} (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÷yWìF) ñ5ñ . (12%) j: V = 2π{Rπ
0 x[(1+sin x)−1]dx+R2π
π x[1−(1+sin x)]dx} = 2π(Rπ
0 x sin xdx−
R2π
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, R2π
π x sin xdx = −x cos x + sin x|2ππ = −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 2π
0
q
(1 − cost)2+ sin2tdt
= Z 2π
0
√2 − 2 cos tdt
= Z 2π
0
r 4 sin2 t
2dt
= 2 Z 2π
0
sin t 2dt
= 4(− cos t 2)|2π0
= 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
= 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
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
(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