2.5.6 · Physics › Optics
Intuition Bada picture (WHY lenses light ko modte hain)
Ek lens bas do refracting surfaces ko jod kar banaya hota hai. Light har ek surface par isliye modti hai kyunki glass aur air ke beech light ki speed badal jaati hai (Snell's law). "Thin" lens ka matlab hai ki sheesha itna patla hai ki hum light ke andar travel karne ki distance ignore kar dete hain — to hum dono surfaces ki bending ko ek hi point par add kar dete hain. Neeche sab kuch usi ek idea ka bookkeeping hai.
Definition Thin lens aur sign convention (Cartesian, real-is-positive light goes →)
Thin lens : thickness ≪ object/image distances, isliye dono surfaces ek hi plane par act karte hain (optical centre).
Distances lens se measure ki jaati hain, light direction ke along.
Object distance u : incoming side par real object ⇒ u < 0 .
Image distance v : outgoing side par real image ⇒ v > 0 .
Focal length f : ==converging lens f > 0 ==, diverging f < 0 .
Kisi surface ka radius R : R > 0 agar uska centre of curvature outgoing side par ho.
HUM KYA CHAHTE HAIN: object position aur lens shape diye hue, find karna hai ki image kahan banti hai. Do equations ye kaam karti hain:
Lens equation u , v , f ko relate karta hai (lens ko black box ki tarah use karta hai).
Lens maker's equation f ko glass ki shape (R 1 , R 2 , n ) se compute karta hai.
Intuition YE YAHAAN SE KYUN SHURU KAREIN?
Agar main ek curved glass surface par bending describe kar sakta hoon, to main ise bas do baar apply kar deta hoon. Ek baar derive karo, baar baar use karo.
Radius R wali ek single surface ke liye jo media n 1 (incoming) aur n 2 (outgoing) ko alag karti hai, object–image relation hai single-surface refraction formula :
v n 2 − u n 1 = R n 2 − n 1
Worked example HUM ISSE KAISE DERIVE KARTE HAIN (paraxial, first principles)
Ye step kyun? Chhote angles ke liye Snell's law use karo taaki sin θ ≈ θ .
Axial object O se ek ray surface par height h par hit karti hai, normal ke saath angle i par (normal centre C se guzarta hai). Snell: n 1 i = n 2 r (paraxial).
Exterior-angle geometry use karke (angles chhote, isliye tan θ ≈ θ ≈ h / distance ):
i = α + ϕ , jahan α = − u h (object) aur ϕ = R h (radius).
r = ϕ − β , jahan β = v h (image).
Ye step kyun? n 1 i = n 2 r mein substitute karo aur common h cancel karo:
n 1 ( − u h + R h ) = n 2 ( R h − v h )
− u n 1 + R n 1 = R n 2 − v n 2
Rearrange karne par: v n 2 − u n 1 = R n 2 − n 1 . ∎
Definition ke anusaar f wo jagah hai jahan parallel rays (u → − ∞ ) focus hoti hain, jo deta hai v 1 = f 1 . To:
f 1 = ( n − 1 ) ( R 1 1 − R 2 1 ) Lens maker’s equation
Aur compare karne par, thin-lens (Gaussian) equation :
v 1 − u 1 = f 1
f determine karta hai
( n − 1 ) = "glass mein light kitni slow hai" → agar n bada hai to zyada bending. ( 1/ R 1 − 1/ R 2 ) = "kitna strongly curved hai" → tighter curves zyada modte hain. Flat plate (R → ∞ ) ke liye 1/ f = 0 : wo kuch nahi karta.
Worked example (A) Biconvex lens,
f find karo
Glass n = 1.5 , R 1 = + 20 cm (pehli surface outgoing ki taraf bulge karti hai → centre outgoing side par, + ), R 2 = − 20 cm.
Ye signs kyun? Doosri surface ulti taraf curve karti hai, centre incoming side par ⇒ negative.
f 1 = ( 1.5 − 1 ) ( 20 1 − − 20 1 ) = 0.5 ⋅ 20 2 = 10 0.5 = 0.05 cm − 1
f = + 20 cm. Positive ⇒ converging. ✔
Worked example (B) Lens equation se image position
Same lens f = 20 cm, object 30 cm saamne ⇒ u = − 30 cm.
