92çB$ø`çü5(-ç‚)
Ch11.Ch14 ¡b. ”è™
1. [a] #8ƒb f (x, y) =
( 2x2y
x4+y2 J (x, y) 6= (0, 0) 0 J (x, y) = (0, 0)
I ϕ(t) = (t, at), ψ(t) = (t, t2), a ÑL<ÝÉ¡b, ½-
?´A ? (i) lim
t→0f (ϕ(t)) = lim
t→0f (ψ(t)), (ii) f Ê (0, 0) ©/. sol.
(i)
limt→0f (ϕ(t)) = lim
t→0
2t2·at
t4+a2t2 = lim
t→0 2at
a2+t2 = 0 limt→0f (ψ(t)) = lim
t→0 2t2·t2
t4+t4 = lim
t→01 = 1 limt→0f (ϕ(t)) 6= lim
t→0f (ψ(t))
(ii) J f Ê (0, 0) ©/, † lim
(x,y)→(0,0
f (x, y) = f (0, 0),
Oâ¤, ú‡H ϕ, ψ
limt→0f (ϕ(t)) = 0 = f (0, 0) = lim
t→0f (ψ(t)) = 1 =⇒
0 = 1, 8e ] f Ê (0, 0) .©/
[b] #8ƒb f (x, y) =
( |x|
y2e−
|x|
y2 J y 6= 0
0 J y = 0
½”Ì lim
(x,y)→(0,0)
f (x, y) æÊ´?
sol.
f (x, y) =
( |x|
y2e−
|x|
y2 J y 6= 0
0 J y = 0
5? ϕ(t) = (t2, t), lim
t→0f (ϕ(t)) = lim
t→0f (t2, t) = limt→0
|t2| t2 e−
|t2|
t2 = lim
t→0e−1 = e−1.
5? ψ(t) = (t3, t), f (ψ(t)) = lim
t→0
|t3| t2 e−
|t3|
t2 ,
Y t > 0, t 6= 0 C t < 0, lim
t→0f (ψ(t)) = lim
t→0±tet = 0.
B¤, lim
t→0f (ϕ(t)) 6= lim
t→0f (ψ(t)), ] lim
(x,y)→(0,0)
f (x, y).
æÊ
2. ø”õÊÆ£ì( (circular helix) −→r (t) «,
−
→r (t) = (a cos ωt, a sin ωt, bωt) [a] ½¤õ5§0 (speed) u´Ñb?
sol.
velocity vector= d−→r (t)dt = (−aω sin ωt, aω cos ωt, bω)
|−→r | = √
a2ω2sin2ωt + a2ω2cos2ωt + b2ω2 speed= |−→r | = √
a2 + b2ω, constant.
[b] °¤”õ5§²¾ (velocity vector) D z W5>i sol.−
→z 5ÀP²¾ −→
k = (0, 0, 1), −→r D −→
k íHiÑ θ,
† cos θ = −→r ·
−
→k
|−→r ||−→
k | = bω
(a2+b2)12ω
= b
(a2+b2)12
,
θ = cos−1
b (a2+b2)12
, ø_b
[c] ‚à (b) C¦( −→r (t) ,íù_Ôyõ, j-½
æ: ²¾ƒb(à−→r (t))?´À‰bõbMƒbf : [a, b] → R 5 Mean Value Theorem ?(cì f x5FbíGß4
”) sol.
J −→r (t) = (a cos ωt, a sin ωt, bωt)ÑW, ¦ t1 = 0, t2 =
2π ω , †
−
→r (t1) = (a, 0, 0), −→r (t2) = (a, 0, 2πb), ⤠−→r (t2) −
−
→r (t1) = (0, 0, 2πb), ¤²¾5j²uòk x, y Þ (²
,, Jb > 0)
J −→r ¥_²¾ƒbé°À‰bõbMƒb5 Mean Value Theorem, † ξ k t1D t2 5ÈU) −→r (t2) − −→r (t1) =
(t2−t1)−→r 0(ξ), ¹(0, 0, 2πb) = 2πω (−aω sin ωξ, aω cos ωξ, bω),
ku sin ωξ = 0, cos ωξ = 0, ¤Ñ.ª?59 ] (c) 5
u´ìí
[d] °Æ£ì( (ÊLSøõ) í0 sol.
