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<!--l. 8--><p class="noindent" >Steven R. Dunbar <br 
class="newline" />Department of Mathematics <br 
class="newline" />203 Avery Hall <br 
class="newline" />University of Nebraska-Lincoln <br 
class="newline" />Lincoln, NE 68588-0130 <br 
class="newline" /><span 
class="cmtt-12">http://www.math.unl.edu </span><br 
class="newline" />Voice: 402-472-3731 <br 
class="newline" />Fax: 402-472-8466                  </p>
<div class="center" 
>
<!--l. 1--><p class="noindent" >
</p><!--l. 7--><p class="noindent" > <span 
class="cmbx-12x-x-144">Math 489/Math 889</span><br />
<span 
class="cmbx-12x-x-144">Stochastic Processes and</span><br />
<span 
class="cmbx-12x-x-144">Advanced Mathematical Finance</span><br />
<span 
class="cmbx-12x-x-144">Dunbar, Fall 2009</span>
</p></div>
<!--l. 19--><p class="noindent" >__________________________________________________________________________
</p>
<div class="center" 
>
<!--l. 21--><p class="noindent" >
</p><!--l. 21--><p class="noindent" ><span 
class="cmr-17">Mathematical Modeling</span></p></div>
<!--l. 23--><p class="indent" >   _______________________________________________________________________
</p><!--l. 1--><p class="indent" >   Note: To read these pages properly, you will need the latest version of the
Mozilla Firefox browser, with the STIX fonts installed. In a few sections, you will
also need the latest Java plug-in, and JavaScript must be enabled. If you use a
browser other than Firefox, you should be able to access the pages and run the
applets. However, mathematical expressions will probably not display
correctly. Firefox is currently the only browser that supports all of the open
standards.
</p><!--l. 27--><p class="indent" >   _______________________________________________________________________________________________
</p><!--l. 29--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/rating.png" alt="Rating"  
 />
                                                                          

                                                                          
</p>
   <h3 class="likesectionHead"><a 
 id="x1-1000"></a>Rating</h3>
<!--l. 33--><p class="noindent" >Student: contains scenes of mild algebra or calculus that may require
guidance.
</p><!--l. 38--><p class="indent" >   _______________________________________________________________________________________________
</p><!--l. 40--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/question_mark.png" alt="Section Starter Question"  
 />
</p>
   <h3 class="likesectionHead"><a 
 id="x1-2000"></a>Section Starter Question</h3>
<!--l. 43--><p class="noindent" >Do you believe in the ideal gas law? Does it make sense to &#x201C;believe in&#x201D;
an equation? What do we really mean when we say we &#x201C;believe in&#x201D; an
equation?
</p><!--l. 47--><p class="indent" >   _______________________________________________________________________________________________
</p><!--l. 49--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/keyconcepts.png" alt="Key Concepts"  
 />
</p>
   <h3 class="likesectionHead"><a 
 id="x1-3000"></a>Key Concepts</h3>
<!--l. 52--><p class="noindent" >
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-3002x1">All mathematical models are wrong, but some mathematical models
      are useful.
      </li>
      <li 
  class="enumerate" id="x1-3004x2">If the modeling assumptions are satisfied, proper mathematical models
      should predict well given a wide range of conditions corresponding to
      the assumptions.
      </li>
      <li 
  class="enumerate" id="x1-3006x3">Knowing that all mathematical models are wrong, the real question
      becomes how wrong the model must be before it becomes unacceptable.
                                                                          

                                                                          
      </li>
      <li 
  class="enumerate" id="x1-3008x4">When observed outcomes deviate unacceptably from predicted ideal
      behavior in honest scientific or engineering work, then we must then
      alter our assumptions, re-derive the quantitative relationships, perhaps
      with more sophisticated mathematics or introducing more quantities
      and begin the cycle of modeling again.</li></ol>
<!--l. 73--><p class="noindent" >__________________________________________________________________________
</p><!--l. 75--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/vocabulary.png" alt="Vocabulary"  
 />
</p>
   <h3 class="likesectionHead"><a 
 id="x1-4000"></a>Vocabulary</h3>
<!--l. 77--><p class="noindent" >
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-4002x1">A  <span 
class="cmbx-12">mathematical  model  </span>is  a  mathematical  structure  (often  an
      equation)  expressing  a  relationship  among  a  limited  number  of
      quantifiable elements from the &#x201C;real world&#x201D; or some isolated portion of
      it.</li></ol>
<!--l. 85--><p class="noindent" >__________________________________________________________________________
</p><!--l. 87--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/mathematicalideas.png" alt="Mathematical Ideas"  
 />
</p>
   <h3 class="likesectionHead"><a 
 id="x1-5000"></a>Mathematical Ideas</h3>
<!--l. 90--><p class="noindent" >Remember the following proverb: <span 
class="cmti-12">All mathematical models are wrong, but some</span>
<span 
class="cmti-12">mathematical models are useful.</span>
</p><!--l. 94--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-6000"></a>Mathematical Modeling</h4>
<!--l. 96--><p class="noindent" >Mathematical modeling involves two equally important activities: </p>
                                                                          

                                                                          
      <ul class="itemize1">
      <li class="itemize">Building a mathematical structure, a model, based on hypotheses about
      relations among the quantities that describe the real world situation,
      and then deriving new relations,
      </li>
      <li class="itemize">Evaluating the model, comparing the new relations with the real world
      and making predictions from the model.</li></ul>
<!--l. 106--><p class="noindent" >Good mathematical modeling explains the hypotheses, the development of the model
and its solutions, and then supports the findings by comparing them
mathematically with the actual circumstances. Successful modeling requires a
balance between so much complexity that making predictions from the model may
be intractable and so little complexity that the predictions are unrealistic and
useless. A successful model must allow a user to consider the effects of different
policies.
</p><!--l. 114--><p class="indent" >   At a more detailed level, mathematical modeling involves successive steps in
the cycle of modeling:
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-6002x1">Factors and observations,
      </li>
      <li 
  class="enumerate" id="x1-6004x2">Mathematical structure,
      </li>
      <li 
  class="enumerate" id="x1-6006x3">Testing and sensitivity analysis,
      </li>
      <li 
  class="enumerate" id="x1-6008x4">Effects and observations.</li></ol>
<!--l. 126--><p class="noindent" >Consider the diagram in Figure&#x00A0;<a 
href="#x1-60091">1<!--tex4ht:ref: fig:cycle --></a> which illustrates the cycle of modeling. Steps 1 and
2 in the more detailed cycle are the first activity described above and steps 3 and
4 are the second activity.
</p>
   <hr class="figure" /><div class="figure" 
><table class="figure"><tr class="figure"><td class="figure" 
>
                                                                          

