Neeche, fx jaisa partial derivative ka matlab hai "f ko differentiate karo aur y ko frozen constant maano, dekho f kaise change hota hai jab sirf x move kare." fxy ka matlab hai "pehle x se differentiate karo, phir y se." Hum har ek explicitly banate hain.
HUM KYA karte hain:D=fxxfyy−(fxy)2 mein plug in karo.
D=(4)(9)−02=36>0.fxx kyun check karein:D>0 kehta hai "extremum hai", lekin kaun sa nahi. fxx=4>0 ka sign kehta hai surface upar ki taraf muskurati hai.
Verdict: local minimum.
Recall Solution 1.2
D=(−2)(−5)−(1)2=10−1=9>0.
Dono diagonal entries negative hain, aur waqai D>0 unhe same sign share karne par majboor karta hai. fxx=−2<0 → surface jhukti hai.
Verdict: local maximum.
Recall Solution 1.3
D=(3)(1)−(4)2=3−16=−13<0.Kyun ruk jaate hain:D<0 akele hi settle kar deta hai — fxx dekhne ki zarurat nahi. Geometrically cross-term fxy=4 itna bada hai ki bowl ko Pringle mein tilt kar deta hai.
Verdict: saddle point.
Ab tum khud critical point aur derivatives dhundhte ho.
Recall Solution 2.1
Step 1 — dhundho jahan zameen flat hai. KYU: test sirf ∇f=0 par apply hota hai.
fx=2x−2=0⇒x=1,fy=8y+8=0⇒y=−1.
Critical point: (1,−1).
Step 2 — second derivatives (yahan sab constants hain):
fxx=2,fyy=8,fxy=0.Step 3 — discriminant:D=(2)(8)−02=16>0,fxx=2>0.Verdict:(1,−1) par local minimum.
Recall Solution 2.2
Step 1:fx=2x−y=0,fy=−x+2y−3=0.
Pehli equation se, y=2x. Doosri mein substitute karo: −x+2(2x)−3=0⇒3x=3⇒x=1, toh y=2.
Critical point: (1,2).
Step 2:fxx=2,fyy=2,fxy=−1.
Step 3:D=(2)(2)−(−1)2=4−1=3>0,fxx=2>0.Verdict:(1,2) par local minimum.
Recall Solution 2.3
Step 1:fx=y=0 aur fy=x=0 → sirf ek critical point (0,0).
Step 2:fxx=0,fyy=0,fxy=1.
Step 3:D=(0)(0)−(1)2=−1<0.Verdict:(0,0) par saddle point. Figure dekho: y=x ke saath xy product chadhta hai, y=−x ke saath girta hai — saddle ki pehchaan.
Step 1:fx=2x+ky, fy=kx+2y; dono (0,0) par zero hote hain, toh yeh har k ke liye critical hai.
Step 2:fxx=2,fyy=2,fxy=k.
Step 3:D=(2)(2)−k2=4−k2.
Saddle ke liye D<0 chahiye: 4−k2<0⇒k2>4⇒∣k∣>2.
Verdict:k>2 ya k<−2 par saddle. (k=±2 par, D=0: inconclusive. ∣k∣<2 par: minimum.)
Test ko underlying Taylor / quadratic-form ideas ke saath combine karo.
Recall Solution 4.1
Taylor ka picture. Ek point (a,b) ke paas, u=x−a,v=y−b ke saath second order tak expand karo:
f(a+u,b+v)≈f(a,b)+linearfxu+fyv+21(fxxu2+2fxyuv+fyyv2).
Test sirf quadratic part se shape padhta hai. Yeh tabhi valid hai jab linear part zero ho — yaani fx=fy=0. Warna linear term fxu+fyv chhote u,v ke liye dominant hota hai (woh quadratic ko point ke paas beat karta hai), toh surface tilted hai, aur "min/max/saddle" sahi sawaal bhi nahi hai — sirf ek slope hai.