”õ5 unit velocity vector= −→
T = |−−→→vv |, JsÑÆ£(5 parameter,
−
→T = d−→r dt /ds
dt = d−→r ds
= d
ds(a cos ωt, a sin ωt, bωt)
= dt ds · d
dt(−aω sin ωt, aω cos ωt, bω)
b²ìdt
ds, 1 = (dt
ds)2 · (a2ω2sin2ωt + a2ω2cos2ωt + b2ω2)
= (dt
ds)2 · (a2 + b2)ω2
dt
ds = √ 1
a2+b2ω, â¤−→
T = √ 1
a2+b2(−a sin ωt, a cos ωt, bω) d−→
T
ds = 1
√a2 + b2 dds(−a sin ωt, a cos ωt, bω)
= 1
√a2 + b2 dtdsdtd (−a sin ωt, a cos ωt, bω)
0K =
d−→ T ds
= √ 1
a2+b2
dt
ds
·√
a2ω2cos2ωt + a2ω2sin2ωt
B¤Æ£ì($ÊLSøõ50Ñ a
a2+b2. 3. Let r(t) = (et − t, 2√
6e2t,√
3t), −1 ≤ t ≤ 1, [a] Find the length of the curve;
sol.
r0(t) = (et − 1,√
6e2t,√ 3),
||r0(t)|| = ((et − 1)2 + (√
6e2t)2 + (√
3)2)12 = (e2t + 4et + 4)12 = et + 2.
L = R1
−1||r0(t)||dt = R 1
−1(ey + 2)dt = e − e−1 + 4.
[b] Find the curvature of r(t) at t = 0;
sol.
r00(t) = (et, 12√
6e2t, 0), r0(0) = (0,√
6,√
3), r00(0) = (1,
√6
2 , 0), r0(0)×r00(0) = (−3
√2 2 ,√
3, −√ 6).
So k(0) = ||r0(0)×r||r0(0)||00(0)||3 = 12.
4. Let r(t) = (t2, − sin t + t cos t, cos t + t sin t), t > 0, find an equation of the osculating plane of the curve r(t) at the point (π2, −π, −1).
sol.
r0(t) = (2t, −t sin t, t cos t),
||r0(t)|| = ((2t)2+ (−t sin t)2+ (t cos t)2)12 = √
5|t| =
√5t (by t > 0).
T(t) = ||rr00(t)(t)|| = √1
5(2, − sin t, cos t), T0(t) = √1
5(0, − cos t, − sin t), ||T0(t)|| = √1
5, N(t) = ||TT00(t)(t)|| = (0, − cos t, − sin t),
B(t) = T(t) × N(t) = √1
5(1, 2 sin t, −2 cos t).
So the osculating plane of the curve r(t) at the point (π2, −π, −1) has normal vector B(π) = √ 1
5(1,0,2), so
an equation is 1(x − π2) + 0(y + π) + 2(z + 1) = 0 or x + 2z = π2 − 2.
5. Let f (x, y, z) =
( xy+yz3
x2+z6 if (x, y, z) 6= (0, 0, 0)
0 if (x, y, z) = (0, 0, 0) , de- termine the set of points at which f is continuous.
sol.
The function f (x, y, z) is continuous for (x, y, z) 6=
(0, 0, 0) since it is equal a rational function there.
For (x, y, z) → (0, 0, 0) along curve r(t) = (kt3, kt3, t), we see that f (x, y, z) = f (kt3, kt3, t) = (kt3)2+kt3t3
(kt3)2+t6 =
(k2+k) k2+1 .
