Several Variable Calculus

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Math 221
Examination 1
Spring 2013
Several Variable Calculus
Instructions These problems should be viewed as essay questions. Before making a calculation, you should explain in words what your strategy is.
Please write your solutions on your own paper. Each of the 10 problems counts
for 10 points.
1. Let ๐‘ฃโƒ— be the vector whose ๐šคฬ‚, ๐šฅฬ‚, and ๐‘˜ฬ‚ components are the last three digits of
your student identification number. Find an equation for the plane perpendicular to ๐‘ฃโƒ— and passing through the point (2, 2, 1).
Solution. The numerical answer is different for each student. Here is a
general solution assuming that the last three digits are ๐‘Ž, ๐‘, and ๐‘. The vector
โŸจ๐‘Ž, ๐‘, ๐‘โŸฉ is normal to the plane, so the equation of the plane has the general
form
๐‘Ž๐‘ฅ + ๐‘๐‘ฆ + ๐‘๐‘ง = ๐‘‘.
The value of ๐‘‘ can be determined by plugging in the coordinates of the given
point that lies in the plane:
๐‘‘ = 2๐‘Ž + 2๐‘ + ๐‘.
Thus one form of the answer is
๐‘Ž๐‘ฅ + ๐‘๐‘ฆ + ๐‘๐‘ง = 2๐‘Ž + 2๐‘ + ๐‘.
Another way to write the answer is
๐‘Ž(๐‘ฅ − 2) + ๐‘(๐‘ฆ − 2) + ๐‘(๐‘ง − 1) = 0.
2. Let ๐‘ฃโƒ— be the same vector as in the preceding problem. Find a vector that is
orthogonal both to ๐‘ฃโƒ— and to the vector โŸจ5, 0, 1โŸฉ.
Solution. Of course the vector โŸจ0, 0, 0โŸฉ solves the problem! But presumably
the goal is to find a “nontrivial” solution.
One way to get a vector orthogonal to two specified vectors is to compute
the cross product. If ๐‘ฃโƒ— is the vector โŸจ๐‘Ž, ๐‘, ๐‘โŸฉ, then the required vector is
โŸจ๐‘Ž, ๐‘, ๐‘โŸฉ × โŸจ5, 0, 1โŸฉ.
February 14, 2013
Page 1 of 9
Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
This cross product can be worked out by the determinant formula:
| ๐šคฬ‚ ๐šฅฬ‚ ๐‘˜ฬ‚ |
|
|
|๐‘ ๐‘ |
|๐‘Ž ๐‘ |
|
|
|
|
|
|
|
| ฬ‚ |๐‘Ž ๐‘|
ฬ‚
|๐‘Ž ๐‘ ๐‘ | = ๐šคฬ‚ |
| − ๐šฅฬ‚ |
| + ๐‘˜|
| = ๐‘ฬ‚๐šค − (๐‘Ž − 5๐‘)ฬ‚๐šฅ − 5๐‘๐‘˜.
|
|
|0 1 |
| 5 1|
| 5 0|
|5 0 1 |
|
|
|
|
|
|
|
|
The solution is not unique: any multiple of this vector is another solution.
3. The “twisted cubic” is the curve given by the parametric equations ๐‘ฅ = ๐‘ก,
๐‘ฆ = ๐‘ก2 , and ๐‘ง = ๐‘ก3 . Find parametric equations for the line tangent to this
curve at the point where ๐‘ก = 1.
Solution. The coordinate vector of a point on the curve at time ๐‘ก is โŸจ๐‘ก, ๐‘ก2 , ๐‘ก3 โŸฉ.
The derivative vector โŸจ1, 2๐‘ก, 3๐‘ก2 โŸฉ points in the direction of the tangent line.
When ๐‘ก = 1, this tangent vector becomes โŸจ1, 2, 3โŸฉ. And when ๐‘ก = 1, the
corresponding point on the curve has coordinates (1, 1, 1).
Thus the problem amounts to writing equations for a line passing through
the point (1, 1, 1) in the direction of the vector โŸจ1, 2, 3โŸฉ. Parametric equations
for this line are
๐‘ฅ=1+๐‘ก
๐‘ฆ = 1 + 2๐‘ก
๐‘ง = 1 + 3๐‘ก.
