Malyus qonuni.
Yorug`likning qutblanish qonunini tekshirish uchun
poyarizatorlardan foydalaniladi. Bu o`rinda ular analizatorlar deb ataladi.
Ikkita polyarizator olamiz. Ularning biriga (P polyarizatorga) tabiiy
yorug`lik tushirsak, u yorug`likni yassi qutblab beradi (7-rasm). Bu yassi
qutblangan yorug`lik intensivligini I
0
deb belgilaymiz. Endi ana shu yassi
qutblangan yorug`lik yo`liga A analizatorni shunday qo`yamizki, uning O
1
O`
1
optik o`qi P polyarizatorning OO` o`qi bilan φ burchak tashkil qilsin (7b-rasm). U
holda analizatordan tebranish amplitudasi E= E
0
cos φ bo`lgan yorug`lik to`lqini
o`tadi. Demak, A analizatordan o`tayotgan yorug`lik intensivligi
61
7-rasm
(11)
ifoda bilan aniqlanadi. Bu (11) munosabat
Malyus qonuni
deb yuritiladi. Bizga
ma`lumki,
, bunda I
tab
- polyarizatorga tushayotga tabiiy yorug`lik
intensivligi. U holda polyarizator hamda analizator orqali o`tgan yorug`lik
intensivligi quyidagiga teng bo`ladi:
(12)
Maksimal intensuvlik
ga teng bo`lib, u φ=0 da (polyarizator
analizatorlarning optic o`qlari o`zaro parallel bo`lganda ) hosil bo`ladi. φ=π/2
bo`lganda intensivlik nolga teng bo`ladi, ya`ni analizatordan yorug`lik o`tmaydi.
Boshqa hollarda I intensivlik φ burchak kattaligiga bog`liq ravishda o`zgarib
boradi.
Malyus qonunini tekshirish
. Eksperimental qurilmaning prinsipial
sxemasi 8-rasmda keltirilgan. Bunda Ф - yoritkich lampa (fonar), D -
diafragma, P -polarizator, A - analizator, ФЭ - fotoelement, G - galvanometmi
bildirib, ularning hammasi reyterlar yordamida ОТ optik taglikka o ‘matiladi.
P polarizator va A analizator doira shaklida yasalgan va maxsus halqa
ko‘rinishidagi asbobga o ‘rnatilgan polaroidlardan iborat. Analizator o
‘matilgan halqaning gardishiga graduslarda darajalangan shkala yopishtirilgan.
Analizatomi aylantirib, halqadagi shkaladan analizatoming polarizatorga
nisbatan burilish burhagini o ‘lchash mumkin.
8-rasm.
62
Ishni bajarish tartibi
1.
Yoritgich lampa tok manbaiga ulanadi.
2.
Polaroid optic o`qlari o`zaro parallel bo`lgan holatda joylahtiriladi va
polyarizatorning shu holati saqlanadi.
3.
Analizatorni burib, φ burchakning 0
o
, 10
o
, 20
o
, …., 90
o
qiymatlarida i
φ
fototok qiymatlari yozib olinadi.
4.
Analizatorni teskari yo`nalishda burib, φ burchakning 90
o
, 80
o
, 70
o
, ….,
0
o
qiymatlari uchun
qiymatlari yozib olinadi.
5.
O’lchash natijalaridan foydalanib, φ ning ma`lum qiymati uchun
fototokning
o`rtacha qiymati va
nisbat hisoblanadi.
6.
Natijlar jadvalga yoziladi.
7.
Jadvaldan foydalanib,
bog`lanish grafigi chiziladi, bu
ifodaga kirgan I
0
va I
φ
lar polaroidlar optic o`qlarining orasidagi burchak
mos ravishda 0
o
(o`qlari o`aro parallel) va φ ga teng bo`lganda
fotoelementga tushgan tushgan yorug`lik intensivligini bildiradi.
Shu chizmaning o`zida
funksiya grafigi ham chiziladi. Ikkala
(eksperimental va nazariy) olingan egri chiziqlarni solishtirib, tajribada
qo`llanilgan polaroidlar Malyus qonunini qanchalik qanoatlantirilishi haqida
fikr yuritiladi.
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MUNDARIJA
Laboratoriya ishlarini bajarish jarayonida talabalarga qo‘yiladigan talablar…….
3
O‘lchash natijalarini ishlab chiqish. Xatoliklarning elementar nazariyasi.
Sistematik va tasodifiy xatoliklar……………………………………………………
5
1-laboratoriya ishi. Ignalar yordamida yassi parallel shisha plastinkaning nur sindirish
ko’rsatkichini aniqlash.……………………................................................................
11
2-laboratoriya ishi. Difraktsion panjara yordamida yorug`lik to`lqinining uzunligini
aniqlash.
………………………………………………..…………………………….
16
3-laboratoriya ishi.
Linzaning egrilik radiusini Nyuton (o`tgan to`lqinlar uchun) halqasi
yordamida aniqlash
…………………………………………………………………….
22
4-laboratoriya ishi.
Yorug‘likning suyuqlikda yutilishini aniqlash
……..………………...
32
5-laboratoriya ishi.
Bug‘ va gazlarning nurlanish spektrlarini o‘rganish…
………………..
45
6-laboratoriya ishi. Yorug’likning qutblanish darajasini aniqlash. Malyus qonunini
o’ragish
……………………………………………………………….
….
56
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