WikiDer > Minkovski-Shtayner formulasi

Yilda matematika, Minkovskiy-Shtayner formulasi ga tegishli formuladir sirt maydoni va hajmi ning ixcham pastki to'plamlar ning Evklid fazosi. Aniqrog'i, u sirtni tegishli ma'noda yopiq hajmning "hosilasi" deb belgilaydi.

Minkovski-Shtayner formulasi, bilan birga ishlatiladi Brunn-Minkovskiy teoremasi, isbotlash uchun izoperimetrik tengsizlik. Uning nomi berilgan Hermann Minkovskiy va Yakob Shtayner.

Minkovski-Shtayner formulasining bayonoti

Ruxsat bering ${ displaystyle n geq 2}$va ruxsat bering ${ displaystyle A subsetneq mathbb {R} ^ {n}}$ ixcham to'plam bo'ling. Ruxsat bering ${ displaystyle mu (A)}$ ni belgilang Lebesg o'lchovi (hajmi) ning ${ displaystyle A}$. Miqdorini aniqlang ${ displaystyle lambda ( qisman A)}$ tomonidan Minkovski-Shtayner formulasi

${ displaystyle lambda ( qismli A): = liminf _ { delta dan 0} { frac { mu chap (A + { overline {B _ { delta}}} o'ng) - mu ( A)} { delta}},}$

qayerda

${ displaystyle { overline {B _ { delta}}}: = left {x = (x_ {1}, dots, x_ {n}) in mathbb {R} ^ {n} left | | x |: = { sqrt {x_ {1} ^ {2} + dots + x_ {n} ^ {2}}} leq delta right. right }}$

belgisini bildiradi yopiq to'p ning radius ${ displaystyle delta> 0}$va

${ displaystyle A + { overline {B _ { delta}}}: = left {a + b in mathbb {R} ^ {n} left | a in A, b in { overline { B _ { delta}}} o'ng. O'ng }}$

bo'ladi Minkovskiy summasi ning ${ displaystyle A}$ va ${ displaystyle { overline {B _ { delta}}}}$, Shuning uchun; ... uchun; ... natijasida

${ displaystyle A + { overline {B _ { delta}}} = left {x in mathbb {R} ^ {n} { mathrel {|}} { mathopen {|}} xa { mathclose {|}} leq delta { mbox {uchun}} a in A right }.}$

Izohlar

Yuzaki o'lchov

"Etarli darajada muntazam" to'plamlar uchun ${ displaystyle A}$, miqdori ${ displaystyle lambda ( qisman A)}$ bilan albatta mos keladi ${ displaystyle (n-1)}$-ning o'lchov o'lchovi chegara ${ displaystyle qisman A}$ ning ${ displaystyle A}$. Ushbu muammoni to'liq davolash uchun Federer (1969) ga murojaat qiling.

Qavariq silsilalar

To'plam qachon ${ displaystyle A}$ a qavariq o'rnatilgan, lim-inf yuqoridagi haqiqat chegarava buni ko'rsatish mumkin

${ displaystyle mu chap (A + { overline {B _ { delta}}} o'ng) = mu (A) + lambda ( qisman A) delta + sum _ {i = 2} ^ { n-1} lambda _ {i} (A) delta ^ {i} + omega _ {n} delta ^ {n},}$

qaerda ${ displaystyle lambda _ {i}}$ ba'zilari doimiy funktsiyalar ning ${ displaystyle A}$ (qarang quermassintegrallar) va ${ displaystyle omega _ {n}}$ ning o'lchovini (hajmini) bildiradi birlik to'pi yilda ${ displaystyle mathbb {R} ^ {n}}$:

${ displaystyle omega _ {n} = { frac {2 pi ^ {n / 2}} {n Gamma (n / 2)}},}$

qayerda ${ displaystyle Gamma}$ belgisini bildiradi Gamma funktsiyasi.

Misol: to'pning hajmi va yuzasi

Qabul qilish ${ displaystyle A = { overline {B_ {R}}}}$ ning sirt maydoni uchun quyidagi taniqli formulani beradi soha radiusning ${ displaystyle R}$, ${ displaystyle S_ {R}: = qisman B_ {R}}$:

${ displaystyle lambda (S_ {R}) = lim _ { delta dan 0} { frac { mu chapgacha ({ overline {B_ {R}}} + { overline {B _ { delta) }}} o'ng) - mu chap ({ overline {B_ {R}}} o'ng)} { delta}}}$

${ displaystyle = lim _ { delta to 0} { frac {[(R + delta) ^ {n} -R ^ {n}] omega _ {n}} { delta}}}$

${ displaystyle = nR ^ {n-1} omega _ {n},}$

qayerda ${ displaystyle omega _ {n}}$ yuqoridagi kabi.

Adabiyotlar

• Dakorogna, Bernard (2004). O'zgarishlar hisobiga kirish. London: Imperial kolleji matbuoti. ISBN 1-86094-508-2.
• Federer, Gerbert (1969). Geometrik o'lchov nazariyasi. Nyu York: Springer-Verlag.