2.5.5 · D3 · Physics › Optics › Total internal reflection — critical angle derivation
Yeh page critical-angle idea ki drill floor hai. Parent note ne humein woh ek formula diya jo is poore page pe kaam aayega:
Drill se pehle, chalte hain aur har tarah ke questions ki list banate hain jinme yeh ek formula dress up ho sakta hai. Agar hum har row mein ek example solve kar lein, toh exam mein koi cheez humein surprise nahi kar sakti.
Har critical-angle problem actually sin θ c = n 2 / n 1 ka rearrangement hai. Sirf teen "unknowns" hain jo pooche ja sakte hain, saath mein kuch edge cases bhi hain jahan formula thoda alag behave karta hai. Yeh raha poora map:
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Case class
Kya diya hai
Kya poochha hai
Kaun sa cell
1
Standard forward
n 1 , n 2 (dense→rare)
θ c
forward, do real media
2
Air ke against
n 1 , air
θ c
forward, n 2 = 1
3
Inverse
θ c , air
n 1
index ke liye solve karo
4
Two-media inverse
θ c , ek index
doosra index
index ke liye solve karo
5
Degenerate: equal indices
n 1 = n 2
θ c
limiting value θ c = 90°
6
Impossible: rarer→denser
n 1 < n 2
θ c ?
no solution case
7
Critical se aage
n 1 , n 2 , θ 1 > θ c
kya hoga?
sign/regime test
8
Word problem
fibre / underwater
θ c + matlab
real-world
9
Exam twist
prism / 45° geometry
kya TIR hoga?
compare-to-45°
Ab hum har cell ko hit karte hain.
Worked example Example 1 — Cell 1: standard forward, do real media
Light ek dense plastic (n 1 = 1.60 ) se oil (n 2 = 1.40 ) mein jaati hai. θ c nikalo.
Forecast: dono indices kaafi close hain, toh ray muskil se bend hogi — guess karo: kya θ c zyada 90° ke paas hoga ya 30° ke paas?
Direction check karo: n 1 = 1.60 > n 2 = 1.40 , dense→rare. ✅ TIR possible hai.
Yeh step kyun? Agar light doosri taraf jaati, toh koi critical angle exist hi nahi karta (Cell 6). Direction hamesha pehle verify karo.
Formula apply karo: sin θ c = n 1 n 2 = 1.60 1.40 = 0.875 .
Yeh step kyun? Yahi definition hai — refracted angle ko 90° set karo aur solve karo, jaise Snell's Law mein hai.
Sine ko invert karo: θ c = sin − 1 ( 0.875 ) = 61.0° .
Yeh step kyun? Humein angle ka sine pata hai; sin − 1 woh operation hai jo "sine of" ko undo karta hai aur angle wapas deta hai.
Verify karo: indices close hain (ratio near 1), toh θ c 90° ke paas hona chahiye — aur 61° wakai steep hai. Forecast confirmed. Wapas plug karo: sin 61.0° = 0.875 = 1.40/1.60 . ✅
Worked example Example 2 — Cell 2: forward against air
Diamond ka n 1 = 2.42 hai. Woh air (n 2 = 1 ) mein rakha hai. θ c nikalo.
Forecast: diamond ka index bahut bada hai. Bada index → kya θ c bada hoga ya chhota?
sin θ c = n 1 n 2 = 2.42 1 = 0.4132 .
Yeh step kyun? Air ke against, n 2 = 1 , toh formula sin θ c = 1/ n 1 tak reduce ho jaata hai.
θ c = sin − 1 ( 0.4132 ) = 24.4° .
Yeh step kyun? Angle read karne ke liye sine ko undo karo.
Verify karo: ek chhota critical angle matlab hai ki andar ka almost koi bhi ray trap ho jaata hai — bilkul isi wajah se cut diamonds itne sparkle karte hain (light bahar nikalne se pehle kai baar bounce karti hai). Sanity check: sin 24.4° = 0.413 . ✅
Worked example Example 3 — Cell 3: inverse,
θ c se index nikalo (air ke against)
Ek mystery liquid, air ke against measure ki gayi, ka θ c = 45.0° hai. Uska refractive index n nikalo.
Forecast: 45° ek "beech wala" critical angle hai. Kya n 1 ke paas aayega (jaise air) ya 2 ke paas (jaise glass)?
Air formula likho: sin θ c = n 1 .
Yeh step kyun? Air ke against n 2 = 1 hai, aur denser medium liquid hai, n 1 = n .
n ke liye rearrange karo: n = sin θ c 1 = sin 45° 1 = 0.7071 1 .