                                                                          
<a 
 id="x1-60091"></a>
                                                                          

                                                                          

<!--l. 134--><p class="noindent" ><img 
src="mathmodel1.png" alt="PIC"  
 />
<br /> </p><table class="caption" 
><tr style="vertical-align:baseline;" class="caption"><td class="id">Figure&#x00A0;1: </td><td  
class="content">The cycle of modeling</td></tr></table><!--tex4ht:label?: x1-60091 -->
                                                                          

                                                                          
   </td></tr></table></div><hr class="endfigure" />
   <h4 class="likesubsectionHead"><a 
 id="x1-7000"></a>Modeling</h4>
<!--l. 141--><p class="noindent" >A good description of the model will begin with an organized and complete
description of important factors and observations. The description will often use
data gathered from observations of the problem. It will also include the statement
of scientific laws and relations that apply to the important factors. From there,
the model must summarize and condense the observations into a small set of
hypotheses that capture the essence of the observations. The small set of
hypotheses is a restatement of the problem, changing the problem from a
descriptive, even colloquial, question into a precise formulation that moves the
statement from the general to the specific. This sets the stage for the modeler to
demonstrate a clear link between the listed assumptions and the building of the
model.
</p><!--l. 154--><p class="indent" >   The hypotheses translate into a mathematical structure that becomes the
heart of the mathematical model. Many mathematical models, particularly those
from physics and engineering, become a single equation but mathematical models
need not be a single concise equation. Mathematical models may be a regression
relation, either a linear regression, an exponential regression or a polynomial
regression. The choice of regression model should explicitly follow from the
hypotheses since the growth rate is an important consequence of the observations.
The mathematical model may be a linear or nonlinear optimization model,
consisting of an objective function and a set of constraints. Again the choice of
linear or nonlinear functions for the objective and constraints should explicitly
follow from the nature of the factors and the observations. For dynamic
situations, the observations often involve some quantity and its rates of
change. The hypotheses express some connection between these quantities
and the mathematical model then becomes a differential equation, either
linear or nonlinear depending on the explicit details of the scientific laws
relating the factors considered. For discretely sampled data instead of
continuous time expressions the model may become a difference equation. If an
important feature of the observations and factors is noise or randomness, then
the model may be a probability distribution or a stochastic process. The
classical models from science and engineering usually take one of these
classical equation-like forms but not all mathematical models need to
follow this format. Models may be a connectivity graph, or a group of
                                                                          

                                                                          
transformations.
</p><!--l. 181--><p class="indent" >   If the number of variables is more than a few, or the relations are complicated
to write in a concise mathematical expression then the model can be a computer
program. Programs written in either high-level languages such as C, FORTRAN
or Basic and very-high-level languages such as MATLAB or a computer algebra
system are mathematical models. Spreadsheets combining the data and the
calculations are a popular and efficient way to construct a mathematical model.
The collection of calculations in the spreadsheet express the laws connecting the
factors which are represented by the data in the rows and columns of the
spreadsheet. Some mathematical models may be expressed by using more
elaborate software specifically designed for modeling. Some software allows the
user to describe the connections between factors graphically to create and alter a
model.
</p><!--l. 196--><p class="indent" >   Although this set of examples of mathematical models varies in theoretical
sophistication and the equipment used, the core of each is to connect the data and
the relations into a mechanism that allows the user to vary elements of the model.
Creating a model, whether a single equation, a complicated mathematical
structure, a quick spreadsheet, or a large program is the essence of the first step
connecting the boxes labeled 1 and 2 above.
</p><!--l. 204--><p class="indent" >   First models need not be sophisticated or detailed. For beginning analysis
&#x201C;back of the envelope calculations&#x201D; and &#x201C;dimensional analysis&#x201D; will be as effective
as spending time setting up an elaborate model or solving equations with
advanced mathematics. Unit analysis to check consistency and outcomes of
relations is important to check the harmony of the modeling assumptions. A good
model pays attention to units, the quantities should be sensible and match.
Even more important, a non-dimensionalized model reveals significant
relationships, and major influences. Unit analysis is an important part of
modeling, and goes far beyond simple checking to make sure &#x201C;units cancel.&#x201D;
<span class="cite">[<a 
href="#Xlogan87">3</a>,&#x00A0;<a 
href="#Xlin74">2</a>]</span>
</p><!--l. 218--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-8000"></a>Mathematical Solution</h4>
<!--l. 220--><p class="noindent" >Once the modelers create the model, then they should derive some new relations
among the important quantities selected to describe the real world situation.
This is the step connecting the boxes labeled 2 and 3 in the diagram. If
                                                                          