So f (x, y, z) → (k2+k)
k2+1 as (x, y, z) → (0, 0, 0) along r(t) = (kt3, kt3, t).
Therefore, different path leads to different limit val- ues, hence the limit of f (x, y, z) at (0, 0, 0) dose not exist, so f (x, y, z) is not continuous at (0, 0, 0).
Ch15 Rûb
6. 163 (x3+y2)+xyz2+8z = 0. °ÊÞ, (−1, −1, 0)øõ
5 zx, zy, zxx, zxy £¬¤õ5~Þ(CÉ°zx, zxx, zxy£
~Þ) sol.
zx:
16x2 + yz2 + 2xyzzx + 8zx = 0 16 + 8zx = 0,∴ zx = −2
zy:
16
3 2y + xz2 + 2xyzzy + 8zy = 0
32
3 = 8zy ∴ zy = 43
~Þ:
p(x + 1) + q(y + 1) + (−1) · z = 0
−2(x + 1) + 43(y + 1) − z = 0 zxx :
32x + 2yzzx + 2yzzx + 2xyzx2 + 2xyzzxx+ 8zxx = 0 32x + 2xyzx2 + 8zxx = 0
−32 + 2(4) + 8zxx = 0
−24 + 8zxx = 0
∴ zxx = 3 zxy:
z2 + 2yzzy + 2xzzx + 2xyzyzx + 2xyzzxy + 8xy = 0 2zyzx + 8zxy = 0
∴ zxy = −z4xzy = −14(−2)(43) = 23.
7. ° zx, zy, ~Þ, 1°(−109 , −1110) FÊ5z5,lM
sol.
z = 0 + −2(0.1) + 43(−0.1)
= −0.2 − 304
= −102 − 304 = −1030 = −13.
8. Find the absolute maximum and minimum values of
f (x, y) = 4x + 6y − x2 − y2 in x2 + y2 ≤ 1.
sol.
At a critical point, fx = 4 − 2x = 0, fy = 6 − 2y = 0 =⇒ x = 2, y = 3. So there are no critical points in x2+y2 < 1. Need only look at boundary x2+y2 = 1.
method 1
Use x = cos θ, y = sin θ g(θ) = 4 cos θ + 6 sin θ − 1
g0(θ) = −4 sin θ + 6 cos θ = 0 if tan θ = 32
=⇒ sec2θ = 1 + tan2θ = 1 + 94 = 134
=⇒ cos2θ = 134 , sin2θ = 1 − cos2θ = 139 . So 2 possibilities, (√2
13, √3
13),(−√2
13, −√3
13). The first gives
√26
13 − 1 = 2√
13 − 1 ←− maximum.
The second gives −2√
13 − 1 ←− minimum.
method 2.
Lagrange multipliers:
4 − 2x = 2λx (1)
6 − 2y = 2λy (2)
x2 + y2 = 1 (3)
(1),(2)=⇒ 2(1 + λ)x = 4, 2(1 + λ)y = 6 =⇒
3(1 + λ)x = 2(1 + λ)y =⇒ x = 23y. Then (3)=⇒
4
9y2 + y2 = 1 =⇒ y2 = 139 =⇒ y = ±√3
13. So get (√2
13, √3
13) or (−√2
13, −√3
13). Finish as in method 1.
9. Find the maximum value of f (x, y, z) = xy + xz + yz subject to the constraints x ≥ 0, y ≥ 0, z ≥ 0 and x + y + z = 1.
sol.
If the maximum occurs in the interior of the set, then the equation y + z = λ, x + z = λ, x + y = λ, x + y + z = 1 must hold for some λ. Then
y + z = x + z =⇒ x = y x + z = x + y =⇒ y = z So x = y = z = 13 =⇒ f (x, y, z) = 39 = 13.
The other possibility is that the maximum occurs where one of x, y, z is 0.
