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− | A non-empty connected open set in a topological space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337601.png" />. The closure <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337602.png" /> of a domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337603.png" /> is called a closed domain; the closed set <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337604.png" /> is called the boundary of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337605.png" />. The points <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337606.png" /> are also called the interior points of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337607.png" />; the points <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337608.png" /> are called the boundary points of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d0337609.png" />; the points of the complement <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376010.png" /> are called the exterior points of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376011.png" />.
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− | Any two points of a domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376012.png" /> in the real Euclidean space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376013.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376014.png" /> (or in the complex space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376015.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376016.png" />, or on a Riemann surface or in a Riemannian domain), can be joined by a path (or arc) lying completely in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376017.png" />; if <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376018.png" /> or <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376019.png" />, they can even be joined by a polygonal path with a finite number of edges. Finite and infinite open intervals are the only domains in the real line <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376020.png" />; their boundaries consist of at most two points. A domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376021.png" /> in the plane is called simply connected if any closed path in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376022.png" /> can be continuously deformed to a point, remaining throughout in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376023.png" />. In general, the boundary of a simply-connected domain in the (open) plane <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376024.png" /> or <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376025.png" /> can consist of any number <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376026.png" /> of connected components, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376027.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376028.png" /> is regarded as a domain in the compact extended plane <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376029.png" /> or <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376030.png" /> and the number <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376031.png" /> of boundary components is finite, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376032.png" /> is called the connectivity order of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376033.png" />; for <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376034.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376035.png" /> is called multiply connected. In other words, the connectivity order <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376036.png" /> is one more than the minimum number of cross-cuts joining components of the boundary in pairs that are necessary to make <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376037.png" /> simply connected. For <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376038.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376039.png" /> is called doubly connected, for <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376040.png" />, triply connected, etc.; for <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376041.png" /> one has finitely-connected domains and for <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376042.png" /> infinitely-connected domains. The connectivity order of a plane domain characterizes its topological type. The topological types of domains in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376043.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376044.png" />, or in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376045.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376046.png" />, cannot be characterized by a single number.
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− | Even for a simply-connected plane domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376047.png" /> the metric structure of the boundary <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376048.png" /> can be very complicated (see [[Limit elements|Limit elements]]). In particular, the boundary points can be divided into accessible points <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376049.png" />, for which there exists a path <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376050.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376051.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376052.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376053.png" />, joining <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376054.png" /> in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376055.png" /> with any point <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376056.png" />, and inaccessible points, for which no such paths exists (cf. [[Attainable boundary point|Attainable boundary point]]). For any simply-connected plane domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376057.png" /> the set of accessible points of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376058.png" /> is everywhere dense in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376059.png" />.