                                                                          
the model is an equation, for instance the Ideal Gas Law, then one can
solve the equation for one of the variables in terms of the others. In the
Ideal Gas Law, solving for one of the gas parameters is quite easy. A
regression equation model may require almost no mathematical solution,
although it might be useful to find auxiliary quantities such as rates of
growth or maxima or minima. For an optimization problem the solution is
the set of optima or the rates of change of optima with respect to the
constraints. If the model is a differential equation or a difference equation, then
the solution may have some mathematical substance. For instance, for
a ballistics problem, the model may be a differential equation and the
solution by calculus methods yields the equation of motion. For a problem
with randomness, the derivation may find the mean or the variance. For
a connectivity graph, one might be interested in the number of cycles,
components or the diameter of the graph. If the model is a computer
program, then this step usually involves running the program to obtain the
output.
</p><!--l. 241--><p class="indent" >   It is easy for students to focus most attention on this stage of the process,
since the usual methods are the core of the typical mathematical curriculum. This
step usually requires no interpretation, the model dictates the methods that
must be used. This step is often the easiest in the sense that it is the
clearest on how to proceed, although the mathematical procedures may be
daunting.
</p><!--l. 248--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-9000"></a>Testing and Sensitivity</h4>
<!--l. 250--><p class="noindent" >Once this step is done, the model is ready for testing and sensitivity analysis. This
is the step that connects the boxes labeled 3 and 4. At the least, the
modelers should try to verify, even with common sense, the results of the
solution. Typically for a mathematical model, the previous step allows the
modelers to produce some important or valuable quantity of the model.
Modelers compare the results of the model with standard or common
inputs with known quantities for the data or statement of the problem.
This may be as easy as substituting into the derived equation, regression
expression, or equation of motion. When running a computer model or
program, this may involve sequences of program runs and related analysis.
                                                                          

                                                                          
With any model, the results will probably not be exactly the same as
the known data so interpretation or error analysis will be necessary. The
interpretation requires judgment on the relative magnitudes of the quantities
produced in light of the confidence in the exactness or applicability of the
hypotheses.
</p><!--l. 266--><p class="indent" >   Another important activity at this stage in the modeling process is the
sensitivity analysis. The modelers should choose some critical feature of the model
and then vary the parameter value that quantifies that feature. The results should
be carefully compared to the real world and to the predicted values. If the results
do not vary substantially, then perhaps the feature or parameter is not as critical
as believed. This is important new information for the model. On the other hand,
if a predicted or modeled value varies substantially in comparison to the
parameter as it is slightly varied, then the accuracy of measurement of the critical
parameter assumes new importance. In sensitivity analysis, just as in all
modeling, this comparison of &#x201C;varying substantially&#x201D; should be measured with
significant digits, relative magnitudes, and rates of change. Here is another
area where expressing parameters in dimensionless groups is important
<span class="cite">[<a 
href="#Xlogan87">3</a>]</span>. In some areas of applied mathematics such as linear optimization
and statistics, a side effect of the solution method is that it produces
sensitivity parameters. In linear optimization, these are sometimes called the
shadow prices and these additional solution values should be used whenever
possible.
</p><!--l. 287--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-10000"></a>Interpretation and Refinement</h4>
<!--l. 289--><p class="noindent" >Finally the modelers must take the results from the previous steps and use them
to refine the interpretation and understanding of the real world situation. This
interpretation step is represented in the diagram by connection between the boxes
labeled 4 and 1, completing the cycle of modeling. For example, if the
situation is modeling motion, then examining results may show that the
predicted motion is faster than measured, or that the object does not
travel as far as the model predicts. Then it may be that the model does
not include the effects of friction, and so friction should be incorporated
into a new model. At this step, the modeler has to be open and honest
in assessing the strengths and weaknesses of the model. It also requires
                                                                          

                                                                          
an improved understanding of the real world situation to include the
correct new elements and hypotheses to correct the discrepancies in the
results.
</p><!--l. 303--><p class="indent" >   The step between stages 4 and 1 may suggest new processes, or experimental
conditions to alter the model. If the problem suggests changes then those
changes should be implemented and tested in another cycle in the modeling
process.
</p><!--l. 308--><p class="indent" >   A good summary of the modeling process is that it is an intense and
structured application of &#x201C;critical thinking&#x201D;. Sophistication of mathematical
techniques is not always necessary, the mathematics connecting steps 2 and 3 or
potentially steps 3 and 4 may only be arithmetic. The key to good modeling is the
critical thinking that occurs between steps 1 and 2, steps 3 and 4, and 4 and 1. If
a model does not fit into this paradigm, it probably does not meet the criteria for
a good model.
</p><!--l. 317--><p class="indent" >   Good mathematical modeling, like good critical thinking, does not arise
automatically or naturally. The craft of creating, solving, using, and interpreting a
mathematical model must be practiced and developed. The structured approach
to modeling helps distinguish the distinct steps, each requiring separate
intellectual skills. It also provides a framework for developing and explaining a
mathematical model.
</p><!--l. 324--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-11000"></a>A classification of mathematical models</h4>
<!--l. 326--><p class="noindent" >The goal of mathematical modeling is to represent a real-world situation in a way
which is a close approximation, even ideally exact, with a mathematical structure
which is still solvable. This represents the interplay between the mathematics
occurring between steps 1 and 2 and steps 2 and 3. Then we can classify models
based on this interplay.
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-11002x1">Exact models with exact solutions.
      </li>
      <li 
  class="enumerate" id="x1-11004x2">Exact models with approximate solutions.
      </li>
      <li 
  class="enumerate" id="x1-11006x3">Approximate models with exact solutions.
                                                                          

