Article
Reference
Recognition of the Form of Planar Objects by Means of Statistical Tests
STREIT, Franz
Abstract
Dans cette étude on montre l'utilité des techniques statistiques pour reconnaitre la forme commune d'objets plans à partir d'un système de ces objets soumis à des déformations aléatoires de leurs contours.
STREIT, Franz. Recognition of the Form of Planar Objects by Means of Statistical Tests.
Microscopy Microanalysis Microstructures , 1996, vol. 7, no. 5-6, p. 441 - 445
DOI : 10.1051/mmm:1996143
Available at:
http://archive-ouverte.unige.ch/unige:12773
Disclaimer: layout of this document may differ from the published version.
1 / 1
Recognition of the Form of Planar Objects by Means
of Statistical Tests
Franz Streit
Section de
Mathématiques
de l’Université deGenève,
Casepostale 240, 1211
Genève24,
SwitzerlandRésumé. 2014 Dans cette étude on montre l’utilité des
techniques statistiques
pour reconnaitre la formecommune
d’objets plans à partir
d’unsystème
de cesobjets
soumis à des déformations aléatoires de leurs contours.Abstract. 2014 In this article the use of statistical technics to discover the
underlying
form ofobjects subject
to random deformations isexplained.
1. The Problem
In
experimental
sciences wefrequently
observesystems
ofobjects
of similar but not identical form which aredispersed
in an Euclidean spaceIRk,
for instance in aplane IR2.
Often it is reasonable to suppose that the individualobjects
of thesystem
are obtained from anobject
of ideal formby deforming
the contour of thisobject
in a random way. It is then of interest totry
to reconstruct theoriginal
ideal form based on astudy
of the individual deformedobjects
of thesystem.
It is thegoal
of this paper to demonstrate theutility
ofsimple
statisticaltechniques
to solveproblems
ofthis kind.
2. On a Model
Proposed
in a Book of D. and H.Stoyan
Of course there exist different ways to formalize the influence of random fluctuations in this con-
text. In order to
explain
the main ideas 1 shall considersystems
ofplanar objects
and shall use astochastic model
proposed
in the book of D. and H.Stoyan [6, p.110, f.(2.72)].
We suppose that theactually
observedobjects 0 j [j
=1,..., n]
may be describedby
indication of a referencepoint Pj,
which is an interiorpoint
ofOj (for
instance the center ofgravity
ofOj),
and the radius vec- tor functionRj
of its contour measured from the referencepoint
and from a referencedirection,
which may be
specified
eitherby
a fixed direction inIR2 or by
a referencepoint
on the contour ofOj. Rj (~)
is thus thelength
of thesegment
that emanates fromP -7 -
in cl -direction and ends on thecontour of
Oj.
It issupposed
thatOj
is anon-empty compact
set which isstarlike,
i. e. the aboveArticle available at http://mmm.edpsciences.org or http://dx.doi.org/10.1051/mmm:1996143
442
mentioned
segments
are all subsets ofOh.
We suppose furthermore that the formsKl, ... , Kn
of theseobjects
constitute a randomsample,
i. e. thatKi,..., Kn
areindependent
andidentically
dis-tributed random sets obtained
by
relocation ofOj
to theorigin
ofIR ,
thusKj = (Oj )-PJ ,where
Ax designates
the translate of Aby
x. Note that ourinterpretation
of form includes an indicationof the size of the
object
and of its orientation as in[5,
pp.35,36]
andopposed
to the use of thisnotion in
[6, p.72]. Designating by
r the radius vector function of the idealform,
theproposed
model for the random deformation of the contour relates the
quantities
as follows:We shall first discuss the situation for the case where we admit
ellipses
as forms. In standardorientation
r(~)
satisfies the main formulatogether
with thecomplementary symmetry
formulaewith half-axes
a, b > 1 ; a
and b are unknown. Thestudy
ofKl , ... , Kn
isconcretely
carried outby measuring
the radius vector onprescribed angles,
for instance for cep =0° , 90°, 180°
and 270°. We suppose that the individual deformationsZt (17r /2),
... ,Zn(l7r /2), [1
=0, 1, 2, 3]
at theseangles
form
independent
randomsamples
from apopulation
withdensity
functionThus the additive deformations follow a truncated normal distribution. The truncation is cho-
sen in such a way that the radius vector of the
resulting
form does not takenegative
values.3. Are the
Object
of Circular or ofNon-Degenerated Elliptical
Form?Consider the
following testing problem,
which is ofpractical
relevance in the context of the sto- chastic model described in theprevious paragraph.
We want toknow,
whether we needeffectively
to admit the class of
ellipses
or whether the more restricted class of circles would be sufficient forour purpose, i. e. we want to test the
hypothesis
versus the
hypothesis
where a and b are
unknown,
but a, b > 1. In such a case statisticalmethodology [3, 7, 8]
recom-mends to use the
generalized
likelihood ratio test for the decisionfinding.
