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(1)

1082 ®201-10íÊ!D01-02í-KëLsãÊU–

1. (15 pts) Consider the function

f(x, y) =⎧⎪⎪

⎨⎪⎪⎩

x2+ y2

4 ⋅ ln(x2+ y2) ,if (x, y) ≠ (0, 0), 0 ,if (x, y) = (0, 0).

(a) (3 pts) Is f(x, y) continuous at (0, 0)?

(b) (4 pts) Find fx(0, 0), fy(0, 0), and fx(x, y), fy(x, y) for (x, y) ≠ (0, 0).

(c) (4 pts) Find fxy(0, 0) and fxy(x, y) for (x, y) ≠ (0, 0).

(d) (4 pts) Is fxy(x, y) continuous at (0, 0)?

Solution:

(a) Set x= r cos θ and r sin θ. Then lim

(x,y)→(0,0)

x2+ y2

4 ln(x2+ y2) = lim

r→0+

r2

4 ln(r2) = 1 2 lim

r→0+r2ln r=1 2 lim

r→0+

ln r r−2

= 1 2 lim

r→0+

r1

−2 r−3 =1 2 lim

r→0+

r2

−2 =0= f(0, 0).

Therefore, f(x, y) is continuous at (0, 0).

f(0, 0) = 0 (1%), Computation of the limit (2%).

(b) For (x, y) ≠ (0, 0), fx(x, y) = x

2 ⋅ ln(x2+ y2) +x2+ y2

4 ⋅ 1

x2+ y2 ⋅ 2x = x

2(ln(x2+ y2) + 1). (1%) fy(x, y) = y

2 ⋅ ln(x2+ y2) +x2+ y2

4 ⋅ 1

x2+ y2 ⋅ 2y = y

2(ln(x2+ y2) + 1). (1%)

fx(0, 0) = lim

h→0

f(h, 0) − f(0, 0)

h = lim

h→0

h2 4 ln h2

h = 1

4lim

h→0h⋅ ln h2

= 1 2lim

h→0

ln∣h∣

h−1 =1 2lim

h→0

h−1

−h−2 =1 2lim

h→0−h = 0 (1%) fy(0, 0) = lim

h→0

f(0, h) − f(0, 0)

h = lim

h→0

h2 4 ln h2

h = 0 (1%).

(c) For (x, y) ≠ (0, 0),

fxy(x, y) = x 2 ⋅ 2y

x2+ y2 = xy

x2+ y2. (2%)

fxy(0, 0) = lim

h→0

fx(0, h) − fx(0, 0)

h = lim

h→0

0

2(ln(h2) + 1) − 0

h = 0 (2%)

(2)

(d) Solution 1.

Set x= r cos θ and r sin θ. Then lim

(x,y)→(0,0)fxy(x, y) = lim

r→0+

r2cos θ sin θ r2 = lim

r→0+cos θ sin θ. (2%)

For different θ, the limit value is different. So the limit does not exist. (1%) Therefore, fxy(x, y) is not continuous at (0, 0). (1%)

Solution 2.

First, let’s approach (0, 0) along the y = x. Then y = x gives fxy(x, x) = 1/2 for all x ≠ 0, so fxy(x, y) → 1/2 as (x, y) → (0, 0) along the line y = x. (1%)

Next, we approach (0, 0) along the y = −x. Then y = −x gives fxy(x, −x) = −1/2 for all x≠ 0, so fxy(x, y) → −1/2 as (x, y) → (0, 0) along the line y = −x. (1%)

So lim

(x,y)→(0,0)fxy(x, y) does not exist. (1%)

Therefore, fxy(x, y) is not continuous at (0, 0). (1%)

(3)

2. (8 pts) f(x, y) is a differentiable function on R2. Consider two points P0 = (x0, y0) ≠ P1 = (x1, y1) and define a function g(t) = f(x0+ t(x1− x0), y0+ t(y1− y0)).

(a) (2 pts) Compute g(t) by the chain rule.

(b) (6 pts) Suppose that f(x0, y0) = f(x1, y1) and ∇f ≠ ⃗0. Prove that the line segment P0P1 is tangent to at least one level curve f(x, y) = c for some c.