                                                                          
      </li>
      <li 
  class="enumerate" id="x1-11008x4">Approximate models with approximate solutions.</li></ol>
<!--l. 342--><p class="indent" >   Exact models are uncommon because only rarely do we know physical
representations well enough to claim to represent situations exactly. Exact
representations typically occur when in discrete situations where we can
enumerate all cases and represent them mathematically.
</p>
   <div class="newtheorem">
<!--l. 347--><p class="noindent" ><span class="head">
<span 
class="cmti-12">Example.</span>  </span>The average value of the pennies, nickles, dimes and quarters in
Paula&#x2019;s purse is 20 cents (the average value is the total money value divided
by the number of coins.) If she had one more quarter, the average value would
be 21 cents. What coins does Paula have in her purse?
</p><!--l. 354--><p class="indent" >   The mathematical model is to let
<!--l. 354--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>V</mi> </mrow></math> be the total value
of the coins and <!--l. 355--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>c</mi></mrow></math>
be the number of coins. Write two equations in two unknowns
</p><!--tex4ht:inline--><!--l. 360--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="block" ><mtable 
columnalign="left" class="align-star">
                          <mtr><mtd 
columnalign="right" class="align-odd"><mi 
>V</mi><mo 
class="MathClass-bin">&#x2215;</mo><mi 
>c</mi></mtd>                                       <mtd 
class="align-even"> <mo 
class="MathClass-rel">=</mo> <mn>2</mn><mn>0</mn><mspace width="2em"/></mtd>                           <mtd 
columnalign="right" class="align-label"></mtd>                          <mtd 
class="align-label">
                          <mspace width="2em"/></mtd></mtr><mtr><mtd 
columnalign="right" class="align-odd"><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>V</mi> <mo 
class="MathClass-bin">+</mo> <mn>2</mn><mn>5</mn></mrow><mo 
class="MathClass-close">)</mo></mrow><mo 
class="MathClass-bin">&#x2215;</mo><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>c</mi> <mo 
class="MathClass-bin">+</mo> <mn>1</mn></mrow><mo 
class="MathClass-close">)</mo></mrow></mtd>                          <mtd 
class="align-even"> <mo 
class="MathClass-rel">=</mo> <mn>2</mn><mn>1</mn><mo 
class="MathClass-punc">.</mo><mspace width="2em"/></mtd>                          <mtd 
columnalign="right" class="align-label"></mtd>                          <mtd 
class="align-label">
   <mspace width="2em"/></mtd></mtr></mtable></math>
<!--l. 361--><p class="noindent" >The solution is <!--l. 361--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mn>3</mn></mrow></math>
quarters and <!--l. 361--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mn>1</mn></mrow></math>
nickel. Because of the discrete nature and fixed value of the coins, and the
simplicity of the equations, an exact model has an exact solution.
                                                                          

                                                                          
</p>
   </div>
<!--l. 366--><p class="indent" >   Approximate models are much more typical.
</p>
   <div class="newtheorem">
<!--l. 368--><p class="noindent" ><span class="head">
<span 
class="cmti-12">Example.</span>  </span>Modeling the motion of a pendulum is a classic problem in applied
mathematics.  Galileo  first  modeled  the  pendulum  mathematically  and
mathematicians and physicists still investigate more sophisticated models.
Modeling the pendulum is considered in most books on applied mathematics
and  differential  equations,  for  example  <span class="cite">[<a 
href="#Xlin74">2</a>]</span>.  An  overview  of  modeling  the
pendulum appears in <span class="cite">[<a 
href="#Xsangwin11">5</a>]</span>.
</p>
   <hr class="figure" /><div class="figure" 
><table class="figure"><tr class="figure"><td class="figure" 
><a 
 id="x1-110092"></a><img 
src="pendulum3.png" alt="PIC"  
 />
<br /> <table class="caption" 
><tr style="vertical-align:baseline;" class="caption"><td class="id">Figure&#x00A0;2: </td><td  
class="content">Schematic diagram of a pendulum</td></tr></table><!--tex4ht:label?: x1-110092 -->
   </td></tr></table></div><hr class="endfigure" />
<!--l. 386--><p class="indent" >   As a physically inclusive model of the pendulum, consider the general
elastic pendulum shown in Figure&#x00A0;<a 
href="#x1-110092">2<!--tex4ht:ref: fig:pendulum --></a>. The pendulum is a heavy bob
<!--l. 388--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>B</mi></mrow></math> attached to
a pivot point <!--l. 389--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>P</mi></mrow></math>
by means of an elastic spring. The pendulum has at least 5 degrees of
freedom relative to its rest position. The pendulum can swing in the
<!--l. 391--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>x</mi></mrow></math>-<!--l. 391--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>y</mi></mrow></math>-<!--l. 391--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>z</mi></mrow></math>
spatial dimensions. The pendulum can rotation torsionally around the axis of the
spring <!--l. 393--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>P</mi><mi 
>B</mi></mrow></math>.
Finally, the pendulum can lengthen and shorten along the axis
<!--l. 394--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>P</mi><mi 
>B</mi></mrow></math>.
Although we usually think of a pendulum as the short rigid rod in a clock, some
pendula move in all these degrees of freedom, for example a huge construction
crane.
</p><!--l. 398--><p class="indent" >   We usually simplify the modeling with assumptions:
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-11011x1">The pendulum is a rigid rod so that it does not lengthen or shorten,
      nor does it rotate torsionally.
      </li>
                                                                          

