4.4.6 · Maths › Multivariable Calculus
Single-variable calculus mein, ek function a par differentiable hai agar wahan ek tangent line ho. Multiple variables mein, differentiability ka matlab hai ki surface ka ek tangent plane ho jo graph ko genuinely hug kare — jab tum zoom in karo toh function linear dikhta hai.
Yahan ek trap hai: partial derivatives hona KAAFI NAHI hai. Ek point par ∂ f / ∂ x aur ∂ f / ∂ y dono exist kar sakte hain, phir bhi function wahan continuous bhi nahi hoga! Sachi differentiability ek stronger condition hai "partials exist" se.
Ek strict hierarchy hai. Har ek neeche wale ko imply karta hai, kabhi ulta nahi.
continuously diff. ( C 1 ) ⇒ differentiable ⇒ partials exist
differentiable ⇒ continuous
Definition Partial derivative
f : R 2 → R ke liye,
f x ( a , b ) = lim h → 0 h f ( a + h , b ) − f ( a , b ) , f y ( a , b ) = lim h → 0 h f ( a , b + h ) − f ( a , b ) .
Partial derivative sirf ek seedhi direction probe karta hai (axis ke saath). Yeh us line se hatke jo kuch bhi hota hai, usse andha hai.
Definition Differentiability (asli definition)
f point a = ( a , b ) par differentiable hai agar ek linear map (gradient ∇ f ( a ) ) exist kare aisa ki
lim h → 0 ∥ h ∥ f ( a + h ) − f ( a ) − ∇ f ( a ) ⋅ h = 0.
Seedhi baat: linear approximation ki error ko distance ∥ h ∥ se tez shrink karna chahiye jab tum har direction se ek saath approach karo.
Hum ek tangent plane L ( x ) = f ( a ) + m ⋅ ( x − a ) chahte hain jo f ko approximate kare. Bacha hua error likhte hain:
E ( h ) = f ( a + h ) − plane [ f ( a ) + m ⋅ h ] .
Tangent plane ke liye hum sirf E → 0 nahi chahte (woh toh sirf continuity hai). Hum chahte hain ki E step size ∥ h ∥ ke mukable negligible ho — ek higher-order error:
E ( h ) = o ( ∥ h ∥ ) ⟺ ∥ h ∥ E ( h ) → 0.
∥ h ∥ se divide kyun karte hain?
Agar tum sirf E → 0 maango, toh koi bhi continuous function "pass" kar leta. ∥ h ∥ se divide karna error ko quadratically-fast maarne ke liye force karta hai. Yehi cheez ise tangent plane banati hai aur sirf koi bhi plane nahi jo point ko touch kare.
Kaun sa m ? x -axis ke saath approach karo, h = ( h , 0 ) . Tab ∥ h ∥ = ∣ h ∣ aur definition force karta hai
∣ h ∣ f ( a + h , b ) − f ( a , b ) − m 1 h → 0 ⇒ m 1 = f x ( a , b ) .
Usi tarah m 2 = f y ( a , b ) . Toh agar f differentiable hai, toh ek hi possible linear map hai ∇ f = ( f x , f y ) .
f ( a + h ) = f ( a ) + ∇ f ( a ) ⋅ h + o ( ∥ h ∥ )
Maano f , a par differentiable hai. Tab
f ( a + h ) − f ( a ) = ∇ f ( a ) ⋅ h + E ( h ) , E = o ( ∥ h ∥ ) .
Jab h → 0 : dot product → 0 (h mein linear hai) aur E → 0 (kyunki E /∥ h ∥ → 0 matlab E → 0 aur bhi tezi se). Isliye f ( a + h ) → f ( a ) . Continuous. ■
Worked example Example 1 — Aasaan tarike se differentiability confirm karo
f ( x , y ) = x 2 y + sin y at ( 1 , 0 ) .
f x = 2 x y , f y = x 2 + cos y . Yeh step kyun? Partials compute karo dusre variable ko constant maanke.
Dono sab jagah continuous hain (continuous functions ke products/sums). Kyun? C 1 ⇒ differentiable — koi limit nahi chahiye.
∇ f ( 1 , 0 ) = ( 0 , 1 + 1 ) = ( 0 , 2 ) . Tangent plane: z = 0 + 0 ( x − 1 ) + 2 ( y − 0 ) = 2 y .
