KYA chahiye humein: Rn(x) ka ek usable formula.
KYU hum ise directly compute nahi kar sakte: agar hume f(x) exactly pata hoti toh approximation ki zaroorat hi nahi hoti. Isliye humein ek bound chahiye.
Hum ise Mean Value Theorem se derive karte hain, generalized form mein. Yeh sabse clean tarika hai.
Derivation (Cauchy MVT trick).x ko fix karo. a ko variable t maano aur define karo:
g(t)=f(x)−∑k=0nk!f(k)(t)(x−t)k.
Yeh step kyun?g(t) bas woh remainder hai jab hum t par center karte hain. Note karo g(x)=0 (x par centered Taylor polynomial f(x) ke barabar hai) aur g(a)=Rn(x).
g(t) ko differentiate karo. Lagbhag sab kuch telescope ho jaata hai:
g′(t)=−n!f(n+1)(t)(x−t)n.
Yeh step kyun? Consecutive k ke product-rule terms cancel ho jaate hain — yahi Taylor structure ka kamaal hai. Sirf top derivative bachti hai.
Ab h(t)=(x−t)n+1 introduce karo, toh h(x)=0, h(a)=(x−a)n+1, aur h′(t)=−(n+1)(x−t)n.
Cauchy Mean Value Theorem ko g aur h par [a,x] par apply karo: koi c exists karta hai a aur x ke beech jisme:
h(a)−h(x)g(a)−g(x)=h′(c)g′(c).
Yeh step kyun? Cauchy MVT do functions ki rates compare karta hai; isse unknown c appear hota hai.
Sab kuch substitute karo:
(x−a)n+1−0Rn(x)−0=−(n+1)(x−c)n−n!f(n+1)(c)(x−c)n=(n+1)!f(n+1)(c).
(x−c)n cancel ho jaata hai, aur exactly Lagrange form milta hai. ■
Socho tum memory se kuch pencil strokes mein ek smooth hill draw kar rahe ho (yahi Taylor polynomial hai). Remainder theorem ek rule hai jo kehta hai: "tera sketch itne se zyada galat nahi hai." Woh "itna" nikalne ke liye, tum dekhte ho ki hill kitni wildly bend karti hai (next derivative) jitni stretch tumne draw ki, usse kitna door gaye ussse multiply karo, aur ek bade factorial number se divide karo jo jaldi error ko chhota bana deta hai. Toh kuch strokes se short walk ke liye almost perfect guarantee milti hai.