                                                                          
      <li 
  class="enumerate" id="x1-11013x2">All the mass is concentrated in the bob <!--l. 404--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>B</mi></mrow></math>,
      that is, the pendulum rod is massless.
      </li>
      <li 
  class="enumerate" id="x1-11015x3">The motion occurs only in one plane, so that there is only one degree of
      freedom, measured by the angle <!--l. 408--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>&#x03B8;</mi></mrow></math>.
      </li>
      <li 
  class="enumerate" id="x1-11017x4">There is no air resistance or friction in the bearing at <!--l. 410--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>P</mi></mrow></math>.
      </li>
      <li 
  class="enumerate" id="x1-11019x5">The only forces on the pendulum are at the contact point <!--l. 413--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>P</mi></mrow></math>
      and the force of gravity due to the earth.
      </li>
      <li 
  class="enumerate" id="x1-11021x6">The pendulum is small relative to the earth so that gravity acts in the
      &#x201C;down&#x201D; direction only and is constant.</li></ol>
<!--l. 419--><p class="noindent" >Then with standard physical modeling with Newton&#x2019;s laws of motion,
we obtain the differential equation for the pendulum angle
<!--l. 420--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>&#x03B8;</mi></mrow></math> with
respect to vertical
</p>
   <div class="math-display"><!--l. 422--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="block" ><mrow 
>
                       <mi 
>m</mi><mi 
>l</mi><msup><mrow 
><mi 
>&#x03B8;</mi></mrow><mrow 
><mi 
>&#x2032;</mi><mi 
>&#x2032;</mi></mrow></msup 
> <mo 
class="MathClass-bin">+</mo> <mi 
>m</mi><mi 
>g</mi><mo class="qopname"> sin</mo><!--nolimits--> <mi 
>&#x03B8;</mi> <mo 
class="MathClass-rel">=</mo> <mn>0</mn><mo 
class="MathClass-punc">,</mo><mspace width="2em" class="qquad"/><mi 
>&#x03B8;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mn>0</mn></mrow><mo 
class="MathClass-close">)</mo></mrow> <mo 
class="MathClass-rel">=</mo> <msub><mrow 
><mi 
>&#x03B8;</mi></mrow><mrow 
>
<mn>0</mn></mrow></msub 
><mo 
class="MathClass-punc">,</mo><msup><mrow 
><mi 
>&#x03B8;</mi></mrow><mrow 
><mi 
>&#x2032;</mi></mrow></msup 
><mrow ><mo 
class="MathClass-open">(</mo><mrow><mn>0</mn></mrow><mo 
class="MathClass-close">)</mo></mrow> <mo 
class="MathClass-rel">=</mo> <msub><mrow 
><mi 
>v</mi></mrow><mrow 
>
<mn>0</mn></mrow></msub 
><mo 
class="MathClass-punc">.</mo>
</mrow></math></div>
<!--l. 425--><p class="nopar" > Note the application of the math modeling process moving from step 1 to step 2
with the identification of important variables, the hypotheses that simplify, and
the application of physical laws. It is clear that already the differential equation
describing the pendulum is an approximate model.
                                                                          

                                                                          
</p><!--l. 431--><p class="indent" >   Nevertheless, this nonlinear differential equation cannot be solved in terms of
elementary functions. It can be solved in terms of a class of higher transcendental
functions known as elliptic integrals, but in practical terms that is equivalent to
not being able to solve the equation analytically. There are two alternatives, either
to solve the equation numerically or to reduce the equation further to a yet
simpler form.
</p><!--l. 439--><p class="indent" >   For small angles <!--l. 439--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mo class="qopname">sin</mo><!--nolimits--> <mi 
>&#x03B8;</mi> <mo 
class="MathClass-rel">&#x2248;</mo> <mi 
>&#x03B8;</mi></mrow></math>
so if the pendulum does not have large oscillations the model becomes
</p>
   <div class="math-display"><!--l. 441--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="block" ><mrow 
>
                         <mi 
>m</mi><mi 
>l</mi><msup><mrow 
><mi 
>&#x03B8;</mi></mrow><mrow 
><mi 
>&#x2032;</mi><mi 
>&#x2032;</mi></mrow></msup 
> <mo 
class="MathClass-bin">+</mo> <mi 
>m</mi><mi 
>g</mi><mi 
>&#x03B8;</mi> <mo 
class="MathClass-rel">=</mo> <mn>0</mn><mo 
class="MathClass-punc">,</mo><mspace width="2em" class="qquad"/><mi 
>&#x03B8;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mn>0</mn></mrow><mo 
class="MathClass-close">)</mo></mrow> <mo 
class="MathClass-rel">=</mo> <msub><mrow 
><mi 
>&#x03B8;</mi></mrow><mrow 
>
<mn>0</mn></mrow></msub 
><mo 
class="MathClass-punc">,</mo><msup><mrow 
><mi 
>&#x03B8;</mi></mrow><mrow 
><mi 
>&#x2032;</mi></mrow></msup 
><mrow ><mo 
class="MathClass-open">(</mo><mrow><mn>0</mn></mrow><mo 
class="MathClass-close">)</mo></mrow> <mo 
class="MathClass-rel">=</mo> <msub><mrow 
><mi 
>v</mi></mrow><mrow 
>
<mn>0</mn></mrow></msub 
><mo 
class="MathClass-punc">.</mo>
</mrow></math></div>
<!--l. 444--><p class="nopar" > This differential equation is analytically solvable with standard methods
yielding
</p>
   <div class="math-display"><!--l. 446--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="block" ><mrow 
>
                                     <mi 
>&#x03B8;</mi><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>t</mi></mrow><mo 
class="MathClass-close">)</mo></mrow> <mo 
class="MathClass-rel">=</mo> <mi 
>A</mi><mo class="qopname"> cos</mo><!--nolimits--><mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>&#x03C9;</mi><mi 
>t</mi> <mo 
class="MathClass-bin">+</mo> <mi 
>&#x03D5;</mi></mrow><mo 
class="MathClass-close">)</mo></mrow>
</mrow></math></div>
<!--l. 448--><p class="nopar" > for appropriate constants <!--l. 448--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>A</mi></mrow></math>,
<!--l. 448--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>&#x03C9;</mi></mrow></math>, and
<!--l. 448--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>&#x03D5;</mi></mrow></math>
                                                                          