Worked example Example 2 — Partials exist karte hain par differentiable NAHI
f ( x , y ) = ⎩ ⎨ ⎧ x 2 + y 2 x y 0 ( x , y ) = ( 0 , 0 ) ( 0 , 0 )
Origin par partials: y = 0 ke saath, f ( x , 0 ) = 0 , toh f x ( 0 , 0 ) = 0 . Usi tarah f y ( 0 , 0 ) = 0 . Kyun? y = 0 plug karo phir differentiate karo — function axes par identically 0 hai.
Par continuity fail karta hai: y = x ke saath approach karo: f ( x , x ) = 2 x 2 x 2 = 2 1 = 0 = f ( 0 , 0 ) . Yeh kyun khatam karta hai? Differentiable ⇒ continuous; yeh continuous nahi hai, toh differentiable nahi ho sakta — chahe dono partials exist karte ho!
Moral: partials = 0 ek mirage of niceness hai. Diagonal direction sach dikhata hai.
Common mistake Steel-man: "Partials exist ⇒ differentiable"
Sahi kyun lagta hai: 1D mein, "derivative exists" hi differentiability hai — toh hum same expect karte hain. Aur f x , f y "the derivatives" jaisi lagti hain, toh surely unka hona matlab kaam ho gaya.
Galat kyun hai: Partials sirf dono axis directions test karte hain. Ek function x aur y ke saath smooth ho sakta hai phir bhi diagonal ke saath jagged ya discontinuous ho (Example 2). Differentiability har direction se ek saath achhe behaviour ki demand karta hai — ek 2D requirement.
Fix: Ya toh o ( ∥ h ∥ ) limit directly verify karo, ya check karo ki partials continuous hain (C 1 ). C 1 check hi woh hai jo tum 99% time use karoge.
Common mistake "Har direction mein directional derivatives exist karte hain" ko differentiability se confuse karna
Chahe ek point se guzarne wali har line ke saath directional derivatives exist karte hon, f phir bhi differentiable hone mein fail ho sakta hai (linear formula D u f = ∇ f ⋅ u break ho sakta hai). Differentiability strictly stronger hai.
Recall Feynman: 12-saal ke bacche ko samjhao
Ek ulhar-pulhar pahaad imagine karo. Ek jagah par khade hokar, tum slope check karte ho ekdum East chalte hue aur ekdum North chalte hue — woh "partial slopes" hain. Par iska North-East direction mein achanak ek cliff ke baare mein kuch pata nahi chalta! Ek pahaad "smooth" (differentiable) tabhi hai jab, chahe tum kisi bhi direction mein kadam rakho, zameen aise uthe jaise ek flat tilted board tumhare paairon ke neeche rakhi ho. Agar ek bhi diagonal direction tumhe dhoka de, toh pahaad us jagah se secretly toot hua hai — chahe East aur North bilkul theek lage hoon.
"Partials diagonals ke andhe hain; sirf plane sab dekh sakta hai."
Aur hierarchy: C ontinuously-diff → D ifferentiable → C ontinuous → (aur alag se) P artials.
"C ould D ucks C arry P lanes?" — left right ko imply karta hai, akele P ke liye kabhi ulta nahi.
f : R 2 → R ki a par differentiability define karolim h → 0 ∥ h ∥ ∣ f ( a + h ) − f ( a ) − ∇ f ( a ) ⋅ h ∣ = 0 .
"Partials exist" differentiability ke liye kyun kaafi nahi? Partials sirf axis directions test karte hain; function diagonals ke saath discontinuous/jagged ho sakta hai (jaise x y / ( x 2 + y 2 ) ).
Sufficient C 1 condition kya hai? Agar f x , f y exist karte hain aur a ke paas continuous hain, toh f , a par differentiable hai.
Differentiable hona kaun si weaker property imply karta hai? Continuity (aur sab directional derivatives ka exist karna).
Agar f differentiable hai toh linear map kiska equal hona chahiye? Gradient ∇ f = ( f x , f y ) — har axis ke saath approach karke mila.
Definition mein error ko ∥ h ∥ se divide kyun karte hain? Error ko higher-order (o ( ∥ h ∥ ) ) force karne ke liye, taaki woh genuine tangent plane bane na ki sirf koi touching plane.
f ( x , y ) = x 2 + y 2 x y ke liye, f x ( 0 , 0 ) , f y ( 0 , 0 ) kya hain, aur kya f differentiable hai?Dono = 0 , par f continuous bhi nahi hai (y = x ke saath limit 2 1 hai), toh differentiable nahi.
Estimation ke liye linearization formula f ( a + h ) ≈ f ( a ) + ∇ f ( a ) ⋅ h .
Limit definition: error over norm h to 0
Gradient nabla f = fx, fy
Higher-order error o of norm h
Trap: partials alone insufficient