ppalldem.html

演示matlab曲线拟和与插直的基本方法

fnplt(pp,[breaks(3),breaks(4)+1],'m',1.8)
lp1 = length(breaks);
xb = repmat(breaks,3,1);
yb = repmat([2;-2.2;NaN],1,lp1);
plot(xb(:),yb(:),'r')
title('a pp made up of three quadratic polynomials, i.e., l=3=k')
axis([-1 7 -2.5 2.3])
hold off

%%
% With this, the precise description of our  pp  in terms of the break
% sequence BREAKS and the coefficient array COEFS is
%
%  pp(t) = polyval( coefs(j,:), t-breaks(j) )  for breaks(j) <= t < breaks(j+1)
%
% where, to recall,
%
%   polyval(a,x)  equals  a(1)*x^(k-1) + a(2)*x^(k-2) + ... + a(k)*x^0 .
%
% In the above picture, BREAKS(1) is  0, and COEFS(1,:) equals
% [-1/2  0  0], while BREAKS(3) is 4, and COEFS(3,:) equals  [ 0  1  -1] .
% For  t  not in [BREAKS(1) .. BREAKS(l+1)),  pp(t)  is defined by
% extending the first, resp. last, polynomial piece.

%%
% A pp is usually constructed through a process of interpolation or
% approximation. But it is also possible to make one up in ppform from
% scratch, using  PPMAK( BREAKS, COEFS ). E.g., the above pp can be
% obtained by the statement
%
%   fn = ppmak( [0 1 4 6],  [1/2 0 0   -1/2 1 1/2   0 1 -1] );
%
% This stores, in FN, a complete description of this pp function in the
% so-called  ppform .
%
% Various M-files in the toolbox can operate on this form. The next slides
% show some examples.

fn = ppmak( [0 1 4 6], [1/2 0 0 -1/2 1 1/2 0 1 -1] );

%%
% Evaluation:

fnval( fn , -1:7 )

%%
% Differentiation:
% Note that  the derivative is continuous at 1 but discontinuous at  4 .
% Also note that, by default, FNPLT plots a ppform on its  b a s i c
%  i n t e r v a l , i.e., on the interval [ BREAKS(1)  ..  BREAKS(end) ] .

hold on
dfn = fnder ( fn );
fnplt( dfn , 'jumps','y', 3)
title(' a pp and its first derivative')
hold off

%%
% Differentiation (continued):
%
%   ddfn = fnder( fn, 2 );  fnplt( ddfn , 'j', 'k', 1.6)
%
% The second derivative (shown here in black) is piecewise constant.
%
% Note that differentiation via FNDER is done separately for each polynomial
% piece. E.g., although the first derivative (yellow) has a jump discontinuity
% across 4 , the second derivative is not infinite there.  This has
% consequences when we integrate the second derivative, on the next slide.

hold on
ddfn = fnder( fn, 2 );
fnplt( ddfn ,'j', 'k', 1.6)
title('a pp and its first derivative, and its second derivative')
hold off

%%
% Integration:
%
%   iddfn = fnint( ddfn );  fnplt( iddfn, 'c', .5)
%
% Note that integration of the second derivative does recover the first
% derivative, REPLACE_WITH_DASH_DASH except for the jump across 4 which cannot be recovered
% since the integral of any pp function is continuous.

hold on
iddfn = fnint( ddfn );
fnplt( iddfn, .5)
title(' ... and the integral of its second derivative')
hold off

%%
% Parts of a ppform can be obtained with the aid of FNBRK. For example
%
%   breaks = fnbrk( fn, 'break' )
%
% recovers the break sequence of the pp  in FN, while
%
%   piece2 = fnbrk( fn, 2);
%
% recovers the second polynomial piece, as this plot confirms:
%
%   fnplt( piece2, 'r', 2.5, breaks([2 3])+[-1 .5] )

hold on
breaks = fnbrk( fn, 'breaks' )
piece2 = fnbrk( fn, 2);
fnplt( piece2, 'r', 2.5, breaks([2 3])+[-1 .5] )
title(' Its second polynomial piece highlighted')
hold off

%%
% A  pp  can also be vector-valued, to describe a curve, in 2-space or
% 3-space. In that case, each local polynomial coefficient is a vector
% rather than a number, but nothing else about the ppform changes. There is
% one additional part of the ppform to record this, the  d i m e n s i o n
% (of its target).
%
% For example, here is a 2-vector-valued pp describing the unit square, as
% its plot shows. It is a 2D-curve, hence its dimension is 2.

square = ppmak( 0:4, [ 1 0  0 1  -1 1   0 0 ; 0 0  1 0   0 1  -1 1 ] );
fnplt(square,'r',2)
axis([-.5 1.5 -.5 1.5])
axis equal
title('a vector-valued pp that describes a square')

%%
% A pp in this toolbox can also be multivariate, namely a tensor product of
% univariate pp functions. The ppform of such a multivariate  pp  is only
% slightly more complicated, with BREAKS now a cell-array containing the
% break sequences for each variable, and COEFS now a multidimensional
% array. It is much harder to make up a non-random such function from
% scratch, so I won't try that here, particularly since the toolbox is
% meant to help with the construction of pp functions from some conditions
% about them. E.g., the sphere above is constructed with the aid of CSAPE,
% and then displayed by FNPLT.

x = 0:4; y=-2:2;
s2 = 1/sqrt(2);
clear v
v(3,:,:) = [0 1 s2 0 -s2 -1 0].'*[1 1 1 1 1];
v(2,:,:) = [1 0 s2 1 s2 0 -1].'*[0 1 0 -1 0];
v(1,:,:) = [1 0 s2 1 s2 0 -1].'*[1 0 -1 0 1];
sph = csape({x,y},v,{'clamped','periodic'});
fnplt(sph)
axis equal
axis off
title('a sphere described by a bicubic 3-vector-valued spline')

%%
% While the  PPFORM  of a pp is efficient for EVALUATION, the
% CONSTRUCTION of a pp from some data is usually more efficiently
% handled by determining first its  B-FORM , i.e., its representation as
% a linear combination of B-splines.
%
% For this, look at SPALLDEM, the demonstration about the B-form.


displayEndOfDemoMessage(mfilename)

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