                                                                          
derived from the constants of the model. This is definitely an
exact solution to an approximate model. The approximation of
<!--l. 450--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mo class="qopname">sin</mo><!--nolimits--> <mi 
>&#x03B8;</mi></mrow></math> by
<!--l. 451--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>&#x03B8;</mi></mrow></math> is
made specifically so that the differential equation is explicitly solvable in
elementary functions. The solution to the differential equation is the process that
leads from step 2 to step 3 in the modeling process. The analysis necessary to
measure the accuracy of the exact solution compared to the physical motion is
difficult. The measurement of the accuracy would be the process of moving from
step 2 to step 3 in the cycle of modeling.
</p><!--l. 460--><p class="indent" >   For a clock maker the accuracy of the solution is important. There are
<!--l. 461--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mn>8</mn><mn>6</mn><mo 
class="MathClass-punc">,</mo> <mn>4</mn><mn>0</mn><mn>0</mn></mrow></math>
seconds in a day, so an error on the order of even 1 part in 10,000 for a physical
pendulum oscillating once per second accumulates unacceptably. This error
concerned physicists such as C. Huygens who created advanced pendula with a
period independent of the amplitude. This illustrates step 3 to step 4 and the next
modeling cycle.
</p><!--l. 470--><p class="indent" >   Models of oscillation, including the pendulum, have been a central paradigm in
applied mathematics for centuries. Here we use the pendulum model to illustrate
the modeling process leading to an approximate model with an exact
solution.
</p>
   </div>
<!--l. 476--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-12000"></a>An example from physical chemistry</h4>
<!--l. 478--><p class="noindent" >This section illustrates the cycle of mathematical modeling with a simple example
from physical chemistry. This simple example provides a powerful analogy to the
role of mathematical modeling in mathematical finance. The historical order of
discovery is slightly modified to illustrate the idealized modeling cycle. Scientific
progress rarely proceeds in simple order.
</p><!--l. 485--><p class="indent" >   Scientists observed that diverse gases such as air, water vapor, hydrogen, and
carbon dioxide all behave predictably and similarly. After many observations,
scientists derived empirical relations such as Boyle&#x2019;s law, and the law of Charles
and Gay-Lussac about the gas. These laws express relations among the volume
                                                                          

                                                                          
<!--l. 491--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>V</mi> </mrow></math>, the pressure
<!--l. 491--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>P</mi></mrow></math>, the amount
<!--l. 491--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>n</mi></mrow></math>, and the
temperature. <!--l. 492--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>T</mi></mrow></math>
of the gas.
</p><!--l. 494--><p class="indent" >   In classical theoretical physics, we can define an <span 
class="cmti-12">ideal gas </span>by making the
following assumptions <span class="cite">[<a 
href="#Xhalliday66">1</a>]</span>:
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-12002x1">A  gas  consists  of  particles  called  molecules  which  have  mass,  but
      essentially have no volume, so the molecules occupy a negligibly small
      fraction of the volume occupied by the gas.
      </li>
      <li 
  class="enumerate" id="x1-12004x2">The molecules can move in any direction with any speed.
      </li>
      <li 
  class="enumerate" id="x1-12006x3">The number of molecules is large.
      </li>
      <li 
  class="enumerate" id="x1-12008x4">No appreciable forces act on the molecules except during a collision.
      </li>
      <li 
  class="enumerate" id="x1-12010x5">The collisions between molecules and the container are elastic, and
      of  negligible  duration  so  both  kinetic  energy  and  momentum  are
      conserved.
      </li>
      <li 
  class="enumerate" id="x1-12012x6">All molecules in the gas are identical.</li></ol>
<!--l. 518--><p class="indent" >   From this limited set of assumptions about theoretical entities called molecules
physicists can derive the equation of state for an ideal gas in terms of the 4
quantifiable elements of volume, pressure, amount, and temperature. The <span 
class="cmti-12">equation</span>
<span 
class="cmti-12">of state </span>or <span 
class="cmti-12">ideal gas law </span>is
</p>
                                                                          

                                                                          
   <div class="math-display"><!--l. 526--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="block" ><mrow 
>
                                          <mi 
>P</mi><mi 
>V</mi> <mo 
class="MathClass-rel">=</mo> <mi 
>n</mi><mi 
>R</mi><mi 
>T</mi><mo 
class="MathClass-punc">.</mo>
</mrow></math></div>
<!--l. 528--><p class="nopar" > where <!--l. 528--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>R</mi></mrow></math>
is a measured constant, called the universal gas constant. This gives a simple
algebraic equation relating the 4 quantifiable elements describing a gas. The
equation of state or ideal gas law predicts very well the properties of gases
under the wide range of pressures, temperatures, masses and volumes
commonly experienced in everyday life. The ideal gas law predicts with
accuracy necessary for safety engineering the pressure and temperature in
car tires and commercial gas cylinders. This level of prediction works
even for gases we know do not satisfy the assumptions, such as air, which
chemistry tells us is composed of several kinds of molecules which have
volume and do not experience completely elastic collisions because of
intermolecular forces. We know the mathematical model is wrong, but it is still
useful.
</p><!--l. 542--><p class="indent" >   Nevertheless, scientists soon discovered that the assumptions of an ideal gas
predict that the difference in the constant-volume specific heat and the
constant-pressure specific heat of gases should be the same for all gases, a
prediction that scientists observe to be false. The simple ideal gas theory works
well for monatomic gases, such as helium, but does not predict so well for more
complex gases. This scientific observation now requires additional assumptions,
specifically about the shape of the molecules in the gas. The derivation of the
relationship for the observable in a gas is now more complex, requiring more
mathematical techniques.
</p><!--l. 553--><p class="indent" >   Moreover, under extreme conditions of low temperatures or high pressures,
scientists observe new behaviors of gases. The gases condense into liquids,
pressure on the walls drops and the gases no longer behave according to the
relationship predicted by the ideal gas law. We cannot neglect these deviations
                                                                          