Yeh step kyun? Humein n akela chahiye, toh dono sides flip karo.
n = 1.414 .
Yeh step kyun? Yeh 2 hai — ek clean numeric value.
Verify karo: n = 1.414 water (1.33 ) aur glass (1.5 ) ke beech mein hai, jo ek physically reasonable liquid hai. Wapas plug karo: sin θ c = 1/1.414 = 0.707 = sin 45° . ✅
Worked example Example 4 — Cell 4: two-media inverse
Light glass (n 1 = 1.50 ) se ek unknown coating mein jaati hai. Us boundary par critical angle θ c = 60.0° hai. Coating ka index n 2 nikalo.
Forecast: TIR ke liye coating glass se rarer honi chahiye, toh guess karo: kya n 2 1.50 se upar hoga ya neeche?
sin θ c = n 1 n 2 se shuru karo.
Yeh step kyun? Dono media real hain (koi bhi air nahi hai), toh poora do-index form rakhte hain.
n 2 ke liye solve karo: n 2 = n 1 sin θ c = 1.50 × sin 60° = 1.50 × 0.8660 .
Yeh step kyun? Unknown index ko isolate karne ke liye dono sides ko n 1 se multiply karo.
n 2 = 1.299 ≈ 1.30 .
Yeh step kyun? Arithmetic.
Verify karo: 1.30 < 1.50 , toh coating genuinely rarer hai — TIR possible hai, jo is baat ke consistent hai ki wahan ek critical angle hai hi. ✅
Worked example Example 5 — Cell 5: degenerate, equal indices
Do media dono ka n = 1.50 hai (woh optically identical hain). θ c kya hai?
Forecast: agar media identical hain, toh kya koi aisi boundary bhi hai jo light ko bend kare? Kaunsa angle light ko "trap" karta?
sin θ c = n 1 n 2 = 1.50 1.50 = 1 .
Yeh step kyun? Equal indices plug karo — ratio exactly 1 aata hai.
θ c = sin − 1 ( 1 ) = 90° .
Yeh step kyun? Sirf wahi angle jiska sine 1 ke barabar ho, woh 90° hai.
Verify karo: θ c = 90° ka matlab hai ki "critical" angle grazing incidence hai — light tab hi trap ho sakti hai jab woh surface ke saath exactly flat chale, yaani effectively kabhi nahi . Yeh sahi hai: jab koi index difference nahi hota toh koi bending nahi hoti (dekho Refraction of Light ), toh TIR occur nahi ho sakta. Formula gracefully limiting value 90° report karta hai. ✅
Worked example Example 6 — Cell 6: impossible direction (rarer → denser)
Light air (n 1 = 1.00 ) se glass (n 2 = 1.50 ) mein jaati hai. Koi critical angle poochh raha hai. Nikalo — ya explain karo kyun nahi nikala ja sakta.
Forecast: light denser medium mein ja rahi hai. Kya TIR yahan sense bhi banta hai?
Blindly formula apply karo: sin θ c = n 1 n 2 = 1.00 1.50 = 1.50 .
Yeh step kyun? Contradiction expose karne ke liye, formula ko bolne dete hain.
Poochho: kya sin θ c = 1.50 ho sakta hai? Nahi. Kisi bhi real angle ka sine [ − 1 , 1 ] mein hota hai.
Yeh step kyun? sin θ c = 1.5 ka koi real solution nahi hai — geometrically, aisa koi angle exist nahi karta.
Conclude karo: rarer→denser jaate waqt koi critical angle nahi hota . TIR is direction mein impossible hai.
Yeh step kyun? Denser medium mein refraction hamesha succeed karta hai (ray normal ki taraf bend hoti hai), toh light kabhi "trap" nahi hoti.
Verify karo: yeh parent note ki pehli condition se match karta hai — TIR ke liye n 1 > n 2 chahiye. Yahan n 1 < n 2 hai, toh machinery sahi se refuse kar rahi hai. ✅
Worked example Example 7 — Cell 7: critical angle se aage
Water ke andar (n 1 = 1.33 , air n 2 = 1 ) ek ray surface se θ 1 = 60° par takraati hai. Pehle θ c nikalo, phir decide karo is ray ka kya hoga.
Forecast: kya 60° water ke critical angle se upar hai ya neeche? Ray kya karti hai?
Critical angle: sin θ c = 1.33 1 = 0.7519 ⇒ θ c = 48.8° .
Yeh step kyun? Compare karne se pehle threshold chahiye.
Compare karo: θ 1 = 60° > 48.8° = θ c .
Yeh step kyun? Regime decide hota hai is baat se ki hum θ c se upar hain ya neeche.