| + | A non-empty connected open set in a topological space $ X $. |
| + | The closure $ \overline{D}\; $ |
| + | of a domain $ D $ |
| + | is called a closed domain; the closed set $ \textrm{ Fr } D = \overline{D}\; \setminus D $ |
| + | is called the boundary of $ D $. |
| + | The points $ x \in D $ |
| + | are also called the interior points of $ D $; |
| + | the points $ x \in \textrm{ Fr } D $ |
| + | are called the boundary points of $ D $; |
| + | the points of the complement $ C \overline{D}\; = X \setminus \overline{D}\; $ |
| + | are called the exterior points of $ D $. |
| | | |
− | A domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376060.png" /> in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376061.png" /> or <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376062.png" /> is called bounded, or finite, if
| + | Any two points of a domain $ D $ |
| + | in the real Euclidean space $ \mathbf R ^ {n} $, |
| + | $ n \geq 1 $( |
| + | or in the complex space $ \mathbf C ^ {m} $, |
| + | $ m \geq 1 $, |
| + | or on a Riemann surface or in a Riemannian domain), can be joined by a path (or arc) lying completely in $ D $; |
| + | if $ D \subset \mathbf R ^ {n} $ |
| + | or $ D \subset \mathbf C ^ {m} $, |
| + | they can even be joined by a polygonal path with a finite number of edges. Finite and infinite open intervals are the only domains in the real line $ \mathbf R = \mathbf R ^ {1} $; |
| + | their boundaries consist of at most two points. A domain $ D $ |
| + | in the plane is called simply connected if any closed path in $ D $ |
| + | can be continuously deformed to a point, remaining throughout in $ D $. |
| + | In general, the boundary of a simply-connected domain in the (open) plane $ \mathbf R ^ {2} $ |
| + | or $ \mathbf C = \mathbf C ^ {1} $ |
| + | can consist of any number $ k $ |
| + | of connected components, $ 0 \leq k \leq \infty $. |
| + | If $ D $ |
| + | is regarded as a domain in the compact extended plane $ \overline{\mathbf R}\; {} ^ {2} $ |
| + | or $ \overline{\mathbf C}\; $ |
| + | and the number $ k $ |
| + | of boundary components is finite, then $ k $ |
| + | is called the connectivity order of $ D $; |
| + | for $ k > 1 $, |
| + | $ D $ |
| + | is called multiply connected. In other words, the connectivity order $ k $ |
| + | is one more than the minimum number of cross-cuts joining components of the boundary in pairs that are necessary to make $ D $ |
| + | simply connected. For $ k = 2 $, |
| + | $ D $ |
| + | is called doubly connected, for $ k = 3 $, |
| + | triply connected, etc.; for $ k < \infty $ |
| + | one has finitely-connected domains and for $ k = \infty $ |
| + | infinitely-connected domains. The connectivity order of a plane domain characterizes its topological type. The topological types of domains in $ \mathbf R ^ {n} $, |
| + | $ n \geq 3 $, |
| + | or in $ \mathbf C ^ {m} $, |
| + | $ m \geq 2 $, |
| + | cannot be characterized by a single number. |
| | | |
− | <table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376063.png" /></td> </tr></table>
| + | Even for a simply-connected plane domain $ D $ |
| + | the metric structure of the boundary $ \textrm{ Fr } D $ |
| + | can be very complicated (see [[Limit elements|Limit elements]]). In particular, the boundary points can be divided into accessible points $ x _ {0} \in \textrm{ Fr } D $, |
| + | for which there exists a path $ x ( t) $, |
| + | $ 0 \leq t \leq 1 $, |
| + | $ x ( 0) \in D $, |
| + | $ x ( 1) = x _ {0} $, |
| + | joining $ x _ {0} $ |
| + | in $ D $ |
| + | with any point $ x ( 0) \in D $, |
| + | and inaccessible points, for which no such paths exists (cf. [[Attainable boundary point|Attainable boundary point]]). For any simply-connected plane domain $ D $ |
| + | the set of accessible points of $ \textrm{ Fr } D $ |
| + | is everywhere dense in $ \textrm{ Fr } D $. |
| | | |
− | if not, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376064.png" /> is called unbounded or infinite. A closed plane Jordan curve divides the plane <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376065.png" /> or <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376066.png" /> into two Jordan domains: A finite domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376067.png" /> and an infinite domain <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376068.png" />. All boundary points of a Jordan domain are accessible.
| + | A domain $ D $ |
| + | in $ \mathbf R ^ {n} $ |
| + | or $ \mathbf C ^ {m} $ |
| + | is called bounded, or finite, if |
| | | |
| + | $$ |
| + | \sup \ |
| + | \{ {| x | } : { |
| + | x \in D } \} |
| + | < \infty ; |
| + | $$ |
| | | |
| + | if not, $ D $ |
| + | is called unbounded or infinite. A closed plane Jordan curve divides the plane $ \mathbf R ^ {2} $ |
| + | or $ \mathbf C $ |
| + | into two Jordan domains: A finite domain $ D ^ {+} $ |
| + | and an infinite domain $ D ^ {-} $. |
| + | All boundary points of a Jordan domain are accessible. |
| | | |
| ====Comments==== | | ====Comments==== |
− | Instead of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376069.png" />, the boundary of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376070.png" /> is also denoted by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376071.png" /> or <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/d/d033/d033760/d03376072.png" />. | + | Instead of $ \textrm{ Fr } D $, |
| + | the boundary of $ D $ |
| + | is also denoted by $ \textrm{ b } D $ |
| + | or $ \partial D $. |
| | | |
| From the definition it can be seen that a domain is bounded if (and only if) it is contained in a ball centred at the coordinate origin and of finite radius. | | From the definition it can be seen that a domain is bounded if (and only if) it is contained in a ball centred at the coordinate origin and of finite radius. |
A non-empty connected open set in a topological space $ X $.
