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2-rasm
.
vaqtdan so’ng etib keladi. υ
1
- birinchi muhitdagi yorug’lik tezligi. B nuqtada
ikkilamchi to’lqin uyg’ona boshlaganda A nuqtada yuzaga kelgan to’lqinlar AD=
υ
2
Δt radiusli yarim sferalar chizadilar. υ
2
- ikkinchi muhitdagi yorug’lik tezligi.
Shakldan <α=
ΔABS dan sinα=BS/AB= υ
1
Δt/AB (2)
ΔABD dan sinβ=AD/AB= υ
2
Δt/AB
(3)
(2) ifodadan AB ni topib (3) ifodaga qo’ysak,
(4)
Muhitning absolyut sindirish ko’rsatgichidan
dan foydalanib topiladi.
(5)
Bu yerda
m/s yorug’likning bo’shliqdagi tezligidir.
Demak, tushish burchagi sinusining sinish burchagi
sinusiga nisbati ikkinchi
muhitning birinchi muhitga nisbatan nisbiy sindirish ko’rsatgichiga teng bo’lar
ekan.
Ishni bajarish tartibi
1.
Yassi tekislikka penoplast taglik o’rnatiladi.
2.
Oq katakli qog’oz penoplast taglik ustiga qo’yiladi.
3.
Shisha plastinka qog’ozning o’rtasiga joylashtiriladi.
4.
Qog’ozga qalam bilan shisha plastinkaning sindiruvchi yoqlari bo’ylab
chiziladi.
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5.
Plastinkaning bir yog’i yaqinidagi A va B nuqtalarga ignalar tik holda
qadaladi. Plastinkaning ikkinchi yog’iga C va D ignalarni tik holda shunday
qadaladiki, shisha orqali qaralganda to’rtala ignalarning asoslari bir to’g’ri
chiziqda turgandek ko’rinadi.
6.
Ignalar olib tashlanib ular o’rinlari bekgilab olinadi.
Yorug’lik nuri AB yonalish bo’yicha shishaga tushadi.
B nuqtada u
singan C nuqtaga keladi. So’ngra shishaning ikkinchi tomonida CD
yo’nalish bo’yicha tarqaladi.
7.
Suvning sindirish ko’rsatgichini hisoblash uchun transporter yordamida α va
β burchaklar o’lchanadi. Ularning sinuslari qiymatlari (5) formulaga qo’yilib
n hisoblanadi.
Shakldan foydalangan holda hisoblash quyidagicha bajariladi:
;
AK, AB, NC kesmalarni chizg’ich bilan o’lchanadi va
n
hisoblanadi (3-rasm):
3-rasm.
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