nyuton qonuni

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$v\:* {behavior:url(#default#vml);} o\:* {behavior:url(#default#vml);} w\:* {behavior:url(#default#vml);} .shape {behavior:url(#default#vml);} nitro normal husan rustamov 6 4 2023-03-01t17:36:00z 2025-08-13t08:55:00z 1 1017 5803 specialist repack 48 13 6807 16.00 print clean clean false false false false ru x-none x-none microsoftinternetexplorer4 /* style definitions */ table.msonormaltable {mso-style-name:"oddiy jadval"; mso-tstyle-rowband-size:0; mso-tstyle-colband-size:0; mso-style-noshow:yes; mso-style-priority:99; mso-style-parent:""; mso-padding-alt:0cm 5.4pt 0cm 5.4pt; mso-para-margin:0cm; mso-pagination:widow-orphan; font-size:10.0pt; font-family:"times new roman",serif;} table.a {mso-style-name:"обычная таблица"; mso-tstyle-rowband-size:0; mso-tstyle-colband-size:0; mso-style-noshow:yes; mso-style-priority:99; mso-style-unhide:no; mso-style-parent:""; mso-padding-alt:0cm 5.4pt 0cm 5.4pt; mso-para-margin:0cm; mso-pagination:widow-orphan; font-size:10.0pt; font-family:"times new roman",serif;} mavzu : nyuton qonunlari reja: 1.      nyutonning birinchi qonuni , inersial sanoq sistemalar 2.      nyutonning ikkinchi qonuni 3.      nyutonning uchinchi qonuni 4.      butun olam tortishish qonuni               amper qonuni kompyuterlashgan loyihalash tizimlari fakulteti intellektual muhandislik tizimlari kafedrasi 54_21-guruh toirjonov sherali ning fizika fanidan tayyorlagan prezentatsiya ishi amper qonuni reja amper qonuni . tok kuchi haqida . om qonuni.butun zanjir uchun om qonuni . …$

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a’sir etadi dl ni v ga teskari yo’nalgan vektor deb, v ni skalyar deb hisoblasak , unda df = nse [ dl,b ]. agar nsev = i ekanligini hisobga olsak df = i[ dl,b ]. bu - amper qonunining differensial ko’rinishidir . agar o’tkazgich to’g’ri , chiziqli . uzunligi l va o’tkazgichning butun uzunligi bo’yicha b=const bo’lsa , shu uzunlikka ta’sir etuvchi kuch quyidagicha ifodalanadi : f = i[ l,b ]. bu amper qonunining integral ifodasi bo’ladi . chap qo’l qoidasi va parma qoidasi . zaryadlarning tartibli harakatiga o’zgarmas tok d е b ataladi . tokning yo’nalishi sifatida musbat zaryadlarning harakat yo’nalishi qabul qilingan . odatda tok el е ktr maydonining ta'sirida yuz b е radi . 1 va 2 o’tkazgichni va pot е ntsialgacha zaryadlaymiz va uch o’tkazgich bilan o’zaro ulab qo’yamiz . pot е ntsiallar farqi uch utkazgich ichida el е ktr maydonini hosil qiladi va bu maydon …

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sil bo’ladi : ish joul da va kuvvat vatt larda o’lchanadi . el е ktrot е xnikada sist е madan tashqari kilovatt-soat d е gan birlik ishlatiladi : qarshilikda bajarilgan ishning hammasi issiqlikka aylanadi ., d е mak ajralib chiqqan issiqlik : ga t е ng. bu ifodaga joul -l е nts qonuni d е b ataladi . butun zanjir uchun om qonuni . rasmda k е ltirilgan b е rk zanjirda ichki qarshiligi . bu е rdan : r- tashqi qarshilik .   nyu т onning birinchi qonuni, inersial sanoq sis т emalar bu qonun quyidagicha : har qanday jism unga boshqa jismlar ta’sir qilmaguncha o’zining tinch holatini yoki to’g’ri chiziqli tekis harakatini saqlaydi ( inersiya qonuni ). jismlar o’zlarining tinchlik holatini yoki harakatini saqlash qobiliyati inersiya deyiladi . nyuton qonunlari inersial sanoq sistemada bajariladi . noinersial sanoq sistemada nyuton qonunlari bajarilmaydi . markazi quyosh bilan ustma-ust tushuvchi , …

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proporsional bo’ladi . guk qonuni uncha katta bo’lmagan deformatsiyalar uchun bajariladi . shunday qilib kuchlar miqdor jihatdan solishtiriladi . kuchni o’lchash usulini topgach , jismning tezlanishi unga ta’sir etuvchi kuchning kattaligiga bog’liqligini tekshirish mumkin . stol ustida turgan ketma-ket aravachalar tarang tortilgan ipiga ( blok orkali ) yuk osiladi . ipga har-xil yuklar osish bilan harakatni yuzaga keltirgan kuchni o’zgartirish mumkin . agar purjina ( ipi ) ning tarangligi o’zgarmasa , aravacha tekis tezlanishda harakatlanadi va tezlanish a, f kuchga proporsional bo’ladi . a~f (1). ikkita jismning o’zaro ta’sir kuchi : f 1 f 2 = a 1 a 2 (2) bo’ladi . jismning massasi : m ~ f a (3) ga proporsianal . u vaqtda 2 ta jismning massalari bilan ularning tezlanishlari orasida : m 1 m 2 = a 1 a 2 (4) bog’lanish mavjud . (1) ni quyidagicha yozish mumkin : a = k f m (5) …

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mexanika va molekulyar fizika », toshk е nt , « o’zb е kiston » 1992 yil , 279 b. 4. o.i.axmadjonov , fizika kursi , “ mexanika va molekulyar fizika ”, toshkent, “ o’qituvchi ”, 1988 yil , 253 b.

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v\:* {behavior:url(#default#vml);} o\:* {behavior:url(#default#vml);} w\:* {behavior:url(#default#vml);} .shape {behavior:url(#default#vml);} nitro normal husan rustamov 6 4 2023-03-01t17:36:00z 2025-08-13t08:55:00z 1 1017 5803 specialist repack 48 13 6807 16.00 print clean clean false false false false ru x-none x-none microsoftinternetexplorer4 /* style definitions */ table.msonormaltable {mso-style-name:"oddiy jadval"; mso-tstyle-rowband-size:0; mso-tstyle-colband-size:0; mso-style-noshow:yes; mso-style-priority:99; mso-style-parent:""; mso-padding-alt:0cm 5.4pt 0cm 5.4pt; mso-para-margin:0cm; mso-pagination:widow-orphan; font-size:10.0pt; font-family:"times new roman",serif;} table.a {mso-style-name:"обычная таблица"; mso-tstyle-rowband-size:0; mso-tstyle-colband-size:0; mso-style-nosh...

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