Solution:

(a) Define g(t) = f(x0+ t(x1− x0), y0+ t(y1− y0)). Then (1%) g(t) = fx(x0+ t(x1− x0), y0+ t(y1− y0)) xt

+ fy(x0+ t(x1− x0), y0+ t(y1− y0)) yt

(1%) = fx(x0+ t(x1− x0), y0+ t(y1− y0)) (x1− x0) + fy(x0+ t(x1− x0), y0+ t(y1− y0)) (y1− y0) (b) P0≠ P1 and f(x0, y0) = f(x1, y1) ⇒

(2%) g(0) = f(x0, y0) = f(x1, y1) = g(1) ⇒

There exists a 0≤ t≤ 1 such that g(t) = g(1) − g(0) 1− 0 = 0 (2%) There exists a point P(x0+ t(x1− x0), y0+ t(y1− y0))

lying on P0P1 with f(x, y) = c = g(t)

(1%) At this point P, ∇f ⋅ (x1− x0, y1− y0) = g(t) = 0 (1%) ⇒ P0P1 tangent to the level curve f(x, y) = c = g(t)

(4)

3. (10 pts) Let C be the hyperbola formed by the intersection of the cone x2+3z2= 4y2 and the plane 2x+ y = 5. Find the maximum and the minimum distance between the origin and the point on C (if exist) by the method of Lagrange multipliers.

Solution:

Let f(x, y, z) = x2+y2+z2, g(x, y, z) = x2−4y2+3z2, h(x, y, z) = 2x+y. We want to find extreme values of f under constraints g= 0 and h = 5. By the method of Lagrange multiplizers, we solve the system of equations:

⎧⎪⎪⎪⎪

⎪⎪⎪⎪⎪

⎪⎨⎪⎪⎪⎪⎪

⎪⎪⎪⎪⎪

fx= λgx+ µhx fy= λgy+ µhy fz= λgz+ µhz g= 0

h= 5

⎧⎪⎪⎪⎪

⎪⎪⎪⎪⎪

⎪⎨⎪⎪⎪⎪⎪

⎪⎪⎪⎪⎪

2x= λ2x + 2µ⋯ ⋅ 1O 2y= −λ8y + µ⋯⋯ 2O 2z= λ6z⋯⋯ 3O

x2− 4y2+ 3z2= 0⋯⋯ 4O 2x+ y = 5⋯⋯ 5O

(3pts for correct setting and equations.) O3⇒ λ = 1

3 or z= 0.

Case 1: z= 0, 4O⇒ x = ±2y. If x = 2y, 5O⇒ y = 1, x = 2 ⇒ λ = 0, µ = 2.

There is one solution (x, y, z) = (2, 1, 0), (λ, µ) = (0, 2).

If x= −2y 5O⇒ y = −5

3, x= 10

3 ⇒ λ = −2

3, µ= 50 9 . There is another solution (x, y, z) = (10

3 ,−5

3 , 0), (λ, µ) = (−2 3 ,50

9 ). 2pts.

Case 2: λ=1

3 but z≠ 0, 1O⇒ x = 3

2µ, 2O⇒ y = 3 14µ However, 4O⇒ (3

2µ)2− ( 3

14µ)2+ 3z2= 0

⇒ 3z2 = − (9 4− ( 3

14)2) µ2< 0 . . . (→←) 2pts.

Hence the only solutions are (x, y, z) = (2, 1, 0), (x, y, z) = (10 3 ,−5

3, 0)

∵f(2, 1, 0) = 5 < f(10 3 ,−5

3, 0) = 125

9 ∴f obtains minimum value at (2, 1, 0). 1pt i.e the minimum distance between (0, 0, 0) and C is √

5. 1pt

The C is unbounded and the maximum distance doesn’t exist. 1pt Sol 2:

⎧⎪⎪⎨⎪⎪

x2+ 3z2 = 4y2

2x+ y = 5 ⇒ Let x = t, y = 5 − 2x = 5 − 2t, 3z2 = 4y2− x2 = 4(5 − 2t)2− t2 x2+ y2+ z2 = t2+ (5 − 2t)2+4

3(5 − 2t)2−1

3t2= f(t).

Find t such that f(t) is minimized.

