NAME¶

math::calculus - Integration and ordinary differential equations

SYNOPSIS¶

package require Tcl 8.4

package require math::calculus 0.8.2

::math::calculus::integral begin end nosteps func

::math::calculus::integralExpr begin end nosteps expression

::math::calculus::integral2D xinterval yinterval func

::math::calculus::integral2D_accurate xinterval yinterval func

::math::calculus::integral3D xinterval yinterval zinterval func

::math::calculus::integral3D_accurate xinterval yinterval zinterval func

::math::calculus::qk15 xstart xend func nosteps

::math::calculus::qk15_detailed xstart xend func nosteps

::math::calculus::eulerStep t tstep xvec func

::math::calculus::heunStep t tstep xvec func

::math::calculus::rungeKuttaStep t tstep xvec func

::math::calculus::boundaryValueSecondOrder coeff_func force_func leftbnd rightbnd nostep

::math::calculus::solveTriDiagonal acoeff bcoeff ccoeff dvalue

::math::calculus::newtonRaphson func deriv initval

::math::calculus::newtonRaphsonParameters maxiter tolerance

::math::calculus::regula_falsi f xb xe eps

DESCRIPTION¶

This package implements several simple mathematical algorithms:

• The integration of a function over an interval
• The numerical integration of a system of ordinary differential equations.
• Estimating the root(s) of an equation of one variable.

The package is fully implemented in Tcl. No particular attention has been paid to the accuracy of the calculations. Instead, well-known algorithms have been used in a straightforward manner.

This document describes the procedures and explains their usage.

PROCEDURES¶

This package defines the following public procedures:

::math::calculus::integral begin end nosteps func

Determine the integral of the given function using the Simpson rule. The interval for the integration is [begin, end]. The remaining arguments are:

::math::calculus::integralExpr begin end nosteps expression

Similar to the previous proc, this one determines the integral of the given expression using the Simpson rule. The interval for the integration is [begin, end]. The remaining arguments are:

::math::calculus::integral2D xinterval yinterval func

::math::calculus::integral2D_accurate xinterval yinterval func

The commands integral2D and integral2D_accurate calculate the integral of a function of two variables over the rectangle given by the first two arguments, each a list of three items, the start and stop interval for the variable and the number of steps.

The command integral2D evaluates the function at the centre of each rectangle, whereas the command integral2D_accurate uses a four-point quadrature formula. This results in an exact integration of polynomials of third degree or less.

The function must take two arguments and return the function value.

::math::calculus::integral3D xinterval yinterval zinterval func

::math::calculus::integral3D_accurate xinterval yinterval zinterval func

The commands integral3D and integral3D_accurate are the three-dimensional equivalent of integral2D and integral3D_accurate. The function func takes three arguments and is integrated over the block in 3D space given by three intervals.

::math::calculus::qk15 xstart xend func nosteps

Determine the integral of the given function using the Gauss-Kronrod 15 points quadrature rule. The returned value is the estimate of the integral over the interval [xstart, xend]. The remaining arguments are:

::math::calculus::qk15_detailed xstart xend func nosteps

Determine the integral of the given function using the Gauss-Kronrod 15 points quadrature rule. The interval for the integration is [xstart, xend]. The procedure returns a list of four values:

The remaining arguments are:

::math::calculus::eulerStep t tstep xvec func

Set a single step in the numerical integration of a system of differential equations. The method used is Euler's.

::math::calculus::heunStep t tstep xvec func

Set a single step in the numerical integration of a system of differential equations. The method used is Heun's.

::math::calculus::rungeKuttaStep t tstep xvec func

Set a single step in the numerical integration of a system of differential equations. The method used is Runge-Kutta 4th order.

::math::calculus::boundaryValueSecondOrder coeff_func force_func leftbnd rightbnd nostep

Solve a second order linear differential equation with boundary values at two sides. The equation has to be of the form (the "conservative" form):

         d      dy     d


         -- A(x)--  +  -- B(x)y + C(x)y  =  D(x)


         dx     dx     dx

Ordinarily, such an equation would be written as:

             d2y        dy


         a(x)---  + b(x)-- + c(x) y  =  D(x)


             dx2        dx

The first form is easier to discretise (by integrating over a finite volume) than the second form. The relation between the two forms is fairly straightforward:

         A(x)  =  a(x)


         B(x)  =  b(x) - a'(x)


         C(x)  =  c(x) - B'(x)  =  c(x) - b'(x) + a''(x)

Because of the differentiation, however, it is much easier to ask the user to provide the functions A, B and C directly.

