Exam Problems: Chain Rule, Directional Derivative, Tangent Plane, and Temperature Max., Exams of Calculus

Solutions to exam problems involving the chain rule, directional derivative, finding the equation of the tangent plane, and maximizing temperature on a sphere using the lagrange multiplier method. The problems also include calculating volumes and integrals.

Typology: Exams

Pre 2010

Uploaded on 08/19/2009

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Exam 2: Solutions
Problem 1. Use the chain rule to find ∂z
∂u and ∂z
∂v if z=x2y3+xsin y,
x=u2,y=uv.
Solution.
∂z
∂u =z
∂x
∂x
∂u +z
∂y
∂y
∂u = (2xy3+ sin y)(2u) + (3x2y2+xcos y)v
= (2u2u3v3+ sin(uv))(2u) + (3u4u2v2+u2cos(uv))v
= 4u6v3+ 2usin(uv)+3u6v3+u2vcos(uv)
= 7u6v3+ 2usin(uv) + u2vcos(uv).
∂z
∂v =z
∂x
∂x
∂v +z
∂y
∂y
∂v = (2xy3+ sin y)·0 + (3x2y2+xcos y)u
= (3u4u2v2+u2cos(uv))u= 3u7v2+u3cos(uv).
Problem 2. Find the directional derivative of f(x, y, z) = x2y3+
xz at (1,2,3) in the direction of
a= 5
j+
k.
Solution. The unit vector in the direction of
ais
u=
a
k
ak=5
26
j+1
26
k .
Then
D
uf(1,2,3) = f(1,2,3) ·
u
=2xy3+z
2x
i+ 3x2y2
j+x
2z
k(1,2,3)
·5
26
j+1
26
k
= (16 + 3
2)
i+ 12
j+1
23
k!·5
26
j+1
26
k
=60
26 +1
278.
Problem 3. Find the equation of the tangent plane to the surface
z=x2yat the point (1,2,2).
1
pf3
pf4

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Exam 2: Solutions

Problem 1. Use the chain rule to find ∂z∂u and ∂z∂v if z = x^2 y^3 +x sin y, x = u^2 , y = uv.

Solution. ∂z ∂u

∂z ∂x

∂x ∂u

∂z ∂y

∂y ∂u

= (2xy^3 + sin y)(2u) + (3x^2 y^2 + x cos y)v

= (2u^2 u^3 v^3 + sin(uv))(2u) + (3u^4 u^2 v^2 + u^2 cos(uv))v = 4 u^6 v^3 + 2u sin(uv) + 3u^6 v^3 + u^2 v cos(uv) = 7 u^6 v^3 + 2u sin(uv) + u^2 v cos(uv). ∂z ∂v

∂z ∂x

∂x ∂v

∂z ∂y

∂y ∂v

= (2xy^3 + sin y) · 0 + (3x^2 y^2 + x cos y)u

= (3u^4 u^2 v^2 + u^2 cos(uv))u = 3u^7 v^2 + u^3 cos(uv).

Problem 2. Find the directional derivative of f (x, y, z) = x^2 y^3 + √ xz at (1, − 2 , 3) in the direction of −→a = 5

j +

k.

Solution. The unit vector in the direction of −→a is

−→u =

−→a ‖−→a ‖

j +

k.

Then

D−→u f (1, − 2 , 3) = ∇f (1, − 2 , 3) · −→u

=

2 xy^3 +

z 2

x

i + 3x^2 y^2

j +

x 2

z

k

(1,− 2 ,3)

j +

k

i + 12

j +

k

j +

k

Problem 3. Find the equation of the tangent plane to the surface z = x^2 y at the point (1, 2 , 2). 1

Solution. The equation of the tangent plane to the surface z = f (x, y) at the point (x 0 , y 0 , z 0 ) is

z = z 0 + fx(x 0 , y 0 )(x − x 0 ) + fy(x 0 , y 0 )(y − y 0 ).

We have fx(x, y) = 2xy, fy(x, y) = x^2 , fx(1, 2) = 2 · 1 · 2 = 4, fy(1, 2) = 12 = 1. Thus, the tangent plane is z = 2 + 4(x − 1) + 1(y − 2), i.e.,

z = 4x + y − 4.

Problem 4. The temperature, T , at a point in space is given by T (x, y, z) = 400xyz^2 degrees Celsius. Use the Lagrange multiplier method to find the highest temperature on the sphere x^2 + y^2 + z^2 = 1.

Solution. The problem is to maximize T (x, y, z) = 400xyz^2 which is subject to the constraint g(x, y, z) = x^2 + y^2 + z^2 − 1 = 0. The Lagrange equations Tx = λgx, Ty = λgy, Tz = λgz become 400yz^2 = 2 λx, 400xz^2 = 2λy, 800xyz = 2λz. Eliminating λ from these equations, we obtain 200 yz^2 x

200 xz^2 y

= 400xy.

(Note that z 6 = 0, otherwise it follows from the Lagrange equations that x = y = z = 0 which is impossible for the given constraint.) The first of the two equations above gives x^2 = y^2 , and the second one gives z^2 = 2y^2. From the constraint equation we obtain y^2 +y^2 +2y^2 = 1, i.e., 4 y^2 = 1. Thus y = 12 or y = −^12. Correspondingly, x = 12 or x = −^12 ,

and z =

√ 2 2 or^ z^ =^ −

√ 2 2.^ The maximal value of the temperature T (x, y, z) on the sphere x^2 + y^2 + z^2 = 1 is therefore

T

= 50 (degrees Celsius).

Problem 5. Find the volume of the solid in the first octant enclosed by z = 4 − y^2 , z = 0, x = 0, y = x, and y = 2.

Solution. The projection of the solid onto the xy-plane is the (tri- angle) domain D bounded by the lines x = 0, y = x, and y = 2. It can be described by the inequalities 0 ≤ y ≤ 2, 0 ≤ x ≤ y. Therefore the

Solution. The domain of integration D is described as a type II domain by 0 ≤ y ≤ 1, 2y ≤ x ≤ 2. It can be easily seen that D is a triangle bounded by the lines y = 0, x = 2y, and x = 2. The domain D is described also as a type I domain by 0 ≤ x ≤ 2, 0 ≤ y ≤ x 2. Therefore,

∫^1

0

∫^2

2 y

cos(x^2 ) dx dy =

∫^2

0

x 2 ∫

0

cos(x^2 ) dy dx =

∫^2

0

y cos(x^2 )

x 2 y=0 dx

∫^2

0

x 2

cos(x^2 ) dx =

∫^2

0

2 x cos(x^2 ) dx

∫^2

0

cos(x^2 ) d(x^2 ) =

sin(x^2 )

∣^2

sin 4 4