Inner differential dy hai, isliye hum y ke upar pehle integrate karte hain. Us inner step ke dauran, xfrozen rehta hai — bilkul ek fixed number ki tarah treat hota hai (jaise 7).
Concretely inner step yeh hai:
∫14x2ydy=x2[2y2]14=x2⋅216−1=215x2,
jahaan x2 bahar aa gaya kyunki woh y ke respect mein constant hai. Answer: pehle y; x constant.
Kya f(x,y)=x3e2yseparable hai (yaani g(x)h(y) form ka)? Agar haan, toh g aur h batao.
Recall Solution 1.2
Haan. Yeh sirf x ki function aur sirf y ki function ka product hai:
g(x)=x3,h(y)=e2y.
Kyunki yeh separate hota hai, ek rectangle par hum double integral ko do 1-D integrals ke product mein split kar sakte hain (parent shortcut). x3e2xy se compare karo: exponent x aur y ko mix karta hai, isliye woh separable nahi hai.
x ko FREEZE karo, y par FILL karo (inner):
∫02(3x2+2y)dy=[3x2y+y2]02=6x2+4.
Yahaan 3x2, y mein constant hai, isliye 3x2y milta hai; 2y ka antiderivative y2 hai.
Outer x-integral mein FILE karo:∫01(6x2+4)dx=[2x3+4x]01=2+4=6.Answer: 6.
∬RxeydA, R=[1,3]×[0,1] compute karo, separable shortcut use karke, phir confirm karo ki yeh iterated integral ke barabar hai.
Recall Solution 2.2
f=x⋅ey separable hai, isliye
(∫13xdx)(∫01eydy)=[2x2]13⋅[ey]01=29−1⋅(e−1)=4(e−1).Iterate karke confirm karo (inner y par, x frozen):
∫13x(∫01eydy)dx=∫13x(e−1)dx=(e−1)⋅29−1=4(e−1).✓Answer: 4(e−1)≈6.873.
∬RyexydA, R=[0,1]×[0,1] compute karo. Woh order choose karo jo integration by parts se bachaye.
Recall Solution 3.1
Notice karo ki ∂x∂exy=yexy — bilkul wohi integrand hai. Toh pehle x par integrate karna (with y frozen) trivial hai:
∫01yexydx=[exy]x=0x=1=ey−1.y-integral mein FILE karo:∫01(ey−1)dy=[ey−y]01=(e−1)−(1−0)=e−2.
Agar hum pehle y par integrate karte, toh ∫yexydy ke liye integration by parts chahiye hota — same answer, zyada mehnat.
Answer: e−2≈0.718.
∬Rxcos(xy)dA, R=[0,π/2]×[0,1] (yahaan x∈[0,π/2], y∈[0,1]) compute karo. Clean order choose karo.
Recall Solution 3.2
Kyunki ∂y∂sin(xy)=xcos(xy), pehle y par integrate karna (freeze x) directly derivative ko undo karta hai:
∫01xcos(xy)dy=[sin(xy)]y=0y=1=sinx−0=sinx.FILE karo:∫0π/2sinxdx=[−cosx]0π/2=0−(−1)=1.Answer: 1. (Pehle x par integrate karne par parts ki zaroorat padti.)
R=[−1,1]×[−1,1] par z=4−x2−y2 ke neeche ke solid ka volume nikalo. (Figure dekho.)
Recall Solution 4.1
Volume =∬R(4−x2−y2)dA. Sum ko split karo:
∬R4dA−∬Rx2dA−∬Ry2dA.Pehla piece:4⋅area(R)=4⋅(2⋅2)=16.Doosra piece (separable, x2⋅1): (∫−11x2dx)(∫−111dy)=32⋅2=34.Teesra piece symmetry se same hai: 34.V=16−34−34=16−38=340.
Surface R par xy-plane ke upar rehti hai (corners par minimum value: 4−1−1=2>0), isliye yeh ek sach mein positive volume hai — koi cancellation nahi.
Answer: 340≈13.33.
Order dy first (freeze x>0):
∫01(x2+y2)2x2−y2dy=[x2+y2y]01=x2+11.
Phir ∫01x2+11dx=[arctanx]01=4π.
Order dx first: integrand x↔y swap karne par antisymmetric hai (sign flip ho jaata hai). x mein same antiderivative se,
∫01(x2+y2)2x2−y2dx=[x2+y2−x]01=1+y2−1,
phir ∫011+y2−1dy=−4π.
Yahan Fubini humein kyun nahi bachata: integrand corner (0,0) ke paas blow up ho jaata hai; actually ∬R(x2+y2)2x2−y2dA=∞. Fubini require karta hai ki fintegrable ho (closed rectangle par continuous ho, ya ∬∣f∣<∞ ho). Yeh funbounded aur absolutely integrable nahi hai, isliye orders ki equality guarantee nahi hai — aur waakai mein fail hoti hai. Yeh woh textbook example hai jiske baare mein parent ke third mistake callout ne warn kiya tha.
Answer: +4π (order dydx), −4π (order dxdy); Fubini fail hota hai kyunki f, (0,0) ke paas integrable nahi hai.