a plane not parallel to the given line.^{[12]} Such cylinders have, at times, been referred to as *generalized cylinders*. Through each point of a generalized cylinder there passes a unique line that is contained in the cylinder.^{[13]} Thus, this definition may be rephrased to say that a cylinder is any ruled surface spanned by a one-parameter family of parallel lines.

A cylinder having a right section that is an ellipse, parabola, or hyperbola is called an **elliptic cylinder**, **parabolic cylinder**, or **hyperbolic cylinder** respectively. These are degenerate quadric surfaces.^{[14]}

The general equation of a quadric in three dimensions is given by

- $f(x,y,z)=Ax^{2}+By^{2}+Cz^{2}+Dx+Ey+Gz+H=0,$

with the coefficients being real numbers and not all of A, B and C being 0. If at least one variable does not appear in the equation, then the quadric is degenerate. If one variable is missing, we may assume by an appropriate rotation of axes that the variable z does not appear and the general equation of this type of degenerate quadric can be written as^{[15]}

- $A\left(x+{\frac {D}{2A}}\right)^{2}+B\left(y+{\frac {E}{2B}}\right)^{2}=\rho ,$

where

- $\rho =-H+{\frac {D^{2}}{4A}}+{\frac {E^{2}}{4B}}.$

If *AB* > 0 this is the equation of an *elliptic cylinder*.^{[15]} Further simplification can be obtained by translation of axes and scalar multiplication. If $\rho$ has the same sign as the coefficients A and B, then the elliptic cylinder has the following equation in Cartesian coordinates:

- $\left({\frac {x}{a}}\right)^{2}+\left({\frac {y}{b}}\right)^{2}=1.$

This equation of an elliptic cylinder is a generalization of the equation of the ordinary, **circular cylinder** (*a* = *b*). Elliptic cylinders are also known as **cylindroids**, but that name is ambiguous, as it can also refer to the Plücker conoid.

If $\rho$ has a different sign than the coefficients, we obtain the *imaginary elliptic cylinders*:

- $\left({\frac {x}{a}}\right)^{2}+\left({\frac {y}{b}}\right)^{2}=-1,$

which have no real points on them. ($\rho =0$ gives a single real point.)

If A and B have different signs and $\rho \neq 0$, we obtain the *hyperbolic cylinders*, whose equations may be written as:

- $\left({\frac {x}{a}}\right)^{2}-\left({\frac {y}{b}}\right)^{2}=1.$

Finally, if *AB* = 0 we may assume that *B* = 0 and *A* = 1 to obtain the *parabolic cylinders* with equations that can be written as:^{[16]}

- ${x}^{2}+2a{y}=0.$

In projective geometry, a cylinder is simply a cone whose apex (vertex) lies on the plane at infinity. If the cone is a quadratic cone, the plane at infinity passing through the vertex can intersect the cone at two real lines, a single real line (actually a coincident pair of lines), or only at the vertex. These cases give rise to the hyperbolic, parabolic or elliptic cylinders respectively.^{[17]}

This concept is useful when considering degenerate conics, which may include the cylindrical conics.

A *circular cylinder* can be seen as a limiting case of a n-gonal prism where *n* approaches infinity. It can also be seen as a dual of a bicone as an infinite-sided bipyramid.

Polyhedron | ||||||||||
---|---|---|---|---|---|---|---|---|---|---|

Coxeter | ||||||||||

Tiling | ||||||||||

Config. | 3.4.4 | 4.4.4 | 5.4.4 | 6.4.4 | 7.4.4 | 8.4.4 | 9.4.4 | 10.4.4 | 11.4.4 | 12.4.4 |

- Steinmetz solid, the intersection of two or three perpendicular cylinders

AnchorBottleConeSpherical trigonometryPentakis dodecahedronCarbon nanotubeNanostructureSwivelCrankcase

This article uses material from the Wikipedia article "Cylinder", which is released under the Creative Commons Attribution-Share-Alike License 3.0. There is a list of all authors in Wikipedia

3d,cad,model,library,download,drawing,step,cad blocks,basics,university,highschool,college,grammer school,statistics,3dprinted

Share