6810: 1094 Session 16

Handouts: "Three-Dimensional Plots with Gnuplot", excerpts from Landau/Paez PDE chapters

Here we'll look at some basic examples of solving partial differential equations (PDE's) based on simple difference methods. Note: The PDE codes were designed to have very short printouts; there are many ways to improve the coding technique!

3-D Plots with Gnuplot

We have frequently used Gnuplot for visualization, but we have only considered two-dimensional plots. Now we will want to make three-dimensional surface plots of functions and data (in particular, the output of today's programs!).

  1. Follow through the handout on "Three-Dimensional Plots with Gnuplot". Make sure to look at the code for 3d_shape.cpp and predict what shape will be plotted.

  2. Note that you can rotate a plot by grabbing it with the mouse.
  3. Figure out how to make a parametric plot of a sphere using trigonometric functions. To plot a 2-d circle, you would type:
      gnuplot> set parametric
      gnuplot> plot [0:2*pi] sin(t),cos(t)
    (hint: think spherical coordinates). What command did you use for the sphere?

Laplace's Equation

Here we take a look at a solution to Laplace's equation by a simple relaxation method.

  1. Take a look at laplace.cpp and see what problem it is solving and how it carries out the method described in section 25.4 of the handout. What are the basic approximations in implementing the PDE?

  2. Compile and run the code and make a 3-d plot of the output using gnuplot. Include contours (try "set contour base" and "set contour surface"). To control the contour spacing, use "set cntrparam" to get contours at every 10 units (find out the details from "help set cntrparam"). What command did you use?

  3. Given the equipotential lines, where is the electric field strongest?

    You might want to sketch in the electric field lines on your plot, starting from the 100V end.
  4. How do you know if the relaxation method is converged? Pick a fixed point (i.e., fixed values of i and j) and see how much potl[i][j] changes from one iteration to the next (i.e., print out the value). Increase the number of iterations until you have five significant figure accuracy for your point. How can you build this into the code so that it stops iterating when this accuracy is reached? Describe a way to test the convergence more generally (you don't need to implement it).

  5. Does it help to "damp" the iterations? Try adding damping (that is, the new value potl[i][j] at each (i,j) point is (1.-fraction) of the old value plus fraction times the formula for potl[i][j]). In fact, try 0 < fraction < 2 (which will reveal that "damping" is a poor choice of words!). What happens?

  6. [Bonus] The numerical solution to the PDE can be used for any boundary conditions. Suppose you have designed a piece of equipment that is essentially a small metal box at 100 V within a larger, grounded one. You find that sparking occurs inside it, which indicates too large an electric field. You need to determine where the field is greatest so you can change the geometry and eliminate the sparking. Modify laplace.cpp (call it laplace_boxes.cpp) to satisfy the new boundary conditions and figure out where the electric field is most intense. How would you redesign the equipment to reduce the field?

Diffusion Equation

Here we look at a solution to the temperature diffusion equation that steps through in time using a (crude) finite difference method.

  1. Take a look at eqheat.cpp and see how it carries out the method described in section 26.4 of the handout. [Note: We assume a cross section of 1 cm^2.] What are the basic approximations in implementing the PDE?

  2. Compile and run the code to generate eqheat.dat. Look at eqheat.dat and then make a 3-d plot of it using gnuplot, using the comments in the code and the handout as guides. Include contours (which are isotherms here). Interpret the plot for your partner.
  3. Stability test: Add a statement to the code to print out the constant so that you can compare it to 1/2 [note: the handout says 1/4 in (26.25) but this is a typo]. Then increase the conductivity to 0.4 and then 0.5. Look at the output file eqheat.dat before trying to plot (you should always do this!). Can you verify the stability criterion numerically?

  4. Now put the conductivity back to 0.12. Instead, let's change delta-x instead. How do we do that? What are delta-x and delta-t in the code? For what delta-x does the calculation become unstable?

  5. [Bonus] Suppose instead of one 100 cm bar we have two identical bars, each 50 cm long, placed end to end. One bar starts at 100 degrees C while the other is at 50 degrees C. The outside ends are again put in an ice bath at 0 degrees C. Modify the code for this case and determine how the temperature varies with time and location with an appropriate plot.

Wave Equation

Here we look at the solution to the wave equation for a string with fixed endpoints.

  1. Take a look at eqstring.cpp and see how it carries out the time-stepping method described in section 27.3 of the handout. Note how the wave speed and delta-x and delta-t are incorporated somewhat indirectly. What are the basic approximations in implementing the PDE?

  2. Compile and run the code and make a 3-d plot of the output using gnuplot (some hints for gnuplot settings are in the comments). Estimate the wave velocity c from the graph (be careful of the scale of the time axis) and compare to the theoretically expected value.

  3. The stability condition is said to be that the wave speed c is less than or equal to c' = Delta-x/Delta-t. Verify that the result is unstable if this is violated. What did you do and what happened?

  4. Modify the code so that the initial conditions are that the string is plucked in the middle (rather than near one end). What did you have to change?

    How would you modify the code so that it is easier to implement more general initial conditions?

6810: 1094 Session 16. Last modified: 07:36 am, April 17, 2013.