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2π(Rπ 0 x sin xdx− R2π π x sin xdx)

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(1)

 } (B) ç‚5t

2003  1 ~ 11 n.

1. IR[ýâ y = 1 + sin x D y − 1 s(Ê x = 0 D x = 2π 5ÈFˇ–, t°

âR÷yWìžF) ñ5ñ . (12%) j: V = 2π{Rπ

0 x[(1+sin x)−1]dx+R

π x[1−(1+sin x)]dx} = 2π(Rπ

0 x sin xdx−

R

π x sin xdx).

Because R x sin xdx = R xd(− cos x) = −x cos x + R cosxdx = −x cos x + sin x + C.

Hence,Rπ

0 x sin xdx = −x cos x + sin x|π0 = π, R

π x sin xdx = −x cos x + sin x|π = −2π − π = −3π.

Therefore, V = 2π[π − (−3π)] = 8π2

2. t°Ö( x = t − sin t, y = 1 − cos t ø‘ (0 ≤ t ≤ 2π) 5Å. (12%) j: Because x = t − sin t, y = 1 − cos t. Hence dxdt = 1 − cos t, dydt = sin t

s = Z

0

q

(1 − cost)2+ sin2tdt

= Z

0

√2 − 2 cos tdt

= Z

0

r 4 sin2 t

2dt

= 2 Z

0

sin t 2dt

= 4(− cos t 2)|0

= 4[1 − (−1)] = 8 3. t°.ì }R e3x

e3x+2e2x+2e+1dx. (12%) j: I u = ex, † x = ln u, dx = duu.

Z e3x

e3x+ 2e2x+ 2ex+ 1dx

=

Z u3

u3+ 2u2+ 2u + 1·du u

=

Z u2

(u + 1)(u2+ u + 1)du

q (u+1)(uu22+u+1) = u+1A +uBu+C2+u+1, † u2= A(u2+ u + 1) + (Bu + C)(u + 1).

I u = −1, ) A = 1, ] −u − 1 = (Bu + C)(u + 1), ¹ Bu + C = −1. Ĥ,

Ÿ =

Z du u + 1−

Z du

u2+ u + 1 1

(2)

= ln |u + 1| −

Z du

(u + 12)2+34

= ln |u + 1| − 1

3 2

tan−1(u +12

3 2

) + C

= ln(ex+ 1) − 2

√3tan−1(2ex+ 1

√3 ) + C

4. t°”Ì limx→0cos 3x cos x

1

x2 5M. (12%) j:

x→0lim(cos 3x cos x)x21

= lim

x→0exp(ln | cos 3x| − ln | cos x|

x2 )

= exp( lim

x→0

−3 sin 3x cos 3x +sin xcos x

2x )

= exp( lim

x→0

−3 tan 3x + tan x

2x )

= exp( lim

x→0

−9 sec23x + sec2x

2 )C = exp[ lim

x→0(sin 3x 3x · −9

2 cos 3x +sin x

x · 1

2 cos x)]

= exp(−9 2+1

2) = exp(−4) = e−4. 5. qp > 1, t°¡ }R

1 (ln x)2

xp dx 5M. (12%) j:

Z (ln x)2 xp dx =

Z

x−p(ln x)2dx

= 1

1 − p Z

(ln x)2dx1−p

= 1

1 − p[x1−p(ln x)2− Z

x1−pd(ln x)2]

= 1

1 − p[x1−p(ln x)2− 2 Z

x−pln xdx]

= (ln x)2

(1 − p)xp−1 − 2 (1 − p)2

Z

ln xdx1−p

= (ln x)2

(1 − p)xp−1 − 2

(1 − p)2[x1−pln x − Z

x1−pd(ln x)]

= (ln x)2

(1 − p)xp−1 − 2 ln x

(1 − p)2xp−1 + 2 (1 − p)2

Z x−pdx

= (ln x)2

(1 − p)xp−1 − 2 ln x

(1 − p)2xp−1 + 2

(1 − p)3xp−1 + C 2

(3)

ÄÑ p > 1, limx→∞(ln x)xp−12 = limx→∞2(p−1)xln xp−1 = limx→∞2(p−1)12xp−1 = 0.

