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[Section 8.2] Area of a surface of revolution

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[Section 8.2] Area of a surface of revolution

1. y = x4 , 0 ≤ x ≤ 1 ⇒ dydx = 4x3 (a) about x-axis:

S = Z

2πy ds = Z 1

0

2πx4p

1 + 16x6dx (b) about y-axis:

S = Z

2πx ds = Z 1

0

2πxp

1 + 16x6dx 

8. y = cos(2x) , 0 ≤ x ≤ π6dydx = −2 sin(2x)

S = Rπ/6

0 2π cos(2x) q

1 + 4 sin2(2x) dx

= R

3/2

0 π√

1 + 4u2du by u = sin(2x)

= Rπ/3 0 π√

1 + tan2θsec22θdθ by u = tan θ2

= π2Rπ/3

0 sec3(θ) dθ

= π2[12(sec θ tan θ + ln | sec θ + tan θ|)]π/30

= π4(2√

3 + ln(2 +√

3)) 

15. x =p

a2− y2, 0 ≤ y ≤ a2dxdy = √−y

a2−y2

S = Ra/2 0 2πp

a2− y2 r

(√−y

a2−y2)2+ 1 dy

= Ra/2 0 2πp

a2− y2q

y2

a2−y2 + 1 dy

= Ra/2 0 2πp

a2− y2a

a2−y2dy

= Ra/2 0 2πa dy

= πa2 

25. S =R

1 2πyp1 + (y0)2dx , y = 1x

S = 2πR 1

1 x

q

1 +x14dx

= 2πR 1

x4+1 x3 dx

> 2πR 1

x4

x3 dx ∀x > 0

= 2πR 1

1

xdx div.

Hence, S diverge. 

1

(2)

29. (a) xa22 +yb22 = 1 , a > b ⇒ dydx = −2xa2/2yb2 = −ab22xy

1 + (dy

dx)2= 1 + b4x2

a4y2 = 1 + b2x2

a2(a2− x2)= a4− (a2− b2)x2 a2(a2− x2)

The ellipsoid’s surface area is twice the area generated by rotating the first-quadrant portion of the ellipse about the x-axis. Thus,

S = 2Ra

0 2πyp1 + [dy/dx]2dx

= 4πRa 0

b a

√a2− x2

a4−(a2−b2)x2 a

a2−x2 dx

= 4πba2

Ra

0 pa4− (a2− b2)x2dx

= 4πba2

R

a2−b2/a 0

√a4− a4u2a2

a2−b2 du let a2u =√

a2− b2x

= 4πa2b

a2−b2

R

a2−b2/a 0

√1 − u2du

= 4πa2b

a2−b2

Rsin−1( a2−b2/a)

0 cos2θ dθ let u = sin θ

= 4πa2b

a2−b2

Rsin−1( a2−b2/a) 0

1+cos(2θ)

2

= 4πa2b

a2−b2[θ2+sin(2θ)4 ]|sin−1 (

a2 −b2 /a)

0 (remind sin(2θ) = 2 sin θ cos θ)

= 2πa2b

a2−b2[sin−1u + u cos(sin−1u)]|

a2 −b2 /a

0 by θ = sin−1u

= 2πa2b

a2−b2[sin−1u + u√ 1 − u2]|

a2 −b2 /a 0

= 2πaa22b

−b2[sin−1(

a2−b2

a ) +

a2−b2

a

q

1 − a2a−b2 2]

= 2π[a2b

a2−b2 sin−1(

a2−b2

a ) + b2] 

(b) Similarly, change a and b, we get

S = 2π[ ab2

√b2− a2sin−1(

√b2− a2

b ) + a2] 

31. S =Rb

a 2π[c − f (x)]p1 + [f0(x)]2dx 

36. g(x) = f (x) + c ⇒ g0(x) = f0(x)

Sg = Rb

a2πg(x)p1 + [g0(x)]2dx

= Rb

a2π[f (x) + c]p1 + [f0(x)]2dx

= Rb

a2πf (x)p1 + [f0(x)]2dx + 2πcRb

ap1 + [f0(x)]2dx

= Sf+ 2πcL 

2

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