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GOLDEN BRAIN
ISSN: 2181-4120
VOLUME 1 | ISSUE 14 | 2023
SILINDRIK VA SFERIK KOORDINATALAR
๐‘ง
SISTEMASI
๐‘ง๐ด
๐ด
Bozorova Oสปgสปiloy Hikmat qizi
๐‘‚
๐œ‘๐ด
๐‘Ÿ๐ด
Chirchiq davlat pedagogika universiteti
๐‘ƒ
ANNOTATSIYA
Qutb koordinatalari sistemasi tekislikdagi nuqtaning vaziyatini aniqlaydi. Fazodagi
nuqtaning vaziyatini aniqlash uchun silindrik
koordinatalar
sistemasini
Silindirsimon
koordiatalar
kiritamiz.
sistemasi
๐œ‹
uch
๐‘… ๐‘‚
oสปlchovli kosmosdagi nuqtalarni topish uchun
ishlatiladi. Sferik koordinatalar sistemasi —
oสปlchamli
koordinatalar
๐œ‹
๐›พ
sistemasi
fazodagi
uch
boสปlib,
nuqtaning
ะขัžา“ั€ะธ ั†ะธะปะธะฝะดั€
vaziyati uchta kattalik bilan bilan aniqlanadi.
๐œ‹ ั‚ะตะบะธัะปะธะบะดะฐะณะธ
๐›พ ัะณั€ะธ ั‡ะธะทะธา›
Silindrik
koordinatalar sistemasi
Avvalo silindr va silindrik
chiziq tushunchasini kiritamiz.
Ma’lumki,
tekislikning
ะฆะธะปะธะฝะดั€ะธะบ ัะธั€ั‚
berilgan nuqtasidan bir xil masofada
yotgan nuqtalari to‘plami aylana deyiladi. Berilgan nuqta aylananing markazi,
markazdan aylananing biror (yoki ixtiyoriy) nuqtasigacha bo‘lgan masofa aylananing
radiusi deyiladi. SHu tekislikni aylana nuqtalari orqali kesib o‘tuvchi parallel to‘g‘ri
https://t.me/goldenbrain_journal
Multidisciplinary Scientific Journal
May, 2023
217
GOLDEN BRAIN
ISSN: 2181-4120
VOLUME 1 | ISSUE 14 | 2023
chiziqlar to‘plami silindr deyiladi. Bunda har bir to‘g‘ri chiziq silindrning yasovchisi
deyiladi. Agar silindrning yasovchisi aylana tekisligiga perpendikulyar bo‘lsa, bu
silindr to‘g‘ri silindr deyiladi, aks holda og‘ma silindr deyiladi.
Tekislikdagi ixtiyoriy ๐›พ egri chiziqni qaraylik (๐›พ – “gamma” deb o‘qiladi, grek
harfi). SHu tekislikni ๐›พ egri chiziq nuqtalari orqali kesib o‘tuvchi parallel to‘g‘ri
chiziqlar to‘plami silindrik sirt deyiladi. Bunda har bir to‘g‘ri chiziq silindrik sirtning
yasovchisi deyiladi. Agar silindrik sirtning yasovchisi ๐›พ egri chiziq tekisligiga
perpendikulyar bo‘lsa, bu silindrik sirt to‘g‘ri silindrik silindrik deyiladi, aks holda
og‘ma silindrik sirt deyiladi.
Endi fazoda {๐‘‚, ๐‘Ÿ, ๐œ‘} qutb koordinatalar sistemasi kiritilgan tekislik va uni ๐‘‚
qutb orqali perpendikulyar kesib o‘tuvchi ๐‘‚๐‘ง o‘q berilgan bo‘lsin. Bunda ๐‘‚๐‘ง o‘q
shunday yo‘nalganki, yo‘nalishning “oxiri”dan kuzatganda qutb tekisligidagi musbat
burilish soat strelkasi harakatiga qarama-qarshi bo‘lsin. Hosil bo‘lgan {๐‘‚, ๐‘Ÿ, ๐œ‘, ๐‘ง}
sistema silindrik koordinatalar sistemasi deyiladi.
Fazodagi har bir nuqta silindrik koordinatalar sistemasida uchta ๐‘Ÿ , ๐œ‘ , ๐‘ง son
orqali bir qiymatli ifodalanadi, bu erda 0 ≤ ๐‘Ÿ < +∞, 0 ≤ ๐œ‘ < 2๐œ‹, −∞ < ๐‘ง < +∞.
Bu sonlar mazkur nuqtaning silindrik koordinatalari deyiladi.
Aytaylik, fazodagi biror ๐ด nuqtaning silindrik koordinatalari ๐‘Ÿ๐ด , ๐œ‘๐ด , ๐‘ง๐ด bo‘lsin.