                                                                          
from ideal behavior in accurate scientific or engineering work. We now have to
admit that under these extreme circumstances we can no longer ignore
the size of the molecules, which do occupy some appreciable volume. We
also must admit that intermolecular forces must be considered. The two
effects just described can be incorporated into a modified equation of state
proposed by J.D. van der Waals in 1873. Van der Waals&#x2019; equation of state
is:
</p>
   <div class="math-display"><!--l. 569--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="block" ><mrow 
>
                                   <mfenced separators="" 
open="("  close=")" ><mrow><mi 
>P</mi> <mo 
class="MathClass-bin">+</mo> <mfrac><mrow 
><mi 
>n</mi><mi 
>a</mi></mrow> 
<mrow 
><msup><mrow 
><mi 
>V</mi> </mrow><mrow 
><mn>2</mn></mrow></msup 
></mrow></mfrac></mrow></mfenced> <mrow ><mo 
class="MathClass-open">(</mo><mrow><mi 
>V</mi> <mo 
class="MathClass-bin">&#x2212;</mo> <mi 
>b</mi></mrow><mo 
class="MathClass-close">)</mo></mrow> <mo 
class="MathClass-rel">=</mo> <mi 
>R</mi><mi 
>T</mi>
</mrow></math></div>
<!--l. 571--><p class="nopar" > The additional constants <!--l. 571--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>a</mi></mrow></math>
and <!--l. 571--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>b</mi></mrow></math>
represent the new elements of intermolecular attraction and volume effects respectively.
If <!--l. 573--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>a</mi></mrow></math>
and <!--l. 573--><math 
 xmlns="http://www.w3.org/1998/Math/MathML" display="inline" ><mrow 
><mi 
>b</mi></mrow></math>
are small because we are considering a monatomic gas under ordinary conditions,
the Van der Waals equation of state can be well approximated by the ideal gas
law. Otherwise we must use this more complicated relation for engineering our
needs with gases.
</p><!--l. 578--><p class="indent" >   Physicists now realize that because of the complex nature of the intermolecular
forces, a real gas cannot be rigorously described by any simple equation of state.
We can honestly say that the assumptions of the ideal gas are not correct, yet are
sometimes useful. Likewise, the predictions of the van der Waals equation of state
describe quite accurately the behavior of carbon dioxide gas in appropriate
conditions. Yet for very low temperatures, carbon dioxide deviates from even
these modified predictions because we know that the van der Waals model of the
gas is wrong. Even this improved mathematical model is wrong, but it still is
useful.
                                                                          

                                                                          
</p><!--l. 589--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-13000"></a>An example from mathematical finance</h4>
<!--l. 591--><p class="noindent" >For modeling mathematical finance, we make a limited number of idealized
assumptions about securities markets. We start from empirical observations of
economists about supply and demand and the role of prices as a quantifiable
element relating them. We ideally assume that
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-13002x1">The market has a very large number of identical, rational traders.
      </li>
      <li 
  class="enumerate" id="x1-13004x2">All traders always have complete information about all assets they are
      trading.
      </li>
      <li 
  class="enumerate" id="x1-13006x3">Prices vary randomly with some continuous probability distribution.
      </li>
      <li 
  class="enumerate" id="x1-13008x4">Trading transactions take negligible time.
      </li>
      <li 
  class="enumerate" id="x1-13010x5">Trading transactions can be made in any amounts.</li></ol>
<!--l. 610--><p class="noindent" >These assumptions are very similar to the assumptions about an ideal gas. From the
assumptions we will be able to make some standard economic arguments to derive
some interesting relationships about option prices. These relationships can help us
manage risk, and speculate intelligently in typical markets. However, caution is
necessary. In discussing the economic collapse of 2008-2009, blamed in part on the
overuse or even abuse of mathematical models of risk, Valencia <span class="cite">[<a 
href="#Xvalencia10">6</a>]</span> says
&#x201C;Trying ever harder to capture risk in mathematical formulae can be
counterproductive if such a degree of accuracy is intrinsically unobtainable.&#x201D; If the
dollar amounts get very large (so that rationality no longer holds!), or
only a few traders are involved, or sharp jumps in prices occur, or the
trades come too rapidly for information to spread effectively, we must
proceed with caution. The observed financial outcomes may deviate from
predicted ideal behavior in accurate scientific or economic work, or financial
engineering.
                                                                          

                                                                          
</p><!--l. 627--><p class="indent" >   We must then alter our assumptions, re-derive the quantitative relationships,
perhaps with more sophisticated mathematics or introducing more quantities and
begin the cycle of modeling again.
</p><!--l. 631--><p class="noindent" >
</p>
   <h4 class="likesubsectionHead"><a 
 id="x1-14000"></a>Sources</h4>
<!--l. 633--><p class="noindent" >Some of the ideas about mathematical modeling are adapted from the article by
Valencia <span class="cite">[<a 
href="#Xvalencia10">6</a>]</span> and the book <span 
class="cmti-12">When Genius Failed </span>by Roger Lowenstein. The
classification of mathematical models and solutions is adpated from Sangwin, <span class="cite">[<a 
href="#Xsangwin11">5</a>]</span>.
The example of an exact model with an exact solution is from the 2009 American
Mathematics Competition 8.
</p><!--l. 643--><p class="indent" >   _______________________________________________________________________________________________
</p><!--l. 645--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/solveproblems.png" alt="Problems to Work"  
 />
</p>
   <h3 class="likesectionHead"><a 
 id="x1-15000"></a>Problems to Work for Understanding</h3>
<!--l. 647--><p class="noindent" >
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-15002x1">A ladder stand with one end on the floor and the other against a wall.
      It slides along the floor and down the wall. If a cat is sitting in the
      middle of the ladder, what curve does it move along?
      <!--l. 654--><p class="noindent" >Create and solve a mathematical model for this situation, enumerating
      explicitly the simplifying assumptions that you make to create and
      solve the model.
      </p></li>
      <li 
  class="enumerate" id="x1-15004x2">How many jelly beans fill a 1-liter jar?
      <!--l. 660--><p class="noindent" >Create and solve a mathematical model for this situation, enumerating
      explicitly the simplifying assumptions that you make to create and
      solve the model.
                                                                          

