Curve Fitting 2
|Column Tag:||Forth Forum
Curve Fitting, Part II
By Jörg Langowski, Chemical Engineer, Grenoble, France, MacTutor Editorial Board
After last month's refresher on accessing floating point routines from Forth, this column is now going to show you the main part of the curve fitter program.
Let's state our objective again: We have a series of data points (measurements) yi at certain time points ti. The measured data is supposed to follow some quantitative law, so that we can state a theoretical relationship between time t and data y:
The ai are parameters that determine the exact form of the function f.
Lets assume we have estimated initial values for the parameters ai° somehow so that they are not too far away from the true values. Then we need a method that creates some correction terms ai, which when added to the initial values give new, better estimates of the parameters ai':
As you could read in last month's column, the ai are eventually obtained from the solution of a system of linear equations, and we had defined the word gauss to implement the Gauss algorithm that solves such a system.
This month I am going to show you how one sets up the equations (example given for three parameters),
starting from the data and the initial estimate of the function that one wants to fit to it. The full details of the method are given in an appendix to this column.
At this point it is only important to know that the coefficients cij, as defined in last month's column, look like the following:
where N is the total number of data points and fk/ai is the first derivative of the theoretical function at the time tk with respect to the parameter ai.
The terms on the right hand side of the equations, bi, are:
Ri are the residuals (as defined last month),
the differences between the theoretical and measured values at the time points ti.
Therefore, the curve fitting algorithm will consist of the following major parts:
- one routine that calculates the theoretical function value f(ti), given a set of parameters (this will be the 'model' that you use to fit your data),
- one routine that calculates the derivative of this function with respect to one of the parameters ai,
- calculation of all the derivatives fk/ai with k ranging from 0 to (# of data points - 1) and i from 0 to (# of parameters - 1) and saving those derivatives in a matrix,
- computation of the coefficients cij and bi (and setting them up in a matrix),
- solution of the linear equation system thus obtained, giving correction values for the parameters ai,
- changing the parameters by the correction terms and repetition of the whole algorithm if the change is still larger than some predefined (small) number.
The algorithm is implemented in this month's program example (listing 1). The first part contains some additions to the floating point and Gauss algorithm routines that you've already seen last month. One bug had to be corrected in gauss, which left a number on the stack that was supposed to be dropped (added drop in italics in the listing). The floating point output routine has been slightly modified so that real numbers are always printed with one digit in front of the decimal.
In order to be able to check whether the iteration has been completed or not, we will have to compare real numbers, so first we define the
Floating point comparison operator
The SANE package provides a routine for the comparison of two floating point numbers. Four cases are distinguished and the processor status register flags set accordingly:
X N Z V C
x < y 1 1 0 0 1
x = y 0 0 1 0 0
x > y 0 0 0 0 0
unordered0 0 0 1 0
where the address of x is on top of the address of y on the stack.
The operation code for floating point comparison in SANE is 8, so we define
hex : f> 8 fp68k @sr 10 and ;
for comparing two real numbers on the stack. Bit 5 of the result (the X flag) is and-ed out, the reason being that this is the only one that is left unchanged after the SANE trap has been called and the Forth interpreter has taken over again. All the other flags cannot be used, so we won't be able to compare two real numbers for being equal. With 80-bit precision, however, such a test does not make much sense, you will almost never check for equality but rather if a number is less than one other or whether their difference is smaller than some predefined value.
The comparison for 'unorderedness', which sets the V flag, is also trashed by the Forth interpreter. This would only be important if we wanted to test for a NaN (Not a Number), which for instance results from a 0/0 division.
This leaves us with the X flag as the only one usable after the fp68k call. It is set when the real number whose address is on top of the stack is less than the number whose address is below it.
Random number generator - floating point version
For initializing the 'data points' as an input to the curve fitting program, we are going to use simulated data from the same function that we are fitting. We add some 'random noise' to it and need a random number generator for that. SANE contains a floating point random number generator, which computes from an 80-bit floating point input a new random 80-bit floating point number in the range 0 < x < 231-1. We want a number between 0 and 1 (for convenience) so the word ranf scales this number after calling the random number routine. ranf leaves the address of the result on the stack. For initializing the random number generator with an arbitrary seed, ranset is defined.
You will notice one important concept in the definition of ranf and ranset: both words operate on variables (rr, rs and sf) that are axed after the definition is completed. The variables are erased from the vocabulary that way and stay local to the random number routines. This is the way the 'nameless' tokens are created that you read about some issues ago.