The problem does not ask for the symmetric equations of the line; those
equations would be
๐‘ฅ−1 ๐‘ฆ−1 ๐‘ง−1
=
=
.
1
2
3
4. Explain how to use a dot product to compute the distance between a plane
and a line parallel to that plane.
Solution. Pick an arbitrary point on the plane and an arbitrary point on the
line. Subtract the corresponding coordinates to get a vector pointing from
one point to the other. Take the dot product of this vector with a unit vector
in the direction of the normal to the plane. Finally, take the absolute value,
if necessary, in case the normal vector is pointing backward.
February 14, 2013
Page 2 of 9
Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
Another way to express this process is to find a vector joining a point on
the plane to a point on the line and to compute the scalar projection of this
vector onto the direction normal to the plane.
If the line and the plane are given by explicit equations, then all the data
needed in this calculation can be read off from the equations. To get a point
on the line (or on the plane), plug in arbitrary values (zero, for instance)
for all the variables but one, and solve for the remaining variable. A vector
normal to the plane with equation ๐‘Ž๐‘ฅ + ๐‘๐‘ฆ + ๐‘๐‘ง = ๐‘‘ is โŸจ๐‘Ž, ๐‘, ๐‘โŸฉ.
√ And you can
make this vector into a unit vector by dividing it by its length ๐‘Ž2 + ๐‘2 + ๐‘ 2 .
5. The vector function ๐‘Ÿโƒ—(๐‘ก) = โŸจ2 cos(๐‘ก), 2 sin(๐‘ก), ๐‘กโŸฉ describes a helix (a spiral).
Show that the curvature of this helix is constant (that is, the same for every
value of ๐‘ก).
Solution. The details of the solution depend on which formula you apply
for the curvature ๐œ….
One formula says that if ๐‘‡โƒ— is the unit tangent vector, namely ๐‘Ÿโƒ— ′ โˆ•|โƒ—๐‘Ÿ ′ |, then
๐œ… equals |๐‘‡โƒ— ′ |โˆ•|โƒ—๐‘Ÿ ′ |. So compute:
๐‘Ÿโƒ— ′ (๐‘ก) = โŸจ−2 sin(๐‘ก), 2 cos(๐‘ก), 1โŸฉ,
√
√
|โƒ—๐‘Ÿ ′ (๐‘ก)| = 4(sin ๐‘ก)2 + 4(cos ๐‘ก)2 + 12 = 5,
1
๐‘‡โƒ— (๐‘ก) = √ โŸจ−2 sin(๐‘ก), 2 cos(๐‘ก), 1โŸฉ ,
5
1
๐‘‡โƒ— ′ (๐‘ก) = √ โŸจ−2 cos(๐‘ก), −2 sin(๐‘ก), 0โŸฉ,
5
√
2
1
|๐‘‡โƒ— ′ (๐‘ก)| = √
4(cos ๐‘ก)2 + 4(sin ๐‘ก)2 = √ ,
5
5
√
2โˆ• 5 2
๐œ…= √ = .
5
5
Thus the curvature is indeed independent of ๐‘ก.
An alternative formula for ๐œ… is
February 14, 2013
|โƒ—๐‘Ÿ ′ × ๐‘Ÿโƒ— ′′ |
. Here is the computation using
|โƒ—๐‘Ÿ ′ |3
Page 3 of 9
Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
that formula:
๐‘Ÿโƒ— ′ (๐‘ก) = โŸจ−2 sin(๐‘ก), 2 cos(๐‘ก), 1โŸฉ,
๐‘Ÿโƒ— ′′ (๐‘ก) = โŸจ−2 cos(๐‘ก), −2 sin(๐‘ก), 0โŸฉ,
|
๐šคฬ‚
๐šฅฬ‚
๐‘˜ฬ‚ ||
|
|
|
′
′′
ฬ‚
๐‘Ÿโƒ— (๐‘ก) × ๐‘Ÿโƒ— (๐‘ก) = | −2 sin(๐‘ก) 2 cos(๐‘ก) 1| = 2 sin(๐‘ก)ฬ‚๐šค − 2 cos(๐‘ก)ฬ‚๐šฅ + 4๐‘˜,
|
|
|−2 cos(๐‘ก) −2 sin(๐‘ก) 0|
|
|
√
√
√
′
′′
2
2
|โƒ—๐‘Ÿ (๐‘ก) × ๐‘Ÿโƒ— (๐‘ก)| = 4(sin ๐‘ก) + 4(cos ๐‘ก) + 16 = 20 = 2 5,
√
√
′
2
2
2
|โƒ—๐‘Ÿ (๐‘ก)| = 4(sin ๐‘ก) + 4(cos ๐‘ก) + 1 = 5,
√
2 5
2
๐œ… = (√ )3 = .