Bu holat ๐ด(๐‘Ÿ๐ด , ๐œ‘๐ด , ๐‘ง๐ด ) kabi yoziladi. ๐‘Ÿ๐ด son ๐‘‚๐‘ง o‘qdan ๐ด nuqtagacha masofani
anglatadi va ๐ด nuqtaning radial masofasi deyiladi; ๐œ‘๐ด sonni ๐ด nuqtaning azimuti
deyishadi; ๐‘ง๐ด songa nibatan ๐ด nuqtaning balandligi iborasini ishlatishadi.
Fazodagi ๐ด nuqtaning (๐‘ฅ๐ด , ๐‘ฆ๐ด , ๐‘ง๐ด ) Dekart koordinatalaridan uning (๐‘Ÿ๐ด , ๐œ‘๐ด , ๐‘ง๐ด )
silindrik koordinatalariga
๐‘Ÿ๐ด = √๐‘ฅ๐ด2 + ๐‘ฆ๐ด2 ,
๐‘ฆ
๐œ‘๐ด = ๐‘Ž๐‘Ÿ๐‘๐‘ก๐‘” ๐‘ฅ๐ด ,
๐ด
๐‘ง๐ด = ๐‘ง๐ด
(3.1)
tengliklar orqali o‘tiladi.
Teskari
o‘tish,
ya’ni
fazodagi
๐ด
(๐‘Ÿ๐ด , ๐œ‘๐ด , ๐‘ง๐ด )
nuqtaning
silindrik
koordinatalaridan uning (๐‘ฅ๐ด , ๐‘ฆ๐ด , ๐‘ง๐ด ) Dekart koordinatalariga o‘tish
๐‘ฅ๐ด = ๐‘Ÿ๐ด cos ๐œ‘๐ด ,
๐‘ฆ๐ด = ๐‘Ÿ๐ด sin ๐œ‘๐ด ,
๐‘ง๐ด = ๐‘ง๐ด
(3.2)
tengliklar orqali amalga oshiriladi.
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Multidisciplinary Scientific Journal
May, 2023
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GOLDEN BRAIN
ISSN: 2181-4120
VOLUME 1 | ISSUE 14 | 2023
Silindrik koordinatalari bilan berilgan ikkita ๐ด(๐‘Ÿ๐ด , ๐œ‘๐ด , ๐‘ง๐ด ) va ๐ต(๐‘Ÿ๐ต , ๐œ‘๐ต , ๐‘ง๐ต )
nuqtalar orasidagi masofa
๐œŒ(๐ด, ๐ต) = ๐ด๐ต = √๐‘Ÿ๐ด2 + ๐‘Ÿ๐ต2 − 2๐‘Ÿ๐ด ๐‘Ÿ๐ต cos(๐œ‘๐ต − ๐œ‘๐ด ) + (๐‘ง๐ต − ๐‘ง๐ด )2
(3.3)
formula orqali hisoblanadi.
2. Sferik koordinatalar sistemasi
Fazoning berilgan nuqtasidan bir xil masofada yotgan nuqtalari to‘plami sfera
deyiladi. Berilgan nuqta sferaning markazi, markazdan sferaning biror (yoki ixtiyoriy)
nuqtasigacha bo‘lgan masofa sferaning radiusi deyiladi.
Fazoda {๐‘‚, ๐‘Ÿ, ๐œ‘} qutb koordinatalar sistemasi kiritilgan tekislik va uni ๐‘‚ qutb
orqali perpendikulyar kesib o‘tuvchi ๐‘‚๐‘ง o‘q berilgan bo‘lsin. Bunda ๐‘‚๐‘ง o‘q shunday
yo‘nalganki, yo‘nalishning “oxiri”dan kuzatganda qutb tekisligidagi musbat burilish
soat strelkasi harakatiga qarama-qarshi bo‘lsin. Fazodagi har bir ๐ด nuqtaning ๐‘‚
nuqtaga nisbatan vaziyati undan ๐‘‚ nuqtagacha bo‘lgan ๐‘Ÿ๐ด masofa, uning qutb
koordinatalar tekisligiga proeksiyasi bilan qutb o‘qi orasidagi ๐œ‘๐ด burchak, ๐‘‚๐ด kesma
bilan ๐‘‚๐‘ง o‘qining musbat yo‘nalishi orasidagi ๐œƒ๐ด burchak orqali aniqlash mumkin. Bu
holat ๐ด(๐‘Ÿ๐ด , ๐œ‘๐ด , ๐œƒ๐ด ) kabi yoziladi. Hosil bo‘lgan {๐‘‚, ๐‘Ÿ, ๐œ‘, ๐œƒ} sistema sferik
koordinatalar sistemasi deyiladi.
Qutb koordinatalar tekisligini sferik koordinatalar sistemasining fundamental
tekisligi deb ham yuritishadi; ๐‘Ÿ masofani radius, ๐œ‘ burchakni azimut, ๐‘‚๐‘ง o‘qini
zenit, ๐œƒ burchakni zenit burchagi deyishadi.