(5)

4. (12 pts) Find the center of mass of a lamina

D= {(x, y) ∈ R2∣x ≥ 0, y ≥ 0, x2+ 9y2 ≤ 1}

whose density function at any point is proportional to the square of its distance from the y-axis.

Solution:

The density function is ρ(x, y) = x2(1 point). Let x= r cos θ and y = r

3sin θ where 0≤ r ≤ 1 and 0≤ θ ≤ π

2(1 point). Thus

∂(x, y)

∂(r, θ) =RRRRRRRRRRRR

cos θ −r sin θ 1

3sin θ 1

3r cos θ RRRRRRRRRRRR= r

3.(1 points)

m = ∬Dρ(x, y)dA = ∬Dx2dA

= ∫0π/201r2cos2θr 3drdθ

= 1

3[∫0π/2cos2θdθ][∫01r3dr]

= 1 3⋅ π

4 ⋅ 1 4= π

48(2 points).

m ¯X = ∬Dxρ(x, y)dA

= ∬Dx3dA(1 point)

= ∫0π/201 1

3r4cos3θdrdθ

= 1

3⋅ [∫0π/2cos3θdθ][∫01r4dr]

= 1

3[∫0π/2(1 − sin2θ)d(sin θ)] ⋅ [1 5]

= 2

45(2 points).

m ¯Y = ∬Dyρ(x, y)dA

= ∬Dx2ydA(1 point)

= 1 9 ∫

π/2

001r4cos2θ sin θdrdθ

= 1

9[∫0π/2cos2θd(− cos θ)][∫01r4dr]

= 1 9⋅ [−1

3 cos3θ∣π/20 ] ⋅1 5

= 1

135(2 points).

Then the center of mass is ( ¯X, ¯Y) = ( 32 15π, 16

45π)(1 point).

(6)

5. (10 pts) Evaluate the integral

U 1

x2+ y2+ z2dV where U = {(x, y, z) ∈ R3 ∶ x2+ y2+ z2≤ 36 and z ≥ 3}.

Solution:

Use spherical coordinate, z ≥ 3 can be expressed as ρ cos φ ≥ 3. We can obtain ρ ≥ 3 sec φ. The bound for ρ is given by 3 sec φ ≤ ρ ≤ 6. Consider the φ value when the upper bound and the lower bound meet, we have sec φ= 2, φ = π

3. The region is rotationally symmetric with respect to z axis, we have 0≤ θ ≤ 2π.

The integral can be expressed in spherical coordinates.

U 1

x2+ y2+ z2dV = ∫0

π 3

03 sec φ6 1

ρ2 ⋅ ρ2sin φdρdφdθ= 2π ⋅ ∫

π 3

0

ρ sin φ∣63 sec φ

= 2π ∫

π 3

0 sin φ(6 − 3 sec φ)dφ = 6π ∫

π 3

0 2 sin φ− tan φdφ

= 6π(−2 cos φ + ln cos φ)0π3 = 6π[(−1 − ln 2) + 2] = 6π lne 2. Grading policies:

ˆ Knowing the formula dV = ρ2sin φdρdφdθ for spherical coordinates. No partial credit is allowed for this part. 3pts.

ˆ Writing the domain in spherical coordinates. 4pts – Correct upper bound for ρ. 1pt

– Correct lower bound for ρ. 1pt

– Correct upper and lower bound for φ. 1pt – Correct upper and lower bound for θ. 1pt

ˆ Evaluating the integral. Partial credits is allowed in this part.3pts

It is possible to use cylindrical coordinate. The equation would be like this

U 1

x2+ y2+ z2dV = ∫036

36−z2 0

1

r2+ z2 ⋅ rdrdzdθ

= 2π ∫36

36−z2 0

1 2

1

r2+ z2 ⋅ dr2dz= π ∫36ln(r2+ z2)036−z2dz

= π ∫36(ln(36) − 2 ln z)dz = π[ln(36)z − 2z ln z + 2z]63 = 6π lne 2 The grading policies are the same:

ˆ Knowing the formula dV = rdrdzdθ. No partial credit is allowed for this part. 3pts.

ˆ Writing the domain in cylindrical coordinates. 4pts

ˆ Evaluating the integral. Partial credits is allowed in this part.3pts

參考文獻

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