5
5
Remark Even without doing any calculation, one can see by geometric
reasoning that the curvature must be constant. Think of the helix as the
threads on a bolt. Any point of the helix can be moved to any other point by
rotating the bolt and moving it parallel to its axis. But a rigid motion does
not change the curvature. Since all points of the helix are equivalent to each
other via rigid motions, the curvature must be the same at all points.
6. Find a function ๐‘“ (๐‘ฅ, ๐‘ฆ) for which
๐œ•๐‘“
๐œ•๐‘“
= 2๐‘ฅ + ๐‘ฆ and
= ๐‘ฅ + ๐‘ฆ.
๐œ•๐‘ฅ
๐œ•๐‘ฆ
Solution. This question is in the spirit of the game show Jeopardy: the
answer to a partial-differentiation problem is given, and you need to recover
the original function.
The systematic method is to start by integrating the first equation with respect to ๐‘ฅ to deduce that
๐‘“ (๐‘ฅ, ๐‘ฆ) = ๐‘ฅ2 + ๐‘ฅ๐‘ฆ + ๐ถ,
where ๐ถ is an integration constant. But from the point of view of the ๐‘ฅ partial
derivative, what “constant” means is “independent of ๐‘ฅ,” so the “constant” ๐ถ
is really a function ๐ถ(๐‘ฆ) that depends on ๐‘ฆ. Next take the ๐‘ฆ partial derivative:
๐œ•๐‘“
๐œ• 2
=
(๐‘ฅ + ๐‘ฅ๐‘ฆ + ๐ถ(๐‘ฆ)) = ๐‘ฅ + ๐ถ ′ (๐‘ฆ).
๐œ•๐‘ฆ
๐œ•๐‘ฆ
February 14, 2013
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Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
๐œ•๐‘“
= ๐‘ฅ + ๐‘ฆ, so ๐ถ ′ (๐‘ฆ) must be equal
๐œ•๐‘ฆ
to ๐‘ฆ. Therefore ๐ถ(๐‘ฆ) = 12 ๐‘ฆ2 + ๐‘˜, where this time ๐‘˜ is authentically a constant
(independent of both ๐‘ฅ and ๐‘ฆ). Accordingly, the final answer is that ๐‘“ (๐‘ฅ, ๐‘ฆ) =
๐‘ฅ2 + ๐‘ฅ๐‘ฆ + 12 ๐‘ฆ2 + ๐‘˜. Since the question asks for “a” function, not “the most
On the other hand, it is given that
general function,” the answer ๐‘ฅ2 + ๐‘ฅ๐‘ฆ + 12 ๐‘ฆ2 is perfectly acceptable.
Alternatively, you could solve the problem by the “guess and check” method.
The simplest function whose ๐‘ฅ partial derivative equals 2๐‘ฅ + ๐‘ฆ is ๐‘ฅ2 + ๐‘ฅ๐‘ฆ,
and the simplest function whose ๐‘ฆ partial derivative equals ๐‘ฅ + ๐‘ฆ is ๐‘ฅ๐‘ฆ + 12 ๐‘ฆ2 .
These two expressions do not match, but if you try merging them as the
function ๐‘ฅ2 + ๐‘ฅ๐‘ฆ + 12 ๐‘ฆ2 , then you can easily check that this function solves
the problem.
