Pythagoras ko scratch se dobara banana (kuch memorise karne ki zaroorat nahi). Apne triangle ki char copies ko ek tilted square ke around rakho jiska side chord Li hai. Bada bahari square ka side Δxi+Δyi hai. Uska area tilted inner square (Li2) aur char triangles (4×21ΔxiΔyi) ke barabar hai:
big square(Δxi+Δyi)2=tilted squareLi2+four triangles4⋅21ΔxiΔyi
Left side expand karo: (Δxi)2+2ΔxiΔyi+(Δyi)2. 2ΔxiΔyi triangles ko cancel kar deta hai, aur milta hai
Li=(Δxi)2+(Δyi)2.
(Δxi)2 — sideways travel, squared.
(Δyi)2 — vertical travel, squared.
— squaring ko undo karta hai taaki actual length mile. Dekho Pythagorean theorem.
Li=(Δxi)2+(Δyi)2=(Δxi)2(1+(Δxi)2(Δyi)2)=1+(chord ki tiltΔxiΔyi)2Δxi
Hum Δxi ko root se bahar nikal sake kyunki Δxi>0 (hum hamesha left-to-right chalte hain — yeh exactly Step 1 ka "no doubling back, advance rightward" assumption hai — toh (Δxi)2=Δxi, koi minus sign nahi).
1 sideways leg se bacha hua hai — yeh wahi hai jo humein horizontal travel bhoolne se rokta hai.
ΔxiΔyi = vertical-move ÷ right-move = chord ka slope (ek "secant slope"). Agar chord gire, yeh ratio negative hai — lekin aage square ho jaata hai, toh phir sign wash out ho jaata hai.
Flat curve (f′=0). Vertical leg Δyi=0; triangle ek horizontal segment mein collapse ho jaata hai. Integrand =1+0=1, toh L=∫ab1dx=b−a — exactly width. ✓ Ek flat line ki length hai hi uska horizontal span.
Vertical wall (f′→∞). Slope blow up karta hai; y=f(x) formula choke karta hai kyunki vertical piece mein Δxi=0 hai (bahar nikalne ke liye kuch nahi). Fix:x=g(y) form par flip karo aur y mein integrate karo — vertical leg "safe" direction ban jaata hai.
Corner (slope jumps). Ek sharp kink par f′ exist nahi karta — yeh us ek point par MVT ki differentiability condition violate karta hai. Kyunki ek bura point zero width ka hota hai, integral unaffected rehta hai — bas corner par interval split karo aur do pieces add karo.
Film strip ko left-to-right padho: curve → chords → ek triangle → dx bahar nikalo → tangent chord se match karta hai → strips sum hokar integral bante hain. Har arrow upar ek step hai.
Recall Feynman: plain words mein poora walkthrough
Tum ek bumpy path ki length chahte ho. Curve ko directly maap nahi kar sakte, toh tum iske saath chhoti straight sticks end-to-end rakhte ho (Step 2). Har stick ek chote right triangle ki lambi side hai jiske legs hain "thoda sa rightward" aur "thoda sa upar ya neeche"; corner-square trick (Pythagoras) kehti hai stick ki length right2+vertical2 hai — aur kyunki vertical bit square hoti hai, koi farq nahi ki curve climb kare ya gire (Step 3). Sab kuch rightward steps par ek sum mein collect karne ke liye, rightward bit ko factor out karo aur milta hai 1+slope2 times the rightward step (Step 4). "Stick ka slope" curve ka real slope nahi hai bilkul, lekin Mean Value Theorem — jab tak curve smooth ho (continuous aur differentiable) — guarantee karta hai ki andar kahin real tangent exactly utni hi tilted hai, toh tum ise f′ se replace karo (Step 5). Ab har stick padhti hai 1+(f′)2Δx; infinitely many infinitely short ones add karna exactly wahi hai jo integral sign matlab hai, deta hai L=∫ab1+(f′)2dx (Step 6). Ise flat road par test karo (length = width), vertical cliff par (instead y mein integrate karo), aur sharp corner par (wahan split karo) — teeno se survive karta hai (Step 7). Wahi ds=dx2+dy2 baad mein surfaces of revolution, parametric aur polar lengths banata hai.