FJ R 1

(ln x)2

xp dx = (1−p)x(ln x)p−12(1−p)2 ln x2xp−1 + (1−p)23xp−1|1 = −(1−p)1 3 =

1 (p−1)3

Y L’Hˆopital ¶† ($) C xα>> (ln x)β (as x → ∞), α, β > 0 ).

6. qa, bÑb, / limx→0(x−3sin 3x + ax−2+ b) = 0, t°a, b 5M. (12%) j: x−3sin 3x + ax−2+ b = sin 3x+ax+bx3

x3 .

I f (x) = sin 3x + ax + bx3, g(x) = x3,

f0(x)

g0(x) = 3 cos 3x+a+3bx2 3x2 f00(x)

g00(x) = −9 sin 3x+6bx

6x = −92·sin 3x3x + b → −92+ b, ç x → 0.

Y L’Hˆopital ¶†, limx→0f (x)

g(x) = limx→0f0(x)

g0(x) = limx→0f00(x)

g00(x) = −92+ b, ]) −92+ b = 0, ¹ b = 92.

¢Ä limx→0fg00(x)(x) = 0, / limx→0g0(x) = 0, ] limx→0f0(x) = 0, 7 f0(x) = 3 cos 3x + a + 3b2→ 3 + a, ç x → 0, ]) 3 + a = 0, ¹ a = −3.

7.

(1) tŸ| tan−1x 5 MacLaurin b£wY¹¸ˇ. (4%) (2) t°bP

n=0 (−1)n

3n(2n+1) 5¸. (8%) j:

(1) tan−x=P n=0

(−1)n

2n+1x2n+1, −1 ≤ x ≤ 1.

(2) I x = 1

3, †

tan−1 1

√3 =

X

n=0

(−1)n 2n + 1· 1

3n · 1

√3,

])

X

n=0

(−1)n

3n(2n + 1) =√

3 tan−1 1

√3 =√ 3 ·π

3 = π√ 3 6 . 8. q f (x) = xq

1−x

1+x, −1 < x < 1.

(a) t° f (x) 5 MacLaurin b. (10%) (b) t° f(n)(0). (6%)

j:

3

(4)

(a)

f (x) = xr 1 − x

1 + x = x(1 − x)

√1 − x2 = (x − x2)(1 − x2)12

= (x − x2)[1 + (−1

2)(−x2) +(−12)(−32)

1 · 2 (−x2)2+ · · · + (−12)(−32) · · · (2n−12 )

n! (−x2n) + · · ·]

= (x − x2)(1 − x2

2 + 1 · 3

22· 2!x4+ · · · +1 · 3 · · · (2n − 1)

2n(n!) x2n+ · · ·)

= x + x3

2 + 1 · 3

22· 2!x5+ · · · + 1 · 3 · · · (2n − 1)

2n(n!) x2n+1+ · · ·

−(x2−x4

2 + 1 · 3

22· 2!x6+ · · · + 1 · 3 · · · (2n − 1)

2n(n!) x2n+2+ · · ·)

= x − x2+x3 2 −x4

2 + · · · +1 · 3 · · · (2n − 1)

2n(n!) x2n−1 · 3 · · · (2n − 1)

2n(n!) x2n+2+ · · ·) (b) I an [ý f (x) 5 MacLaurin b2 xn á5[b, †

an=

( 1·3···(2m−1)

2m(m!) , J n = 2m + 1, m = 0, 1, 2, · · ·

1·3···(2m−1)

2m(m!) , J n = 2m + 2, m = 0, 1, 2, · · · Ä an= f(n)n!(0), ] f(n)(0) = an(n!), Ĥ

f(n)(0) =

( 1·3···(2m−1)

2m(m!) [(2m + 1)!], J n = 2m + 1, m = 0, 1, 2, · · ·

1·3···(2m−1)

2m(m!) [(2m + 2)!], J n = 2m + 2, m = 0, 1, 2, · · ·

4

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