::math::calculus::solveTriDiagonal acoeff bcoeff ccoeff dvalue

Solve a system of linear equations Ax = b with A a tridiagonal matrix. Returns the solution as a list.

::math::calculus::newtonRaphson func deriv initval

Determine the root of an equation given by

    func(x) = 0

using the method of Newton-Raphson. The procedure takes the following arguments:

::math::calculus::newtonRaphsonParameters maxiter tolerance

Set the numerical parameters for the Newton-Raphson method:

::math::calculus::regula_falsi f xb xe eps

Return an estimate of the zero or one of the zeros of the function contained in the interval [xb,xe]. The error in this estimate is of the order of eps*abs(xe-xb), the actual error may be slightly larger.

The method used is the so-called regula falsi or false position method. It is a straightforward implementation. The method is robust, but requires that the interval brackets a zero or at least an uneven number of zeros, so that the value of the function at the start has a different sign than the value at the end.

In contrast to Newton-Raphson there is no need for the computation of the function's derivative.

Notes:

Several of the above procedures take the names of procedures as arguments. To avoid problems with the visibility of these procedures, the fully-qualified name of these procedures is determined inside the calculus routines. For the user this has only one consequence: the named procedure must be visible in the calling procedure. For instance:

    namespace eval ::mySpace {


       namespace export calcfunc


       proc calcfunc { x } { return $x }


    }


    #


    # Use a fully-qualified name


    #


    namespace eval ::myCalc {


       proc detIntegral { begin end } {


          return [integral $begin $end 100 ::mySpace::calcfunc]


       }


    }


    #


    # Import the name


    #


    namespace eval ::myCalc {


       namespace import ::mySpace::calcfunc


       proc detIntegral { begin end } {


          return [integral $begin $end 100 calcfunc]


       }


    }

Enhancements for the second-order boundary value problem:

• Other types of boundary conditions (zero gradient, zero flux)
• Other schematisation of the first-order term (now central differences are used, but upstream differences might be useful too).

EXAMPLES¶

Let us take a few simple examples:

Integrate x over the interval [0,100] (20 steps):

proc linear_func { x } { return $x }
puts "Integral: [::math::calculus::integral 0 100 20 linear_func]"

puts "Integral: [::math::calculus::integralExpr 0 100 20 {$x}]"

The differential equation for a dampened oscillator:

x'' + rx' + wx = 0

can be split into a system of first-order equations:

x' = y
y' = -ry - wx

Then this system can be solved with code like this:

proc dampened_oscillator { t xvec } {


   set x  [lindex $xvec 0]


   set x1 [lindex $xvec 1]


   return [list $x1 [expr {-$x1-$x}]]
}
set xvec   { 1.0 0.0 }
set t      0.0
set tstep  0.1
for { set i 0 } { $i < 20 } { incr i } {


   set result [::math::calculus::eulerStep $t $tstep $xvec dampened_oscillator]


   puts "Result ($t): $result"


   set t      [expr {$t+$tstep}]


   set xvec   $result
}

Suppose we have the boundary value problem:

    Dy'' + ky = 0


    x = 0: y = 1


    x = L: y = 0

This boundary value problem could originate from the diffusion of a decaying substance.

It can be solved with the following fragment:

   proc coeffs { x } { return [list $::Diff 0.0 $::decay] }


   proc force  { x } { return 0.0 }


   set Diff   1.0e-2


   set decay  0.0001


   set length 100.0


   set y [::math::calculus::boundaryValueSecondOrder \


      coeffs force {0.0 1.0} [list $length 0.0] 100]

BUGS, IDEAS, FEEDBACK¶

This document, and the package it describes, will undoubtedly contain bugs and other problems. Please report such in the category math :: calculus of the Tcllib Trackers [http://core.tcl.tk/tcllib/reportlist]. Please also report any ideas for enhancements you may have for either package and/or documentation.

When proposing code changes, please provide unified diffs, i.e the output of diff -u.

Note further that attachments are strongly preferred over inlined patches. Attachments can be made by going to the Edit form of the ticket immediately after its creation, and then using the left-most button in the secondary navigation bar.

SEE ALSO¶

romberg

KEYWORDS¶

calculus, differential equations, integration, math, roots

CATEGORY¶

Mathematics

COPYRIGHT¶

Copyright (c) 2002,2003,2004 Arjen Markus