The closure $ \overline{D}\; $
of a domain $ D $
is called a closed domain; the closed set $ \textrm{ Fr } D = \overline{D}\; \setminus D $
is called the boundary of $ D $.
The points $ x \in D $
are also called the interior points of $ D $;
the points $ x \in \textrm{ Fr } D $
are called the boundary points of $ D $;
the points of the complement $ C \overline{D}\; = X \setminus \overline{D}\; $
are called the exterior points of $ D $.
Any two points of a domain $ D $
in the real Euclidean space $ \mathbf R ^ {n} $,
$ n \geq 1 $(
or in the complex space $ \mathbf C ^ {m} $,
$ m \geq 1 $,
or on a Riemann surface or in a Riemannian domain), can be joined by a path (or arc) lying completely in $ D $;
if $ D \subset \mathbf R ^ {n} $
or $ D \subset \mathbf C ^ {m} $,
they can even be joined by a polygonal path with a finite number of edges. Finite and infinite open intervals are the only domains in the real line $ \mathbf R = \mathbf R ^ {1} $;
their boundaries consist of at most two points. A domain $ D $
in the plane is called simply connected if any closed path in $ D $
can be continuously deformed to a point, remaining throughout in $ D $.
In general, the boundary of a simply-connected domain in the (open) plane $ \mathbf R ^ {2} $
or $ \mathbf C = \mathbf C ^ {1} $
can consist of any number $ k $
of connected components, $ 0 \leq k \leq \infty $.
If $ D $
is regarded as a domain in the compact extended plane $ \overline{\mathbf R}\; {} ^ {2} $
or $ \overline{\mathbf C}\; $
and the number $ k $
of boundary components is finite, then $ k $
is called the connectivity order of $ D $;
for $ k > 1 $,
$ D $
is called multiply connected. In other words, the connectivity order $ k $
is one more than the minimum number of cross-cuts joining components of the boundary in pairs that are necessary to make $ D $
simply connected. For $ k = 2 $,
$ D $
is called doubly connected, for $ k = 3 $,
triply connected, etc.; for $ k < \infty $
one has finitely-connected domains and for $ k = \infty $
infinitely-connected domains. The connectivity order of a plane domain characterizes its topological type. The topological types of domains in $ \mathbf R ^ {n} $,
$ n \geq 3 $,
or in $ \mathbf C ^ {m} $,
$ m \geq 2 $,
cannot be characterized by a single number.
Even for a simply-connected plane domain $ D $
the metric structure of the boundary $ \textrm{ Fr } D $
can be very complicated (see Limit elements). In particular, the boundary points can be divided into accessible points $ x _ {0} \in \textrm{ Fr } D $,
for which there exists a path $ x ( t) $,
$ 0 \leq t \leq 1 $,
$ x ( 0) \in D $,
$ x ( 1) = x _ {0} $,
joining $ x _ {0} $
in $ D $
with any point $ x ( 0) \in D $,
and inaccessible points, for which no such paths exists (cf. Attainable boundary point). For any simply-connected plane domain $ D $
the set of accessible points of $ \textrm{ Fr } D $
is everywhere dense in $ \textrm{ Fr } D $.
A domain $ D $
in $ \mathbf R ^ {n} $
or $ \mathbf C ^ {m} $
is called bounded, or finite, if
$$
\sup \
\{ {| x | } : {
x \in D } \}
< \infty ;
$$
if not, $ D $
is called unbounded or infinite. A closed plane Jordan curve divides the plane $ \mathbf R ^ {2} $
or $ \mathbf C $
into two Jordan domains: A finite domain $ D ^ {+} $
and an infinite domain $ D ^ {-} $.
All boundary points of a Jordan domain are accessible.
Instead of $ \textrm{ Fr } D $,
the boundary of $ D $
is also denoted by $ \textrm{ b } D $
or $ \partial D $.
From the definition it can be seen that a domain is bounded if (and only if) it is contained in a ball centred at the coordinate origin and of finite radius.