Skabelon:Intmath/doc

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This template generates integral symbols using unicode, for inline {{math}} formulae as an alternative to LaTeX generated in <math>.

Parametre

The template has three parameters, applicable one by one:

Integral sign: Choose one of:
- int for ∫ symbol is U+222B
- iint for ∬ (double integral, U+222C),
- iiint for ∭ (triple integral, U+222D),
- oint for ∮ (contour integral, U+222E),
- varointclockwise for ∲ (clockwise contour integral, U+2232)
- ointctrclockwise for ∳ (anticlockwise contour integral, U+2233),
- oiint for ∯ (closed surface integral, U+222F),
- oiiint for ∰ (closed volume integral, U+2230).
These match the LaTeX definitions exactly: please do not modify them for something more "convenient", thank you.
Subscript: Enter the subscript (symbol or short expression), for the lower limit or denoting an n-dimensional space or the (n − 1)- dimensional boundary.
Superscript: Enter the superscript (symbol or short expression) for the upper limit.

NB:

Applying italics to the integral symbol has no effect in Firefox, it remains upright.
This template already includes {{su}}.

Eksempler

No {{math}}

Gamma function

Γ(z) = ∫∞0 e^−tt^{z − 1}dt

Γ(''z'') = {{intmath|int|0|∞}} ''e''−''t''''t''''z'' − 1''dt''

Line integral

∲_C F(x) ∙ dx = −∳_C F(x) ∙ dx

{{intmath|varointclockwise|''C''}} ''F''('''x''') ∙ ''d'''''x''' = −{{intmath|ointctrclockwise|''C''}} ''F''('''x''') ∙ ''d'''''x'''

Maxwell's equations

∯_∂V E ∙ dS = 1/ε₀∭_V ρ dV

∯_∂V B ∙ dS = 0

∮_∂S E ∙ dx = −∬_S ∂B/∂t ∙ dS

∮_∂S B ∙ dx = ∬_S (μ₀J + 1/c²∂E/∂t) ∙ dS

{{intmath|oiint|∂''V''}} '''E''' ∙ ''d'''''S''' = {{sfrac|1|''ε''<sub>0</sub>}}{{intmath|iiint|''V''}} ''ρ'' ''dV''

{{intmath|oiint|∂''V''}} '''B''' ∙ ''d'''''S''' = 0

{{intmath|oint|∂''S''}} '''E''' ∙ ''d'''''x''' = −{{intmath|iint|''S''}} {{sfrac|∂'''B'''|∂''t''}} ∙ ''d'''''S'''

{{intmath|oint|∂''S''}} '''B''' ∙ ''d'''''x''' = {{intmath|iint|''S''}} (''μ''<sub>0</sub>'''J''' + {{sfrac|1|''c''<sup>2</sup>}}{{sfrac|∂'''E'''|∂''t''}}) ∙ ''d'''''S'''

Gamma function

Γ(z) = \int \infty 0 e - t t z - 1 dt

{{math|Γ(''z'') {{=}} {{intmath|int|0|∞}} ''e''−''t''''t''''z'' − 1''dt''}}

Line integral

∲_C

F (x) ∙ d x = - ∳ C F (x) ∙ d x

{{math|{{intmath|varointclockwise|''C''}} ''F''('''x''') ∙ ''d'''''x''' {{=}} −{{intmath|ointctrclockwise|''C''}} ''F''('''x''') ∙ ''d'''''x'''}}

Maxwell's equations

∯ \partial V E ∙ d S = 1 / ε 0 ∭ V ρ dV

∯ \partial V B ∙ d S = 0

\oint \partial S E ∙ d x = - \iint S \partial B / \partial t ∙ d S

\oint \partial S B ∙ d x = \iint S (μ 0 J + 1 / c 2 \partial E / \partial t) ∙ d S

{{math|{{intmath|oiint|∂''V''}} '''E''' ∙ ''d'''''S''' {{=}} {{sfrac|1|''ε''<sub>0</sub>}}{{intmath|iiint|''V''}} ''ρ'' ''dV''}}

{{math|{{intmath|oiint|∂''V''}} '''B''' ∙ ''d'''''S''' {{=}} 0}}

{{math|{{intmath|oint|∂''S''}} '''E''' ∙ ''d'''''x''' {{=}} −{{intmath|iint|''S''}} {{sfrac|∂'''B'''|∂''t''}} ∙ ''d'''''S'''}}

{{math|{{intmath|oint|∂''S''}} '''B''' ∙ ''d'''''x''' {{=}} {{intmath|iint|''S''}} (''μ''<sub>0</sub>'''J''' + {{sfrac|1|''c''<sup>2</sup>}}{{sfrac|∂'''E'''|∂''t''}}) ∙ ''d'''''S'''}}

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