EXAMPLES FOR
SECTION 13.6
Directional Derivative Example
If your answer to the question posed at the end
of the Section 13.3 #40 example related to the directional derivative, or if you have
not yet heard about directional derivatives but your answer somehow
related to a derivative as a rate of change relative to change along the
line y = (4/3)x or change relative to change in the direction of a vector,
say <3,4>, then good show. Here is the DPGraph
Picture again that the question related to. Maple Picture
Here are some notes
on the directional derivative and more examples involving the gradient
and the directional derivative..
|
Section 13.6 #32 Maximizing the Directional Derivative
DPGraph
Picture of the Surface DPGraph
Picture with the Point
DPGraph
Picture of the surface, the point, and a plane containing the point
and a line in the xy-coordinate plane with direction vector u where
the x- and y-components of u equal the x- and y-components of the
direction vector for the directional derivative. See the analysis
below for more details.
|
Maximizing the Directional
Derivative Find the
maximum value of the directional derivative of the given function at the
indicated point.
|
Animation
QT Version |
Powerpoint
Presentation on the Relationship Between the Gradient and Level Curves
Heat
Seeking Particle Examples
T(x,y) = 100 - x2 - 2y2
Starting Point (2,4)
Let the path be described by r(t) = <
x(t) , y(t) >
Then r'(t) = < dx/dt , dy/dt >
gives the direction of motion.
Since this is a heat seeking particle it must move at
all times in the direction of maximum increase in temperature. This must
be the direction of the gradient of the temperature function T(x,y).
grad T(x,y) = < -2x , -4y >
Powerpoint Enhancement |
Click here to see a
Maple worksheet on this example.
Click on the picture to see a larger picture of the
analytical solution constrained so that the path looks orthogonal to the
equal temperature lines. |
In general then it must be the case that grad T =
k r'(t) where k is some constant. Let us assume a parameterization
of the path such that k = 1 so that grad T = r'(t). Note
that we are not claiming that r'(t) gives the velocity of the heat
seeking particle, only that it gives the direction.
From grad T = r'(t) we equate vector
components to get dx/dt = -2x and dy/dt = -4y. Let 0 be the value of t at
the starting point so that x(0) = 2 and y(0) = 4. Thus we have two
differential equations to solve.
dx/dt =
-2x x(0) = 2
(1/x)dx =
-2dt
ln | x |
= -2t + c
| x | = e-2t
+ c = e-2t ec = c1e-2t
x = c2e-2t
x = 2e-2t
since x(0) = 2 yields c2 = 2
In a
similar fashion we would find that from
dy/dt =
-4y and y(0) = 4 we get
y = 4e-4t
Thus the
path is given by r(t) = < 2e-2t , 4e-4t
>.
Since y =
(2e-2t)2 we see that the path is also given by y = x2.
The
picture on the right shows the path. Animation |
|
A similar problem involves finding the path followed by
a heat seeking object in space where the temperature distribution is given by
T(x,y,z) = 100 - 3x - y - z2 and the starting point is (2,2,5).
Let the path be described by r(t) = <
x(t) , y(t) , z(t) >
Then r'(t) = < dx/dt , dy/dt , dz/dt >
gives the direction of motion.
Since this is a heat seeking particle it must move at
all times in the direction of maximum increase in temperature. This must
be the direction of the gradient of the temperature function T(x,y,z).
grad T(x,y,z) = < -3 , -1 , -2z >
In general then it must be the case that grad T =
k r'(t) where k is some constant. Let us assume a parameterization
of the path such that k = 1 so that grad T = r'(t). Note
that we are not claiming that r'(t) gives the velocity of the heat
seeking particle, only that it gives the direction.
From grad T = r'(t) we equate vector
components to get
dx/dt = -3, dy/dt = -1, and
dz/dt = -2z.
Let 0 be the value of t at
the starting point so that
x(0) = 2, y(0) = 2, and z(0) = 5.
We have
three
differential equations to solve and their solutions
will yield x = -3t + 2, y =
-t + 2, and z = 5e-2t.
Thus r(t) = < -3t + 2 , -t + 2 , 5e-2t
>
Click here to see an
animated
picture of a portion of the path. |
|
Heat Seeking Particle Problem To Practice On
Find the path followed by a heat seeking particle on a
plate whose temperature distribution is given by T(x,y) starting at the given
point (two cases given).
Click
here to see a Maple worksheet on the problems above. |
|
The Billy Johnson Heat Seeking Particle Problem
The idea for this problem was suggested by Billy
Johnson. The temperature distribution function given below has multiple
relative hot and relative cold spots. Finding the path followed by a heat
seeking particle (or object) starting at some given point required using the
gradient repeatedly to approximate the direction of motion. The linked
Maple Worksheet shows many possibilities and how Maple can approximate the
paths.
Maple Worksheet
Section 13.6 #76 This is a technology
problem--see this Maple Worksheet
Click here to see a Maple
worksheet depicting a skier taking the path of steepest descent down a mountain.
Here is my Maple Twin Peaks worksheet.
return
|