Suppose x = 0. Then y + z = 1 and f (0, y, z) = yz = y(1 − y). The maximum of this in 0 ≤ y ≤ 1 is 14. Similarly, if y = 0 or z = 0 we get a maximum of 14. Hence the maximum value must be 13.
10. The plane 2x + y + z = 10 intersects the paraboloid z = x2 + y2 in an ellipse. Find the highest point on the ellipse.
sol.
We want to maximize f (x, y, z) = z subject to x2 + y2 − z = 0, 2x + y + z − 10 = 0.
By the method of Lagrange multipliers, we get
0 = λ2x + 2µ (1)
0 = λ2y + µ (2)
1 = −λ + µ (3)
x2 + y2 − z = 0 (4)
2x + y + z − 10 = 0 (5) (1),(2)=⇒ λx = 2λy =⇒ λ = 0 or x = 2y.
If λ = 0, then (1) =⇒ µ = 0 which contradicts (3).
So x = 2y. Then (4)=⇒ z = x2 + y2 = 5y2.
(5)=⇒ 4y + y + 5y2− 10 = 0 =⇒ y2+ y − 2 = 0 =⇒
(y + 2)(y − 1) = 0 =⇒ y = −2, 1.
y = −2 =⇒ (x, y, z) = (−4, −2, 20) ←− highest point.
y = 1 =⇒ (x, y, z) = (2, 1, 5) ←− lowest point.
11. Show that the ellipsoid 3x2 + 2y2 + z2 = 9 and the sphere x2 + y2 + z2 − 8x − 6y − 8z + 24 = 0 are tangent to each other at he point (1, 1, 2).
sol.
Let f (x, y) = 3x2 + 2y2 + z2 − 9 and g(x) = 3x2 + 2y2+ z2− 9. Then f (1, 1, 2) = g(1, 1, 2) = 0 and the ellipsoid and the sphere are the level surfaces of f and g. Thus ∇f (1, 1, 2) and ∇g(1, 1, 2) are orthogonal to the ellipsoid and the sphere (1, 1, 2).
∇f (x, y, z) = h6x, 4y, 2zi and ∇g(x, y, z) = h2x −
8, 2y − 6, 2z − 8i. Hence ∇f (1, 1, 2) = h6, 4, 4i is parallel ∇g(1, 1, 2) = h−6, −4, −4i. This implies that the ellipsoid 3x2 + 2y2 + z2 = 9 and the sphere x2+ y2+ z2 − 8x − 6y − 8z + 24 = 0 are tengent to each other at he point (1, 1, 2).
12. If f (x, y) = 0 define y as a function of x, show that d2y
dx2 = fxxfy2 − 2fxyfxfy + fyyfx2 fy3
sol.
Differentiate f (x, y) = 0 w.r.t x. We have fx + fydy
dx = 0 (1)
Hence if fy 6= 0, dydx = −ff x
y . Differentiate (1) w.r.t x.
We have
fxx + fxydy
dx + fyxdy
dx + fyy(dy
dx)2 + fyd2y dx2 = 0 We assume that fxy and fyx are both continuous, and hence fxy = fyx. Also, from the equation (1), we have
fxx + fxy−fx
fy + fyx−fx
fy + fyy(−fx
fy )2 + fyd2y dx2 = 0 Thus
d2y
dx2 = fxxfy2 − 2fxyfxfy + fyyfx2 fy3
13. Let f (x, y) = x2(x2+ y2)−12esin(x2y) if (x, y) 6= (0, 0) and f (0, 0) = 0.
(1) Let −→u = hcos θ, sin θi and find D−→uf (0, 0).
(2) Prove that f is continuous at (0, 0).
sol.