The function to be fitted is defined as the word func. 50 bytes are reserved for the array par, so that at maximum 5 parameters (extended precision) can be used in the function. The data points are stored in the single precision arrays xdat and ydat. init_pars initializes the parameters to some arbitrary values, in this case par = 1.0, par = 2.0, and par = -0.1. Calling func with these values, init then creates a set of simulated data (including random noise).
deriv calculates the first derivatives of the function with respect to the parameters from differences,
This definition, too, uses the local variables da1, da2, da3 and da4, which are axed afterwards.
make_derivmat computes all necessary derivative values and sets them up in a single precision matrix. This matrix is then used by the word make_resmat to compute the sums that make up the coefficient matrix. For the right-hand-side coefficients one also needs the residuals, which are calculated and stored into a matrix by residuals.
One iteration of the curve fitting process is done by the word one_iter, which sets up the derivative matrix and computes the residuals by calling the appropriate words, prints the sum of error squares (so you can check the quality of the fit) then sets up the coefficient matrix and calls gauss to solve the linear equation system. The solution is stored in the array delta; these are the correction terms that have to be added to the parameters to get improved estimates. new_pars does this correction and prints out the values of the new parameters, leaving false (zero) on the stack if any parameter has changed by more than one part in 10-5.
The actual curve fitter, nlsqfit, then loops through the iteration until the best fit is obtained.
You can check the fitting process by calling init first and then, for instance, setting par = 2.0, par = 1.0, par = -0.05:
two par x2x one par 10+ x2x
two par 20 + f/
and start nlsqfit. This will bring you back close to the simulated values, par = 1.0, par = 2.0, and par = -0.1 in about 4 to 5 iterations. The fitted values will not be exactly equal to the simulated ones because of the random noise added to the data.
So far, this is only a skeleton of a curve fitting program because we cannot input floating point numbers manually or from the clipboard (e.g. it would be nice to transfer data from a spreadsheet); also a graphical output will be needed to display the data points and the fitted curve. Next column will deal with those problems.
Listing 1: Non-linear least squares curve fitting routine
( © 1985 J.Langowski by MacTutor )
( Note that this is not stand-alone but needs some definitions from last
month's example. Only the changed parts are printed here )
: f> 8 fp68k @sr 10 and ; : fabs f fp68k ;
: lnx 0 elems68k ; : log2x 2 elems68k ;
: ln1x 4 elems68k ; : log21x 6 elems68k ;
: expx 8 elems68k ; : exp2x a elems68k ;
: exp1x c elems68k ; : exp21x e elems68k ;
: x^i 8010 elems68k ; : x^y 8012 elems68k ;
: compoundx c014 elems68k ;
: annuityx c016 elems68k ;
: sinx 18 elems68k ; : cosx 1a elems68k ;
: tanx 1c elems68k ; : atanx 1e elems68k ;
: randomx 20 elems68k ; decimal
: dec. ( float\format# -- )
zzformat ! zzformat swap zzs1 b2d
zzs1 dup w@ 255 > if ." -" else ." " then
dup 4+ count over 1 type ." ."
swap 1+ swap 1- type ( mantissa )
2+ w@ ( get exponent )
1 w* zzformat @ + 1-
." E" . ;
( define constants )
float one float -one float zero float two float four
1 sp@ one in2x drop -1 sp@ -one in2x drop
0 sp@ zero in2x drop
2 sp@ two in2x drop 4 sp@ four in2x drop
( define some floating accumulators)
float fa1 float fa2 float fa3 float fa4
( Gauss algorithm for linear equations)
float dg float fk float ee
variable nv variable coeff variable solution
( addresses for storing actual parameters)
: gauss ( z\x\n | --) nv ! 8- coeff ! solution !