(1,0) par f=x2+y2 ke liye:fx=2x=2=0. Gradient nonzero hai; surface bas x mein upar ki taraf slope karti hai. Andhaa dhundh D=fxxfyy−fxy2=4>0 compute karna aur "minimum" declare karna meaningless hai — (1,0) bowl ke neeche nahi, side par hai. Pehle hamesha ∇f=0 solve karo.
Recall Solution 4.2
(a) Direct:D=fxxfyy−fxy2=(3)(3)−(1)2=9−1=8.
(b) Eigenvaluesdet(H−λI)=0 solve karte hain:
det(3−λ113−λ)=(3−λ)2−1=0⇒3−λ=±1⇒λ=2 or 4.
Product: λ1λ2=2×4=8=D. ✓
Geometry: dono eigenvalues positive hain → surface dono principal axes ke saath upar curve karti hai → positive definite → local minimum. Eigenvalues 2 aur 4 bowl ke do principal directions mein curvatures hain.
Recall Solution 4.3
HUM KYA chahiye:(2,−1) par critical point, neeche ki taraf curvature, koi cross-term nahi. Ek shifted downward paraboloid kaam karega:
f(x,y)=−3(x−2)2−2(y+1)2.Critical point check karo:fx=−6(x−2)=0⇒x=2; fy=−4(y+1)=0⇒y=−1. ✓
Derivatives check karo:fxx=−6 ✓, fyy=−4, fxy=0 ✓.
Test:D=(−6)(−4)−02=24>0 aur fxx=−6<0 → local maximum. ✓ Construction successful.
Hard edge cases: D=0, aur poore multi-point landscapes.
Recall Solution 5.1
Step 1:fx=4x3=0, fy=4y3=0 → (0,0) par critical hai.
Step 2:fxx=12x2, fyy=12y2, fxy=0. (0,0) par: fxx=0, fyy=0, fxy=0.
Step 3:D=(0)(0)−02=0 → inconclusive. Quadratic Taylor part bilkul flat hai, toh second-order info kuch nahi batati.
Haath se:f(x,y)=x4+y4≥0 sab (x,y) ke liye, equality sirf (0,0) par (dono fourth powers ≥0 hain). Toh f(0,0)=0 woh sabse chhoti value hai jo f kahi bhi leta hai → global (hence local) minimum. Curvature quartic hai, quadratic nahi, yehi exact reason hai ki second-derivative test ise nahi dekh sakta.
Recall Solution 5.2
Step 1:fx=3x2=0⇒x=0; fy=0 sab y ke liye. Toh poori linex=0 critical hai! (0,0) par focus karo.
Step 2:fxx=6x, fyy=0, fxy=0. (0,0) par: sab zero.
Step 3:D=0 → inconclusive.
Haath se:+x mein move karo, f=x3>0; −x mein move karo, f=x3<0. Toh f ek taraf badhta hai aur doosri taraf ghatta hai usi axis ke saath — jaise y=x3 ka inflection point ek surface mein lift ho gaya. Yeh strict min nahi hai (neeche values exist karti hain), strict max bhi nahi (upar values exist karti hain). y mein move karte waqt, f flat rehta hai. Yeh ek degenerate inflection ridge hai, genuine saddle nahi (saddle ko opposite signs ki curvature chahiye; yahan x-behaviour cubic hai, quadratic nahi). Yahi exact "D=0 = haath se investigate karo" case hai.
Recall Solution 5.3
Step 1 — critical points:fx=4x3−4x=4x(x2−1)=0⇒x=0,1,−1. Aur fy=2y=0⇒y=0.
Teen critical points: (−1,0),(0,0),(1,0).
Step 2 — derivatives:fxx=12x2−4, fyy=2, fxy=0. Toh D=(12x2−4)(2).
(0,0) par:fxx=−4, D=(−4)(2)=−8<0 → saddle point.
(1,0) par:fxx=12−4=8, D=(8)(2)=16>0, fxx>0 → local minimum.
(−1,0) par:fxx=8, D=16>0, fxx>0 → local minimum.
Shape: ek "double well" — do valleys (±1,0) par jo origin ke upar ek saddle ridge se separated hain (classic x4−2x2 double-well profile, y2 bowl se lift kiya gaya).