The test-statistic is then calculatedaccording
to the formulawhere L
designates
thelikelihood-function, specified by
where the
principal arguments
of L are the unknownparameters
of the model a and b and L is conditionedby
the observed formsKi,..., Kn
insofar as known from the measurementsRZ (ln /2), [i = 1,...,n;l = 0, 1, 2, 3].
For the values of the random
variables,
which are used in the evaluation ofAgen
we findThe numerator
(resp.
thedenominator)
ofAgen
is obtainedby replacing
a and bby
their com-mon
(resp. individual)
maximum-likelihoodestimators R (resp. Â
andÊ).
These estimators areobtained in the same way as in standard
theory
fornormally
distributedsamples,
buttaking
intoaccount the size restrictions on a and b. Thus we find
and
This leads to the
explicit analytic expression
of the test statisticgiven by
and for
large
values of n to theasymptotical
criticalregion
of size (tIn this context
Àgen designates
the realized value of the statisticAgen and xî( 1 - a)
is the critical value of theX2
distribution of Pearson with onedegree
offreedom,
which satisfies the relationFor
sufficiently large n
the test is thus easy to carry out and leads to therejection
ofHo
ifÀgen
satisfies the
inequality (1); only
a table of the critical values ofthe X2 1 -distribution
is needed for thepractical implementation
of theprocedure.
4. Generalizations and Extensions
Of course
only
a veryspecial
version of theproblem
ofrecognition
of theunderlying
form hasbeen treated so far and it is obvious that the same
techniques
may be used to resolve many similarproblems.
444
4.1 OTHER CLASSES oF FORMS . - For instance we may
replace
the class ofellipses by
a richerclass of forms for which
r(0)
==r(7r)
= a andr(7r/2)
=r(37r/2)
= b. Such a class is for instance the class ofsuperellipses [2],
definedby
the main formulaand the same
complementary symmetry
formulae as for theellipses.
The class admits convexforms
(for
c >1)
and non-convex forms(for
c1).
For this class of forms the test of the
hypothesis
ofequality
of the half-axes a and b may be carried out inexactly
the same way aspreviously
described.If one wants also to make inference on c, for instance if one wants to estimate c, it will be necessary to measure the radius vector function of the
Kis
at otherangles
than0°, 90°, 180°,
270°.For instance it may be
advantageous
to take additional measurements at theangles 45 ° ,135 ° ,
225 °and 315°. We shall comment on this
point
later in Section 4.4.4.2 RANDOM DEFORMATIONS GENERATED BY OTHER DISTRIBUTIONS Of course one can
adopt probability
laws for the randomdeformations Zi(l03C0/2)
other than the truncated normal distribution. Theprocedure
ofgeneralized
likelihood ratio test may still beuseful,
but the for-mulae for the maximum likelihood estimators and also the test statistic may
change.
One may also extend thetechniques
discussed to situations where the deformations at differentangles
arenot
independent.
This couldimprove
theapplicability
of theproposed methods,
but leads to theproblem
offinding
asufficiently simple
andgenerally meaningful incorporation
ofdependence
relations into the model. Work on this is
currently
in progress.4.3 OTHER DIMENSIONS OF THE SPACE .
- Instead of considering systems of planar objects one
may
study systems
ofobjects
in other Euclidean spaces, for instance in three-dimensional spaces.One
adapts
then the formula for theellipses (superellipses) by including
a third coordinate. Apractical
context where such aset-up
could be of interest is thesituation,
where one has to decide whether the sandgrains
found on aparticular
site havespherical
ornon-degenerate ellipsoidal
form.
4.4 OTHER STOCHASTIC MODELS. - The additive stochastic model used so far may not be the
only
one to take into account. It may for instance be that the observed radius vectors are rathermultiplicatively
thanadditively
related to the radius vectors of the common form as in the formulaThis
type
of model issimpler
to handlemathematically,
since inprinciple
all the distributions concentrated onnon-negative
real values are now admitted for thespecification
of theprobability
law of the
Zi’s;
we do not have toapply
unusual distributions obtainedby
truncation in order tokeep
theRi’s non-negative.
Suppose
that we havealready
established that in the stochastic model with the relation(2)
theclass of
superellipses satisfying a
= b isappropriate,
but that c is still unknown and should be esti- mated.Suppose
that themultiplicative
deformations factorsZi(l03C0/4), [i
=1,..., n ;
l =
1,3,5,7]
form a randomsample
of size 4n from theexponential
distribution withdensity
function
and
We find
where a = b = r. Since
Ri(17r/4)
=Zi(17r/4)/r(17r/4),
we find for theloglikelihood
of themeasurements which
depend
on cThus
Putting
thisexpression equal
to 0yields
the maximum likelihoodequation
Therefore we obtain as estimator
4.5 OTHER APPROACHES . - Instead of
treating
theproblems by
statisticalmethodology,
onecan also use methods of
morphology,
likeconstructing
andstudying
the skeleton of the individualobjects [1,
pp.308-311]
or treat theproblems
in adescriptive
wayusing shape parameters (see
e.g.
[4]
for the definition of suchquantities).
References