Kyunki θ 1 > θ c hai, Snell ko chahiye hoga sin θ 2 = n 2 n 1 sin θ 1 = 1.33 × sin 60° = 1.33 × 0.8660 = 1.152 > 1 .
Yeh step kyun? Snell ka demand check karne se pata chalta hai ki woh kuch impossible maang raha hai.
Koi refracted ray nahi → total internal reflection : 100% light wapas water mein bounce kar jaati hai.
Yeh step kyun? Energy ko kahin jaana hai; refraction forbidden hone par, reflection sab le leta hai.
Verify karo: sin θ 2 = 1.152 > 1 impossibility confirm karta hai, aur 60° > 48.8° confirm karta hai ki hum threshold se aage hain. Dono tests agree karte hain. ✅
Worked example Example 8 — Cell 8: real-world word problem (optical fibre)
Ek optical fibre core ka n 1 = 1.50 hai, jo cladding n 2 = 1.45 se ghiri hui hai. Core ke andar bounce karta hua light core–cladding wall se takraata hai. θ c nikalo, aur woh range of angles batao jo trapped rehti hain.
Forecast: dono indices bahut close hain. Kya trapping angle 90° ke paas hogi (narrow trap) ya 0° ke paas?
Direction check: 1.50 > 1.45 , dense→rare. ✅
Yeh step kyun? Fibres deliberately core mein denser glass rakhte hain taaki light trap ho sake.
sin θ c = 1.50 1.45 = 0.9667 .
Yeh step kyun? Rarer (cladding) over denser (core).
θ c = sin − 1 ( 0.9667 ) = 75.2° .
Yeh step kyun? Sine ko undo karo.
Trapped range: wall se θ 1 ke saath jo bhi ray 75.2° aur 90° ke beech strike kare, woh TIR undergo karegi.
Yeh step kyun? θ c se upar ke (grazing tak) saare incidence angles totally reflect hote hain.
Verify karo: close indices ek bada θ c dete hain jo 90° ke paas hai, matlab light ko fibre axis ke almost parallel chalana padta hai andar rehne ke liye — exactly isi wajah se fibres tiny index differences ke saath engineer kiye jaate hain aur light shallow angles par launch ki jaati hai. ✅
Worked example Example 9 — Cell 9: exam twist (45° prism)
Ek right-angled glass prism (n = 1.50 , bahar air hai) mirror ki tarah use hota hai: light slanted face se exactly 45° par takraati hai. Kya yeh TIR undergo karega? (Yeh periscope prism trick hai.)
Forecast: incidence 45° par fixed hai. Humein isse θ c se compare karna hai — kya 45° jeet payega?
Glass–air ke liye θ c nikalo: sin θ c = 1.50 1 = 0.6667 ⇒ θ c = 41.8° .
Yeh step kyun? Threshold woh hai jo 45° ko beat karna hai.
Compare karo: 45° > 41.8° = θ c .
Yeh step kyun? TIR tab hota hai jab incidence critical angle se zyada ho.
Conclusion: haan — light totally internally reflect hoti hai, toh prism bina silvering ke perfect mirror ki tarah kaam karta hai.
Yeh step kyun? Kyunki 45° threshold clear kar deta hai, poori energy reflect hoti hai.
Verify karo: 45° − 41.8° = 3.2° ka margin hai — TIR hota hai, lekin barely . Agar glass low-index hota (n < 1/ sin 45° = 1.414 ), toh θ c 45° se zyada hota aur trick fail ho jaati. Hamara n = 1.50 > 1.414 hai, toh hum safely upar hain. ✅
Recall Rapid-fire self-test (answers cover karo)
Glass n = 1.5 into air, θ c ? ::: sin − 1 ( 1/1.5 ) ≈ 41.8° .
Diamond n = 2.42 into air, θ c ? ::: sin − 1 ( 1/2.42 ) ≈ 24.4° .
Liquid jiska θ c = 45° air ke against, uska n ? ::: 1/ sin 45° = 1.414 .
Equal indices n 1 = n 2 , θ c ? ::: 90° (koi real trapping nahi).
Air into glass, θ c ? ::: exist nahi karta — galat direction, sin θ c = 1.5 > 1 .
Fibre core 1.50 , cladding 1.45 , θ c ? ::: sin − 1 ( 1.45/1.50 ) ≈ 75.2° .
Mnemonic Sab kuch ek sentence mein
"Pehle direction, phir formula, phir threshold se compare." Dense→rare confirm karo, sin θ c = n rarer / n denser compute karo, phir poochho ki actual incidence θ c ko beat karta hai ya nahi.