cclogo.gif (38585 bytes)   Seminole State Homepage   |   Calculus I   |   Calculus II    |    Calculus III   |   Diff Eq    |    Calculus Homepage cclogo.gif (38585 bytes)

 

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

 

 

 

 


          This site contains links to other Internet sites.  These links are not endorsements of any products or services in such sites, and no information  

           in such site has been endorsed or approved by this site.

        Lane Vosbury, Mathematics, Seminole State College   email:  vosburyl@seminolestate.edu

        This page was last updated on 08/21/14          Copyright 2002          webstats