                                                                          
      </p></li>
      <li 
  class="enumerate" id="x1-15006x3">How many flat toothpicks would fit on the surface of a sheet of poster
      board?
      <!--l. 667--><p class="noindent" >Create and solve a mathematical model for this situation, enumerating
      explicitly the simplifying assumptions that you make to create and
      solve the model.
      </p></li>
      <li 
  class="enumerate" id="x1-15008x4">If your life earnings were doled out to you at a certain rate per hour
      for every hour of your life, how much is your time worth?
      <!--l. 675--><p class="noindent" >Create and solve a mathematical model for this situation, enumerating
      explicitly the simplifying assumptions that you make to create and
      solve the model.</p></li></ol>
<!--l. 679--><p class="noindent" >______________________________________________________________________________
</p><!--l. 681--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/books.png" alt="Books"  
 />
</p>
   <h3 class="likesectionHead"><a 
 id="x1-16000"></a>Reading Suggestion:</h3>
<!--l. 1--><p class="noindent" >
</p>
   <h3 class="likesectionHead"><a 
 id="x1-17000"></a>References</h3>
<!--l. 1--><p class="noindent" >
   </p><div class="thebibliography">
   <p class="bibitem" ><span class="biblabel">
 [1]<span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span><a 
 id="Xhalliday66"></a>D.&#x00A0;Halliday and R.&#x00A0;Resnick. <span 
class="cmti-12">Physics</span>. J. Wiley and Sons, 1966. QC21
   .R42 1966.
   </p>
   <p class="bibitem" ><span class="biblabel">
 [2]<span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span><a 
 id="Xlin74"></a>C.C. Lin and Lee&#x00A0;A. Segel.   <span 
class="cmti-12">Mathematics applied to deterministic</span>
   <span 
class="cmti-12">problems in the natural sciences</span>. Macmillan, 1974. QA37.2 .L55.
                                                                          

                                                                          
   </p>
   <p class="bibitem" ><span class="biblabel">
 [3]<span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span><a 
 id="Xlogan87"></a>J.&#x00A0;David Logan.   <span 
class="cmti-12">Applied Mathematics: A contemporary approach</span>.
   John Wiley and Sons, 1987. QA37.2 .L64 1987.
   </p>
   <p class="bibitem" ><span class="biblabel">
 [4]<span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span><a 
 id="Xlowenstein00"></a>Roger  Lowenstein.    <span 
class="cmti-12">When  Genius  Failed:  The  Rise  and  Fall  of</span>
   <span 
class="cmti-12">Long-Term Capital Management</span>.  Random House, 2000.  HG 4930 L69
   2000.
   </p>
   <p class="bibitem" ><span class="biblabel">
 [5]<span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span><a 
 id="Xsangwin11"></a>Chris Sangwin. Modelling the journey from elementary word problems
   to mathematical research. <span 
class="cmti-12">Notices of the American Mathematical Society</span>,
   58(10):1436&#x2013;1445, November 2011.
   </p>
   <p class="bibitem" ><span class="biblabel">
 [6]<span class="bibsp">&#x00A0;&#x00A0;&#x00A0;</span></span><a 
 id="Xvalencia10"></a>Matthew Valencia. The gods strike back. <span 
class="cmti-12">The Economist</span>, pages 3&#x2013;5,
   February 2010. popular history.
</p>
   </div>
<!--l. 696--><p class="noindent" >__________________________________________________________________________
</p><!--l. 698--><p class="indent" >   <img 
src="../../../../CommonInformation/Lessons/chainlink.png" alt="Links"  
 />
</p><!--l. 700--><p class="noindent" >
</p>
   <h3 class="likesectionHead"><a 
 id="x1-18000"></a>Outside Readings and Links:</h3>
<!--l. 701--><p class="noindent" >
      </p><ol  class="enumerate1" >
      <li 
  class="enumerate" id="x1-18002x1"><a 
href="http://www.youtube.com/watch?v=IqiZ0xso-F0" >Duke University Modeling Contest Team</a>. Accessed August 29, 2009</li></ol>
                                                                          

                                                                          
<!--l. 707--><p class="noindent" >__________________________________________________________________________
</p><!--l. 3--><p class="indent" >   <span 
class="cmr-10x-x-109">I check all the information on each page for correctness and typographical errors.</span>
<span 
class="cmr-10x-x-109">Nevertheless, some errors may occur and I would be grateful if you would alert me to</span>
<span 
class="cmr-10x-x-109">such errors. I make every reasonable effort to present current and accurate information</span>
<span 
class="cmr-10x-x-109">for public use, however I do not guarantee the accuracy or timeliness of information on</span>
<span 
class="cmr-10x-x-109">this website. Your use of the information from this website is strictly voluntary and at</span>
<span 
class="cmr-10x-x-109">your risk.</span>
</p><!--l. 12--><p class="indent" >   <span 
class="cmr-10x-x-109">I have checked the links to external sites for usefulness. Links to external websites</span>
<span 
class="cmr-10x-x-109">are provided as a convenience. I do not endorse, control, monitor, or guarantee the</span>
<span 
class="cmr-10x-x-109">information contained in any external website. I don&#x2019;t guarantee that the links are</span>
<span 
class="cmr-10x-x-109">active at all times. Use the links here with the same caution as you would all</span>
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class="cmr-10x-x-109">information on the Internet. This website reflects the thoughts, interests and opinions of</span>
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</p><!--l. 22--><p class="indent" >   <span 
class="cmr-10x-x-109">Information on this website is subject to change without notice.</span>
</p><!--l. 2--><p class="indent" >   Steve Dunbar&#x2019;s Home Page, <span class="obeylines-h"><span class="verb"><span 
class="cmtt-12">http://www.math.unl.edu/~sdunbar1</span></span></span>
</p><!--l. 4--><p class="indent" >   Email to Steve Dunbar, <span class="obeylines-h"><span class="verb"><span 
class="cmtt-12">sdunbar1</span><span 
class="cmtt-12">&#x00A0;at</span><span 
class="cmtt-12">&#x00A0;unl</span><span 
class="cmtt-12">&#x00A0;dot</span><span 
class="cmtt-12">&#x00A0;edu</span></span></span>
</p><!--l. 711--><p class="indent" >   Last modified: Processed from <span class="LATEX">L<span class="A">A</span><span class="TEX">T<span 
class="E">E</span>X</span></span>&#x00A0;source on December 28, 2011
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