Asosiy tarkibga o'tish

15.6-bo'lim : Silindrsimon koordinatalarda uch karrali integrallar

4. \(x \le 0\) bilan \({x^2} + {y^2} = 3\) silindr ichidagi \(z = 6 - x\) ostida, \(z = - \sqrt {4{x^2} + 4{y^2}} \) ustidagi mintaqa hajmini aniqlash uchun uch karrali integraldan foydalaning.

Yechim

Mayli, keling, \(E\) hududining qisqacha chizmasidan boshlaylik, shunda biz nima bilan shug'ullanayotganimizni his qilishimiz mumkin.

Mana, \(E\) eskizi.

A three dimensional sketch of the region \(E\) drawn with the traditional axes.  It is the half of the cylinder \({x^2} + {y^2} = 3\) with \(x \le 0\), standing upright, with the orange slanted plane \(z = 6 - x\) capping it on top and the cone \(z = - \sqrt {4{x^2} + 4{y^2}} \) forming a downward pointing cap at the bottom.
A three dimensional sketch of the same region \(E\), this time drawn with a set of “box” axes to make the surface and region easier to visualize.  The orange plane \(z = 6 - x\) caps the top of the half cylinder and the cone forms the pointed cap at the bottom.

Biz "an'anaviy" o'qlar to'plami bilan bir qatorda "quti" o'qlari to'plami bilan eskizlarni berdik, bu sirt va mintaqani tasavvur qilishda yordam beradi.

\(z = 6 - x\) samolyoti silindrdagi yuqori "qopqoq" va \(z = - \sqrt {4{x^2} + 4{y^2}} \) konus silindrdagi pastki "qopqoq" hisoblanadi. Muammo bayonotining \(x \le 0\) qismi tufayli bizda silindrning faqat yarmi bor.

2-qadam

Bu qattiq jismning hajmi quyidagicha ifodalanadi:

\[V = \iiint\limits_{E}{{dV}}\]
3-qadam

Shunday qilib, eskizdan umid qilamanki, \(D\) mintaqasi \(xy\) tekisligida bo'ladi va shuning uchun biz avval \(z\) bilan integratsiya qilishimiz kerak. Bu shuni anglatadiki, \(z\) chegaralari,

\[ - \sqrt {4{x^2} + 4{y^2}} \le z \le 6 - x\]
4-qadam

Ushbu muammo uchun \(D\) shunchaki \({x^2} + {y^2} \le \sqrt 3 \) diskining \(x \le 0\) bilan bir qismidir. Mana, chegaralar bilan yordam berish uchun \(D\) ning qisqacha eskizi.

A sketch of the region \(D\).  It is the half of the disk of radius \(\sqrt 3 \) centered at the origin with \(x \le 0\), so its flat edge lies along the y-axis and the semicircular arc bulges away from it.  The inside is shaded orange.

\(D\) aniq diskning bir qismi bo'lgani uchun biz silindrsimon koordinatalardan foydalanamiz. Shunday qilib, bu muammoning silindrsimon koordinatalari.

\[\begin{array}{c}\displaystyle \frac{\pi }{2} \le \theta \le \frac{{3\pi }}{2}\\ 0 \le r \le \sqrt 3 \\ - 2r \le z \le 6 - r\cos \theta \end{array}\]

\(z\) chegaralarini silindrsimon koordinatalarga aylantirishni unutmang.

5-qadam

ushbu limitlarni integralga kiritish va silindrsimon koordinatalarga aylantirish,

\[V = \iiint\limits_{E}{{\,dV}} = \int_{{\frac{\pi }{2}}}^{{\frac{{3\pi }}{2}}}{{\int_{0}^{{\sqrt 3 }}{{\int_{{ - 2r}}^{{6 - r\cos \theta }}{{r\,dz}}\,dr}}\,d\theta }}\]

Shuni unutmangki, \(dV = r\,dx\,dr\,d\theta \) va shuning uchun biz \(dV\) ni silindrsimon koordinatalarga o'tkazishda \(r\)ni olamiz.

6-qadam

OK, endi biz qilishimiz kerak bo'lgan narsa - bu integralni baholash. Mana \(z\) integratsiyasi.

\[\begin{align*}V & = \int_{{\frac{\pi }{2}}}^{{\frac{{3\pi }}{2}}}{{\int_{0}^{{\sqrt 3 }}{{\left. {\left( {rz} \right)} \right|_{ - 2r}^{6 - r\cos \theta }\,dr}}\,d\theta }}\\ & = \int_{{\frac{\pi }{2}}}^{{\frac{{3\pi }}{2}}}{{\int_{0}^{{\sqrt 3 }}{{6r - {r^2}\cos \theta + 2{r^2}\,dr}}\,d\theta }}\end{align*}\]
7-qadam

Keling, \(r\) integratsiyasini amalga oshiramiz.

\[\begin{align*}V & = \int_{{\frac{\pi }{2}}}^{{\frac{{3\pi }}{2}}}{{\left. {\left( {3{r^2} - \frac{1}{3}{r^3}\cos \theta + \frac{2}{3}{r^3}} \right)} \right|_0^{\sqrt 3 }\,d\theta }}\\ & = \int_{{\frac{\pi }{2}}}^{{\frac{{3\pi }}{2}}}{{9 - \sqrt 3 \cos \theta + 2\sqrt 3 \,d\theta }}\end{align*}\]
8-qadam

Nihoyat, biz \(\theta \) integratsiyasini amalga oshiramiz.

\[V = \left. {\left( {9\theta + 2\sqrt 3 \theta - \sqrt 3 \sin \theta } \right)} \right|_{\frac{\pi }{2}}^{\frac{{3\pi }}{2}} = \require{bbox} \bbox[2pt,border:1px solid black]{{2\sqrt 3 + \left( {9 + 2\sqrt 3 } \right)\pi = 42.6212}}\]