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V =<br />

<br />

2π 2π r<br />

s(s cos φ + a) dr dφ dθ<br />

0 0 0<br />

r 2π<br />

= 2πa (s<br />

0 0<br />

2 cos φ + as) dφ ds = 4π 2 r<br />

a s dr = 2π<br />

0<br />

2 ar 2 .<br />

C πr2 <br />

2πa V = 2π2ar2 <br />

<br />

<br />

<br />

I = cos(x + y)e x−y dxdy<br />

D<br />

<br />

D = {(x, y) ∈ R 2 : |x + y| ≤ π<br />

, |x − y| ≤ 1}.<br />

2<br />

u = x+y v = x−y x = (u+v)/2 y = (u−v)/2 <br />

−1/2 1/2 <br />

<br />

I = 1<br />

1 π/2<br />

cos u e<br />

2 −1 −π/2<br />

v du dv = e − e −1 = 2 sinh(1).<br />

<br />

<br />

1 + y<br />

I =<br />

x dx dy,<br />

D 1 − y<br />

D <br />

y 4 + x 2 − 2x = 0<br />

1 − y 4 = (x − 1) 2 (1 − y)(1 + y)(1 + y 2 ) = (x − 1) 2<br />

−1 ≤ y ≤ 1 1 − 1 − y4 < x < 1 + 1 − y4 <br />

1 <br />

√<br />

1+ 1−y4 1 <br />

√<br />

1+ 1−y4 1 + y<br />

I =<br />

x dx dy =<br />

1 − y<br />

= 1<br />

2<br />

= 2<br />

= 4<br />

−1 1− √ 1−y4 1<br />

−1<br />

1<br />

−1<br />

1<br />

0<br />

−1<br />

1− √ 1−y 4<br />

<br />

1 + y<br />

x dx dy<br />

1 − y<br />

<br />

1 + y<br />

1 − y ((1 + 1 − y4 ) 2 − (1 − 1 − y4 ) 2 <br />

1 1 + y <br />

) dy = 2<br />

1 − y4 dy<br />

−1 1 − y<br />

(1 + y) 1 + y2 1 <br />

<br />

dy = 2 1 + y2 dy − 2 y 1 + y2 dy<br />

−1<br />

1 + y 2 dy = 2( √ 2 + arc sinh(1)) = 2( √ 2 + log(1 + √ 2))<br />

|(x, y)| −p B = B(0, 1) ⊆ R 2 <br />

p < 2 R 2 \ B(0, 1) p > 2 |(x, y, z)| −p <br />

B(0, 1) ⊆ R 3 p < 3 R 3 \ B(0, 1) p > 3<br />

p = 2 <br />

<br />

|(x, y)|<br />

B<br />

−p 2π 1 1<br />

dx dy =<br />

ρ dρ dθ = 2π<br />

0 0 ρp p < 2 p = 2 <br />

2π<br />

0<br />

1<br />

ρ = 2π[log ρ]10 = +∞,<br />

B(0, 1) ⊆ R2 p < 2<br />

1<br />

1<br />

0<br />

ρ 1−p dρ = 2π<br />

(2 − p) [ρ2−p ] ρ=1<br />

ρ=0 ,

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