D−→uf (0, 0) = lim
h→0
f (h cos θ, h sin θ) − f (0, 0) h
= lim
h→0
h(cos θ)2esin(h3cos2θ sin θ)
h = (cos θ)2
|x2(x2 + y2)−12esin(x2y)| ≤ |x|e1. Since lim
(x,y)→(0,0)
|x| = 0, it follows that lim
(x,y)→(0,0)
f (x, y) = 0 = f (0, 0).
Ch16 ½ }
14. D = {(x, y)|x2+y2 ≤ 4}, t°RR
D
p4 − x2 − y2dA.
sol.
I u = 4 − r2
Ÿ =
Z 2π 0
Z 2 0
p4 − r2rdrdθ
= 1 2
Z 2π 0
Z 4 0
√ududθ
= 1 2
Z π2
0
2 3u32
4
0
dθ
= 8 3
Z 2π 0
dθ = 16 3 π 15. °R1
0
R1
x cos(y2)dydx.
sol.
‰² }ßå,
Ÿ = Z 1
0
Z 4 0
cos y2dxdy
= Z 1
0
y cos y2dy
= sin y2 2
1
0
= sin 1 2 16. °R1
0
R1 0
√ xy
x2+y2+1dydx.
sol.
I u = x2 + y2 + 1
Ÿ = Z 1
0
1 2x
Z 2+x2 1+x2
√du udx
= Z 1
0
x 2
√
2 + x2dx − Z 1
0
x 2
√
1 + x2dx
= 1
3(2 + x2)32
1
0
− 1
3(1 + x2)32
1
0
= 1 3[3√
3 − 2√
2 − 2√
2 + 1]
= 1 3[3√
3 − 4√
2 + 1]
17. t° R1 0
R1
√y yex2
x3 dxdy sol.
x = √
y =⇒ y = x2
Ÿ = Z 1
0
Z x2 0
yex2
x3 dydx
= Z 1
0
x4ex2 2x3 dx
= 1 2
Z 1 0
xex2dx
= 1 4ex2
1
0
= 1
4(e − 1) 18. (a) t° RR
D 1
(x2+y2)n2dA, n Ñcb. D : {(x, y), a ≤ px2 + y2 ≤ b}
sol.
Ÿ =
Z 2π 0
Z b a
1
rnrdrdθ
= 2π Z b
a
1 rn−1dr (b) ç a −→ 0+, t°nMU }í”ÌæÊ
sol.
(ÿ )
19. t°Þ z = p
x2 + y2 D6Þ x2 + y2 = 2x £ xy
ÞFˇ5ñ
sol.
(x − 1)2 + y2 = 1, r = 2 cos θ
Ÿ = Z π2
−π2
Z 2 cos θ 0
rrdrdθ
= 2 Z π2
0
Z 2 cos θ 0
r2drdθ
20. ρ(x, y) = xy2, D = {(r, θ), 0 ≤ r ≤ a, 0 ≤ θ ≤ π2},
t°Dí”-
sol.
(ÿ )
21. Consider the iterated integralR8 0
R 2 y13
√1 + x4dx dy.
Sketch the region of integration and then evaluate it by reversing the order of integration.
sol.
R2
0 dxRx3
0 dy√
1 + x4 = R2
0 x3√
1 + x4dx = 23 · 14(1 + x4)32
2 0
=
1
6{1732 − 1}
22. Consider the iterated integralR2 0
R 4
y2 y sin(x2)dx dy.
Sketch the region of integration and then evaluate it by reversing the order of integration.
sol.
R4 0 dxR
√x
0 dyy sin(x2) = R4 0
x
2 sin(x2)dx = 1212(− cos(x2))|40 =
1
4(1 − cos 16)
23. By making an appropriate change of variables to evaluate the integral RR
R
dA
1+9x2+9y2, where R is the region bounded by the ellipse 9x2 + 9y2 = 4.
sol.
x = r cos θ, y = r sin θ R2π
0 dθR 23
0 dr r
1+9r2 = 2πln(1+9r18 2)
2 3
0 = π9 ln 5