Yet another approach is to observe that the given first-order partial derivatives are first-degree expressions in ๐‘ฅ and ๐‘ฆ, so the original function ๐‘“ (๐‘ฅ, ๐‘ฆ)
must be a second-degree expression in ๐‘ฅ and ๐‘ฆ. The most general such expression has the form ๐‘Ž๐‘ฅ2 + ๐‘๐‘ฅ๐‘ฆ + ๐‘๐‘ฆ2 for certain numbers ๐‘Ž, ๐‘, and ๐‘. Then
๐œ•๐‘“
= 2๐‘Ž๐‘ฅ + ๐‘๐‘ฆ,
๐œ•๐‘ฅ
๐œ•๐‘“
๐‘ฅ+๐‘ฆ=
= ๐‘๐‘ฅ + 2๐‘๐‘ฆ.
๐œ•๐‘ฆ
2๐‘ฅ + ๐‘ฆ =
Evidently these equations for the undetermined coefficients ๐‘Ž, ๐‘, and ๐‘ are
satisfied when ๐‘Ž = 1, ๐‘ = 1, and ๐‘ = 1โˆ•2.
7. Suppose ๐‘ง = 21 ๐‘ฅ2 − 13 ๐‘ฆ3 . Find the point(s) on this surface where the tangent
plane is parallel to the plane with equation ๐‘ฅ + ๐‘ฆ + ๐‘ง = 1.
Solution. Two planes are parallel precisely when their normal vectors are
parallel. The vector โŸจ1, 1, 1โŸฉ is normal to the given plane, so what needs
to be determined is a vector normal to the surface. If the equation for the
surface is rewritten in the form of a level surface as
๐‘ง − 21 ๐‘ฅ2 + 13 ๐‘ฆ3 = 0,
then a normal vector can be obtained as the gradient vector โŸจ−๐‘ฅ, ๐‘ฆ2 , 1โŸฉ.
The two vectors โŸจ1, 1, 1โŸฉ and โŸจ−๐‘ฅ, ๐‘ฆ2 , 1โŸฉ have the same third coordinate, so
these vectors are parallel precisely when the other two coordinates match
February 14, 2013
Page 5 of 9
Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
up: namely, 1 = −๐‘ฅ and 1 = ๐‘ฆ2 . Consequently, ๐‘ฅ = −1 and ๐‘ฆ = ±1. Going
back to the equation of the surface reveals that if ๐‘ฅ = −1 and ๐‘ฆ = +1, then
๐‘ง = 1โˆ•6; while if ๐‘ฅ = −1 and ๐‘ฆ = −1, then ๐‘ง = 5โˆ•6. Therefore the two
points that solve the problem are (−1, 1, 1โˆ•6) and (−1, −1, 5โˆ•6).
8. Suppose ๐‘ฅ cos(๐‘ฆ) + sin(๐‘ฅ๐‘ง) = ๐‘’๐‘ฆ . Find
๐œ•๐‘ง
at the point (1, 0, ๐œ‹).
๐œ•๐‘ฅ
Solution. Differentiate implicitly with respect to ๐‘ฅ (viewing ๐‘ฆ as constant):
)
(
๐œ•
๐œ•๐‘ง
cos(๐‘ฆ) + cos(๐‘ฅ๐‘ง) (๐‘ฅ๐‘ง) = 0, or cos(๐‘ฆ) + cos(๐‘ฅ๐‘ง) ๐‘ง + ๐‘ฅ
= 0.
๐œ•๐‘ฅ
๐œ•๐‘ฅ
Insert the values of the coordinates at the specified point:
(
)
๐œ•๐‘ง
๐œ•๐‘ง
1− ๐œ‹+
= 0,
so
= 1 − ๐œ‹.
๐œ•๐‘ฅ
๐œ•๐‘ฅ
9. Suppose ๐‘“ (๐‘ฅ, ๐‘ฆ) = ๐‘ฅ3 − 3๐‘ฅ๐‘ฆ + ๐‘ฆ3 . Find the point(s) at which this function
has a local minimum.
Solution. First identify the critical points by setting both partial derivatives
equal to zero:
๐œ•๐‘“
= 3๐‘ฅ2 − 3๐‘ฆ,
๐œ•๐‘ฅ
๐œ•๐‘“
0=
= −3๐‘ฅ + 3๐‘ฆ2 .