Ye step kyun? v 1 − u 1 = f 1 mein plug karo:
v 1 = f 1 + u 1 = 20 1 + − 30 1 = 60 3 − 2 = 60 1
v = + 60 cm (real, outgoing side). Magnification m = v / u = 60/ ( − 30 ) = − 2 ⇒ inverted, do guna bada. ✔
Worked example (C) Diverging lens
f = − 15 cm, u = − 10 cm.
v 1 = − 15 1 + − 10 1 = 30 − 2 − 3 = − 30 5 = − 6 1 ⇒ v = − 6 cm
Negative ⇒ virtual image incoming side par, m = v / u = ( − 6 ) / ( − 10 ) = + 0.6 seedha, chota — exactly wohi jo ek diverging lens karta hai. ✔
v 1 + u 1 = f 1 use karna (mirror form)
Ye sahi kyun lagta hai: mirrors mein "+" use hota hai aur equations ek jaisi lagti hain.
Fix: Lenses ke liye (Cartesian convention) ye ek minus hai: v 1 − u 1 = f 1 . Kyunki real object ke liye u already negative hai, algebra mirror ke "+" jaisa hi end up hota hai — lekin sign rule yaad rakho, memorised pattern nahi.
Common mistake Maker's equation mein
R 2 ka sign bhool jaana
Ye sahi kyun lagta hai: dono faces "same taraf curve hote lagte hain", isliye tum 1/ R 1 + 1/ R 2 likh dete ho.
Fix: Har face ke liye centre-of-curvature rule alag se use karo. Symmetric biconvex lens ke liye R 1 = + R , R 2 = − R , isliye minus sign ke through add hote hain: f 1 = ( n − 1 ) R 2 .
Common mistake Ye sochna ki
f is baat par depend karta hai ki light kis side se enter kare
Ye sahi kyun lagta hai: dono surfaces alag hain.
Fix: Sides swap karne par R 1 ↔ R 2 swap aur re-sign ho jaata hai; maker's equation same f deta hai. Ek thin lens ka ek hi focal length hota hai.
Single spherical surface formula v n 2 − u n 1 = R n 2 − n 1
Lens maker's equation f 1 = ( n − 1 ) ( R 1 1 − R 2 1 )
Thin-lens (Gaussian) equation v 1 − u 1 = f 1
Derivation mein intermediate image kyun gayab ho jaata hai? Do single-surface equations add karne par n / v 1 term cancel ho jaata hai
R ka sign ruleR > 0 agar centre of curvature outgoing (transmission) side par ho
Magnification formula m = h h ′ = u v
Flat plate (R → ∞ ) ke liye f kya hai? Infinite power zero — 1/ f = 0 , koi focusing nahi
Converging lens mein f ka sign Positive (f > 0 )
f = 20 cm lens ke saamne 30 cm par object, v find karov = + 60 cm, real, m = − 2 inverted
Light ka glass mein "slow" hona bending ke liye kyun zaroori hai? ( n − 1 ) factor; agar n = 1 to speed change nahi, bending nahi
Recall Feynman: 12 saal ke bacche ko samjhao
Socho ek marching band road se hata kar keechar wali grass par angle se chal rahi hai. Jo side pehle keechar mein aati hai wo slow ho jaati hai, isliye poori line swing karti hai. Glass light ke liye keechar hai. Ek lens ke do curved keechar wale edges hote hain; light har ek par thodi swing karti hai. Agar dono swings light ko ek jagah push karti hain, to saari rays wahin milti hain — wohi image hai! Mota, zyada curved glass = zyada swing = milne ka point aur paas.
Mnemonic Maker's equation yaad karo
"n-minus-one times curve-difference" → ( n − 1 ) ( R 1 1 − R 2 1 ) .
Aur lens equation ke liye "v-minus-u equals f" (sab reciprocals). Lens = minus , Mirror = plus .
Refraction at a single spherical surface
Snell's law & paraxial approximation
Spherical mirrors — mirror equation
Magnification and image formation
Power of a lens (dioptres)
Lens combinations & equivalent focal length
Lens aberrations (chromatic, spherical)
Single-surface refraction
Sign convention Cartesian