nv @ 1- 0 do ( i-loop)
i dup coeff @ calc.offset dg s2x ( diag elem)
nv @ i 1+ do ( j-loop)
i j coeff @ calc.offset fk s2x dg fk f/
nv @ 1+ j do ( k-loop)
k i coeff @ calc.offset fa1 s2x
fk fa1 f* fa1 fneg ( -fk*x[i,k])
j i coeff @ calc.offset dup fa1 s+
fa1 swap x2s
nv @ dup 0 do i over coeff @ calc.offset fa1 s2x
fa1 solution @ i 4* + x2s loop drop
1 nv @ 1- do
i dup coeff @ calc.offset dg s2x
solution @ i 4* + ee s2x dg ee f/
0 i 1- do i j coeff @ calc.offset fa1 s2x
ee fa1 f* fa1 fneg
solution @ i 4* + dup fa1 s+ fa1 swap x2s
nv @ 0 do solution @ i 4* + fa1 s2x
i dup coeff @ calc.offset fa1 s/
fa1 solution @ i 4* + x2s
( declarations for curve fitter )
create ydat 400 allot create xdat 400 allot
create residues 400 allot
100 10 matrix derivmat 10 11 matrix resmat
3 constant npars 10 constant npts
create par 50 allot create delta 20 allot
float eps float errsum
1 sp@ eps in2x drop 10000 sp@ eps in/ drop
float onehundred 100 sp@ onehundred in2x drop
float ten 10 sp@ ten in2x drop
( define function )
: func ( x -- f[x] = par + par * exp[par*x] )
par 20 + over f* dup expx
par 10 + over f* par over f+ ;
: test 10 0 do i sp@ fa1 in2x . 2 spaces
fa1 func 10 dec. cr loop ;
: >fa1 fa1 s2x ;
one par x2x two par 10+ x2x
-one par 20 + x2x ten par 20 + f/ ;
( derivative, matrix of derivs )
float da1 float da2 float da3 float da4 ( local vars )
: deriv ( par \ x -- d-func/d-par at x )
dup da1 x2x da2 x2x dup da4 x2x eps da4 f*
da4 over f+ da2 func da3 x2x
da4 over 2dup f- f- da1 func da3 f-
da4 da3 f/ two da3 f/ da4 swap f+ da3 ;
axe da1 axe da2 axe da3 axe da4
npts 0 do npars 0 do
xdat j 4* + >fa1
par i 10 * + fa1 deriv j i derivmat x2s
loop loop ;
( calculate residuals )
zero errsum x2x
npts 0 do
xdat i 4* + >fa1 fa1 func ydat i 4* + swap s-
fa1 residues i 4* + x2s fa1 dup f* fa1 errsum f+
npts 0 do residues i 4* + >fa1 fa1 7 dec. cr loop ;
( make matrix of residuals )
npars 0 do npars 0 do zero fa1 x2x
npts 0 do
i k derivmat fa2 s2x i j derivmat fa2 s*
fa2 fa1 f+ loop
fa1 i j resmat x2s fa1 j i resmat x2s
npars 0 do zero fa1 x2x
npts 0 do
i j derivmat fa2 s2x residues i 4* + fa2 s*
fa2 fa1 f- loop
fa1 i npars resmat x2s loop ;
( calculate correction terms)
." sum of error squares: " errsum 7 dec. cr
make_resmat delta 0 0 resmat npars gauss ;
: new_pars 16 ( true if no significant changes )
npars 0 do par i 10 * +
delta i 4* + over s+
." par[" i . ." ] = " dup 7 dec. cr
delta i 4* + fa1 s2x fa1 f/
fa1 fabs eps fa1 f> and loop ;
( ranf, initialize data matrices )
float rr float rs float sf ( local to ranf )
1 31 scale 1 - sp@ sf in2x drop
: ranset rr x2x ;
: ranf rr randomx rr rs x2x sf rs f/ rs ;
axe rr axe rs axe sf
12345678 sp@ fa1 in2x drop fa1 ranset
80 ' npts !
: init npts 0 do i sp@ fa1 in2x 4*
xdat over + fa1 swap x2s
ydat over + fa1 func ranf fa2 x2x
ten fa2 f/ fa2 over f+ swap x2s
i . xdat over + >fa1 fa1 7 dec. 2 spaces
ydat + >fa1 fa1 7 dec. cr loop ;
( print matrices for debugging )
npts 0 do
npars 0 do j i derivmat >fa1 fa1 5 dec. loop
cr loop ;
npars 0 do
npars 1+ 0 do j i resmat >fa1 fa1 5 dec. loop
cr loop ;
( nonlinear fit, core routine)
: nlsqfit cr begin one_iter cr new_pars cr until ;
Appendix: Theoretical background of the curve fitting routine
We want to determine the values of the ai in such a way that the differences between the theoretical function and the measured yk values at times tk become a minimum. These differences are called the residuals rk:
rk = f (tk, a1, a2, a3, .... , an) - yk
and one usually tries to minimize the sum of the squared residuals of all data points.
Lets assume ri are the 'true' residuals that one obtains with the exact ai values. If we estimate the parameters by some initial values ai°, then 'computed' residuals
Rk = f (tk, a1°, a2°, a3°, .... , an°) - yk
can be calculated, which are usually larger than the true ones. To get a correction term that brings the ai° closer to the 'true' ai, one now linearly expands the function f around the estimated value:
f(tk,a1°,a2°,....,an°) + fk/a1(a1-a1°)
+ fk/a2 (a2-a2°)
. . . . .
The differences, (ai-ai°), are denoted by ai, now we can write
f(tk,a1,a2,....,an) - yk
f(tk,a1°,a2°,....,an°) - yk
+ fk/a1 a1 + fk/a2 a2
. . . . .
+ fk/an an
which gives us a relationship between the true and the computed residuals
rk Rk + fk/a1 a1 + fk/a2 a2
. . . . .
+ fk/an an .
It is the sum of the squares of the true residuals (N being the number of data points)
that has to be minimized with respect to changes in ai, this means all the derivatives Q/(ai) have to be zero simultaneously. When you evaluate the expressions for the Q/(ai) and set them to zero, you arrive at the equation system that was desribed in the main article.