๐œ•๐‘ฆ
0=
The first equation implies that ๐‘ฆ = ๐‘ฅ2 , and the second equation implies
that ๐‘ฅ = ๐‘ฆ2 = (๐‘ฅ2 )2 = ๐‘ฅ4 . Consequently, either ๐‘ฅ = 0 or ๐‘ฅ = 1; the
corresponding values of ๐‘ฆ are 0 and 1. Thus the critical points are (0, 0) and
(1, 1).
To apply the second-derivative test, compute the matrix of second-order partial derivatives:
(
) (
)
๐‘“๐‘ฅ๐‘ฅ ๐‘“๐‘ฅ๐‘ฆ
6๐‘ฅ −3
=
.
๐‘“๐‘ฆ๐‘ฅ ๐‘“๐‘ฆ๐‘ฆ
−3 6๐‘ฆ
February 14, 2013
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Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
(
)
0 −3
At the point (0, 0), this matrix becomes
, which has negative
−3
0
determinant, so the point (0, 0) is a saddle point. At
( the point
) (1, 1), the
6 −3
matrix of second-order partial derivatives becomes
. Now the
−3
6
determinant is positive, and both derivatives ๐‘“๐‘ฅ๐‘ฅ and ๐‘“๐‘ฆ๐‘ฆ are positive, so the
point (1, 1) is a local minimum.
10. Suppose ๐‘“ (๐‘ฅ, ๐‘ฆ) = ๐‘ฅ2 +๐‘ฆ. Find the absolute maximum value of this function
on the closed disk where ๐‘ฅ2 + ๐‘ฆ2 ≤ 1.
๐œ•๐‘“
= 1, so the function ๐‘“ has no critical points.
๐œ•๐‘ฆ
Therefore all that is required is to find the maximum of ๐‘“ on the circle where
๐‘ฅ2 + ๐‘ฆ2 = 1.
Solution. Observe that
Apply the method of Lagrange multipliers: the gradient of ๐‘“ , which equals
โŸจ2๐‘ฅ, 1โŸฉ, must be parallel to the gradient of the function defining the circle,
which is โŸจ2๐‘ฅ, 2๐‘ฆโŸฉ. In other words, there is a number ๐œ† such that
2๐‘ฅ = 2๐‘ฅ๐œ†,
1 = 2๐‘ฆ๐œ†.
The second equation says that ๐œ† = 1โˆ•(2๐‘ฆ), and substituting this expression
into the first equation shows that 2๐‘ฅ = 2๐‘ฅโˆ•(2๐‘ฆ), or 2๐‘ฅ๐‘ฆ = ๐‘ฅ, or 2๐‘ฅ๐‘ฆ − ๐‘ฅ = 0,
or ๐‘ฅ(2๐‘ฆ − 1) = 0. Therefore either ๐‘ฅ = 0 or ๐‘ฆ = 1โˆ•2.
If ๐‘ฅ = 0, the constraint that ๐‘ฅ2 + ๐‘ฆ2 = 1 implies that ๐‘ฆ = ±1. In this case,
there are two candidate points, (0, 1) and (0, −1). Now ๐‘“ (0, 1) = 1 and
2
2
๐‘“ (0, −1)
√1 implies that
√ = −1. If ๐‘ฆ = 1โˆ•2, then the constraint that ๐‘ฅ + ๐‘ฆ =
๐‘ฅ =√± 3โˆ•2. In this case, there are two candidate points, (+ 3โˆ•2, 1โˆ•2) and
(− 3โˆ•2, 1โˆ•2). The value of the function ๐‘“ at both of these points is 5โˆ•4.
The maximum value of the function ๐‘“ at the four candidate points is thus
equal to 5โˆ•4.
An alternative method is to observe first that ๐‘ฅ2 + ๐‘ฆ will not achieve a maximum when the number ๐‘ฆ is negative. Moreover, there is no need to consider
negative values of ๐‘ฅ, since ๐‘“ (−๐‘ฅ, ๐‘ฆ) = ๐‘“ (๐‘ฅ, ๐‘ฆ). Thus it suffices to find the
maximum value of ๐‘“ (๐‘ฅ, ๐‘ฆ) on the√part of the circle lying in the first quadrant.
