# Surface area

The surface area of a solid object is a measure of the total area that the surface of an object occupies. The mathematical definition of surface area in the presence of curved surfaces is considerably more involved than the definition of arc length of one-dimensional curves, or of the surface area for polyhedra (i.e., objects with flat polygonal faces), for which the surface area is the sum of the areas of its faces. Smooth surfaces, such as a sphere, are assigned surface area using their representation as parametric surfaces. This definition of surface area is based on methods of infinitesimal calculus and involves partial derivatives and double integration.

A general definition of surface area was sought by Henri Lebesgue and Hermann Minkowski at the turn of the twentieth century. Their work led to the development of geometric measure theory, which studies various notions of surface area for irregular objects of any dimension. An important example is the Minkowski content of a surface.

## Definition

While the areas of many simple surfaces have been known since antiquity, a rigorous mathematical definition of area requires a great deal of care. This should provide a function

${\displaystyle S\mapsto A(S)}$

which assigns a positive real number to a certain class of surfaces that satisfies several natural requirements. The most fundamental property of the surface area is its additivity: the area of the whole is the sum of the areas of the parts. More rigorously, if a surface S is a union of finitely many pieces S1, …, Sr which do not overlap except at their boundaries, then

${\displaystyle A(S)=A(S_{1})+\cdots +A(S_{r}).}$

Surface areas of flat polygonal shapes must agree with their geometrically defined area. Since surface area is a geometric notion, areas of congruent surfaces must be the same and the area must depend only on the shape of the surface, but not on its position and orientation in space. This means that surface area is invariant under the group of Euclidean motions. These properties uniquely characterize surface area for a wide class of geometric surfaces called piecewise smooth. Such surfaces consist of finitely many pieces that can be represented in the parametric form

${\displaystyle S_{D}:{\vec {r}}={\vec {r}}(u,v),\quad (u,v)\in D}$

with a continuously differentiable function ${\displaystyle {\vec {r}}.}$ The area of an individual piece is defined by the formula

${\displaystyle A(S_{D})=\iint _{D}\left|{\vec {r}}_{u}\times {\vec {r}}_{v}\right|\,du\,dv.}$

Thus the area of SD is obtained by integrating the length of the normal vector ${\displaystyle {\vec {r}}_{u}\times {\vec {r}}_{v}}$ to the surface over the appropriate region D in the parametric uv plane. The area of the whole surface is then obtained by adding together the areas of the pieces, using additivity of surface area. The main formula can be specialized to different classes of surfaces, giving, in particular, formulas for areas of graphs z = f(x,y) and surfaces of revolution.

One of the subtleties of surface area, as compared to arc length of curves, is that surface area cannot be defined simply as the limit of areas of polyhedral shapes approximating a given smooth surface. It was demonstrated by Hermann Schwarz that already for the cylinder, different choices of approximating flat surfaces can lead to different limiting values of the area (Known as Schwarz's paradox.) [1] .[2]

Various approaches to a general definition of surface area were developed in the late nineteenth and the early twentieth century by Henri Lebesgue and Hermann Minkowski. While for piecewise smooth surfaces there is a unique natural notion of surface area, if a surface is very irregular, or rough, then it may not be possible to assign an area to it at all. A typical example is given by a surface with spikes spread throughout in a dense fashion. Many surfaces of this type occur in the study of fractals. Extensions of the notion of area which partially fulfill its function and may be defined even for very badly irregular surfaces are studied in geometric measure theory. A specific example of such an extension is the Minkowski content of the surface.

## Common formulas

Surface areas of common solids
Shape Equation Variables
Cube ${\displaystyle 6s^{2}\,}$ s = side length
Rectangular prism ${\displaystyle 2(\ell w+\ell h+wh)\,}$ = length, w = width, h = height
Triangular prism ${\displaystyle bh+l(a+b+c)}$ b = base length of triangle, h = height of triangle, l = distance between triangles, a, b, c = sides of triangle
All Prisms ${\displaystyle 2B+Ph\,}$ B = the area of one base, P = the perimeter of one base, h = height
Sphere ${\displaystyle 4\pi r^{2}=\pi d^{2}\,}$ r = radius of sphere, d = diameter
Spherical lune ${\displaystyle 2r^{2}\theta \,}$ r = radius of sphere, θ = dihedral angle
Torus ${\displaystyle (2\pi r)(2\pi R)=4\pi ^{2}Rr}$ r = minor radius, R = major radius
Closed cylinder ${\displaystyle 2\pi r^{2}+2\pi rh=2\pi r(r+h)\,}$ r = radius of the circular base, h = height of the cylinder
Lateral surface area of a cone ${\displaystyle \pi r\left({\sqrt {r^{2}+h^{2}}}\right)=\pi rs\,}$ ${\displaystyle s={\sqrt {r^{2}+h^{2}}}}$

s = slant height of the cone,
r = radius of the circular base,
h = height of the cone

Full surface area of a cone ${\displaystyle \pi r\left(r+{\sqrt {r^{2}+h^{2}}}\right)=\pi r(r+s)\,}$ s = slant height of the cone,

r = radius of the circular base,
h = height of the cone

Pyramid ${\displaystyle B+{\frac {PL}{2}}}$ B = area of base, P = perimeter of base, L = slant height
Square pyramid ${\displaystyle b^{2}+2bs}$ b = base length, s = slant height

### Ratio of surface areas of a sphere and cylinder of the same radius and height

A cone, sphere and cylinder of radius r and height h.

The below given formulas can be used to show that the surface area of a sphere and cylinder of the same radius and height are in the ratio 2 : 3, as follows.

Let the radius be r and the height be h (which is 2r for the sphere).

The discovery of this ratio is credited to Archimedes.[3]

## In chemistry

{{#invoke:see also|seealso}} Surface area is important in chemical kinetics. Increasing the surface area of a substance generally increases the rate of a chemical reaction. For example, iron in a fine powder will combust, while in solid blocks it is stable enough to use in structures. For different applications a minimal or maximal surface area may be desired.