{๐‘‚, ๐‘Ÿ, ๐œ‘, ๐œƒ} sferik koordinatalar sistemasidagi kattaliklar
0 ≤ ๐‘Ÿ < +∞,
๐‘ง
0 ≤ ๐œ‘ < 2๐œ‹,
๐œƒ๐ด
๐‘Ÿ๐ด
๐ด
0≤๐œƒ≤๐œ‹
๐‘‚
๐œ‘๐ด
๐‘ƒ
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Multidisciplinary Scientific Journal
May, 2023
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GOLDEN BRAIN
ISSN: 2181-4120
VOLUME 1 | ISSUE 14 | 2023
shartlarni qanoatlantirishi talab etiladi.
๐ด nuqtaning
(๐‘Ÿ๐ด , ๐œ‘๐ด , ๐œƒ๐ด ) koordinatalaridan
sferik
Dekart
(๐‘ฅ๐ด , ๐‘ฆ๐ด , ๐‘ง๐ด )
koordinatalariga quyidagicha o‘tiladi:
๐‘ฅ๐ด = ๐‘Ÿ๐ด cos ๐œ‘๐ด sin ๐œƒ๐ด ,
๐‘ฆ๐ด = ๐‘Ÿ๐ด sin ๐œ‘๐ด sin ๐œƒ๐ด ,
๐‘ง๐ด = ๐‘Ÿ๐ด cos ๐œƒ๐ด.
Teskari, ya’ni ๐ด nuqtaning (๐‘ฅ๐ด , ๐‘ฆ๐ด , ๐‘ง๐ด ) Dekart koordinatalaridan uning sferik
(๐‘Ÿ๐ด , ๐œ‘๐ด , ๐œƒ๐ด ) koordinatalariga o‘tish quyidagi almashtirishlar orqali bajariladi:
๐‘Ÿ๐ด = √๐‘ฅ๐ด2 + ๐‘ฆ๐ด2 + ๐‘ง๐ด2 ,
๐‘ฆ
๐‘ง
๐œ‘๐ด = ๐‘Ž๐‘Ÿ๐‘๐‘ก๐‘” ๐ด ,
๐‘ฅ๐ด
๐‘ง๐ด
๐œƒ๐ด = ๐‘Ž๐‘Ÿ๐‘๐‘ก๐‘”
2 +๐‘ฆ 2
√๐‘ฅ๐ด
๐ด
๐‘ง๐ด
.
๐ด
๐œƒ๐ด
๐‘‚
ADABIYOTLAR
๐œ‘๐ด
๐‘ฆ๐ด
๐‘ฆ
1. ะ.ะ. ะ—ะฐะธั‚ะพะฒ. ะญะปะตะผะตะฝั‚ั‹ ะปะธะฝะตะนะฝะพะน ะฐะปะณะตะฑั€ั‹ ะธ
๐‘ฅ
๐‘ฅ
ะฐะฝะฐะปะธั‚ะธั‡ะตัะบะพะน ะณะตะพะผะตั‚ั€ะธะธ. ะฃั‡ะตะฑะฝะพะต
๐‘ƒ
ะฟะพัะพะฑะธะต. – ะขะฐัˆะบะตะฝั‚: «Zuxra baraka biznes.”
– 123 ั.
2. ะ. ะ. ะ—ะฐะธั‚ะพะฒ. ะญะปะตะผะตะฝั‚ั‹ ะดะธั„ั„ะตั€ะตะฝั†ะธะฐะปัŒะฝะพะณะพ ะธัั‡ะธัะปะตะฝะธั. ะฃั‡ะตะฑะฝะพะต ะฟะพัะพะฑะธะต.
– ะขะฐัˆะบะตะฝั‚: ะธะทะด-ะฒะพ ะขะ“ะŸะฃ. – 131 ั.
3. A. A. Zaitov, A. Ya. Ishmetov. Matematika 1. O‘quv qo‘llanma. – Toshkent:
“Zuxra baraka biznes” – 225 bet.
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Fizika-matematika fanlari jurnali, 3(1).
5. D. U. Bozarov. Matritsalar mavzusini mustaqil o‘zlashtirishga doir misollar
//ะœัƒา“ะฐะปะปะธะผ าณะฐะผ ัƒะทะปะธะบัะธะท ะฑะธะปะธะผะปะตะฝะดะธั€ะธัž. – 2022. – ะข. 3. – โ„–. 3.
6. A.R.Qutlimurotov. Oสป.H.Bozorova “Geometrik almashtirishlar” Academic
research in educational sciences.-2021
8. Bozarov D. U. Chiziqli va kvadratik modellashtirish mavzusini mustaqil
o’rganishga doir misollar //Eurasian journal of mathematical theory and
computer sciences. – 2022. – ะข. 2. – โ„–. 6. – ะก. 24-28.
9. https://t.me/zaamath
10. https://in-academy.uz/index.php/EJMTCS/article/view/2606
๐ด
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Multidisciplinary Scientific Journal
May, 2023
220
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