On that part of the circle, ๐‘ฆ = 1 − ๐‘ฅ2 (with the positive square root), so
February 14, 2013
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Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
√
๐‘“ (๐‘ฅ, ๐‘ฆ) reduces to the single-variable function ๐‘ฅ2 + 1 − ๐‘ฅ2 . The problem
then becomes a question of maximizing this function of ๐‘ฅ when 0 ≤ ๐‘ฅ ≤ 1.
Find the critical point of this one-variable function by setting the derivative
equal to 0:
0 = 2๐‘ฅ + 21 (1 − ๐‘ฅ2 )−1โˆ•2 (−2๐‘ฅ).
Either ๐‘ฅ = 0 (which is√an endpoint) or 0 = 2 − (1 − ๐‘ฅ2 )−1โˆ•2 . The latter
2
2
2
equation
√ simplifies to 1 − ๐‘ฅ = 1โˆ•2 or 1 − ๐‘ฅ = 1โˆ•4 or ๐‘ฅ = 3โˆ•4 or
๐‘ฅ = √3โˆ•2 (since ๐‘ฅ is assumed to be positive). The value of the function
๐‘ฅ2 + 1 − ๐‘ฅ2 at this critical point is 5โˆ•4; the value at the endpoint where
๐‘ฅ = 0 is 1; and the value at the endpoint where ๐‘ฅ = 1 is 1. Thus the absolute
maximum value is 5โˆ•4.
Optional bonus problem for extra credit
The parametric equations
๐‘ฅ = (sin ๐‘ก)(sin 12 ๐‘ก)2 ,
๐‘ฆ = (cos ๐‘ก)(sin 12 ๐‘ก)2 ,
0 ≤ ๐‘ก ≤ 2๐œ‹
describe a cardioid, a heart-shaped figure.
Show that the arc length of this cardioid is equal to 4.
Solution. The arc length is the integral of the speed, which is
√
( )2 ( )2
d๐‘ฆ
d๐‘ฅ
+
.
d๐‘ก
d๐‘ก
First compute the derivatives using the product rule and the chain rule:
d๐‘ฅ
= (cos ๐‘ก)(sin 12 ๐‘ก)2 + (sin ๐‘ก)2(sin 21 ๐‘ก)(cos 12 ๐‘ก)(1โˆ•2),
d๐‘ก
d๐‘ฆ
= (− sin ๐‘ก)(sin 12 ๐‘ก)2 + (cos ๐‘ก)2(sin 21 ๐‘ก)(cos 21 ๐‘ก)(1โˆ•2).
d๐‘ก
Of course the factors of 2 and 1โˆ•2 cancel. Now add the squares of these derivatives,
observing that the cross terms cancel out because of the minus sign in the second
February 14, 2013
Page 8 of 9
Dr. Boas
Math 221
Examination 1
Spring 2013
Several Variable Calculus
equation:
(
d๐‘ฅ
d๐‘ก
)2
(
+
d๐‘ฆ
d๐‘ก
)2
= [(cos ๐‘ก)2 + (sin ๐‘ก)2 ](sin 12 ๐‘ก)4
+ [(sin ๐‘ก)2 + (cos ๐‘ก)2 ](sin 21 ๐‘ก)2 (cos 12 ๐‘ก)2
= (sin 12 ๐‘ก)4 + (sin 12 ๐‘ก)2 (cos 12 ๐‘ก)2
= (sin 12 ๐‘ก)2 [(sin 21 ๐‘ก)2 + (cos 12 ๐‘ก)2 ]
= (sin 12 ๐‘ก)2 .
Taking the square root shows that the speed is sin 12 ๐‘ก. Therefore the computation
of the arc length reduces to the following integral:
2๐œ‹
∫0
February 14, 2013
|2๐œ‹
sin 21 ๐‘ก d๐‘ก = −2 cos 21 ๐‘ก | = −2(cos ๐œ‹ − cos 0) = 4.
|0
Page 9 of 9
Dr. Boas
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