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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Estimation of Spring Sti ness under Conditions of Uncertainty. Interval Approach</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Sergey I. Kumkov</string-name>
          <email>kumkov@imm.uran.ru</email>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Krasovskii Institute of Mathematics and Mechanics</institution>
          ,
          <addr-line>Ural Branch RAS</addr-line>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Ural Federal University</institution>
          ,
          <addr-line>Yekaterinburg</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <fpage>63</fpage>
      <lpage>73</lpage>
      <abstract>
        <p>The work deals with a problem of estimation of spring sti ness under conditions of uncertainty of its loading and compression measurements. During spring exploitation, the main its parameters sti ness and initial length change since of the metal strain aging. At the spring checking, values of its compression are measured in the necessary range of loading. It is used to describe the spring compression by the Hooke's law. In practice, a sample of measurements is very short and measuring is implemented with errors, which probability data are unknown. So, it is di cult to validate application of standard statistical methods to estimation of the spring sti ness. Under such conditions, an alternative to now existing approaches is application of the Interval Analysis methods that do not use any probabilistic properties of the measuring errors. In the work, the Interval Analysis methods are used for constructing the information set of admissible values of the spring parameters (the sti ness and initial length).</p>
      </abstract>
      <kwd-group>
        <kwd>Spring</kwd>
        <kwd>parameters</kwd>
        <kwd>sti ness</kwd>
        <kwd>initial length</kwd>
        <kwd>estimation</kwd>
        <kwd>interval analysis methods</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>During practical exploitation of steel springs, some changing of its material
appear. Under this, check (tests) of the spring is performed with prescribed time
period.</p>
      <p>Usually, for estimation of the spring parameters (the sti ness and initial
length), the standard methods to estimation are used that are based on the
mathematical statistics ideology [1], [2], [3].</p>
      <p>But in practice, a sample of measurements is very short and measuring the
loading force and spring compression are implemented with errors, which
probability data are unknown. Moreover, the model of the compression process is
approximately described by the linear dependence corresponding to the Hooke's
law, and the sample of measurements is rather short. So, under these conditions,
it is di cult to strictly validate application of standard methods, and in
practice, they are often used rather formally. As an alternative, application of the
statistical methods can be completed by using the Interval Analysis ones.</p>
      <p>For constructing a set of admissible values of the spring parameters, the
Interval Analysis methods use only the model description of the process (the
Hooke's law) and the bounds on the measuring errors of the loading force and
compression value.</p>
      <p>Such a set is used to call the Information Set. It comprises only such
parameters of the model that are consistent with its description, accumulated sample of
measurements, and the given bounds onto the mentioned measuring errors. On
the basis of the determined Information Set, corresponding tube of the admissible
dependencies of the spring under compression is formed.</p>
      <p>The paper has the following structure. In Section 2, the technical details of the
experiment are considered and typical model of the spring compression vs loading
is introduced. Section 3 is devoted: to description of the main Interval Analysis
procedures used for constructing the Information Set of the spring parameters
(the sti ness and initial length) and the problem of investigation is formulated.
In Section 4, for illustration of the elaborated estimation algorithms, a model
example is investigated on a sample of measurements of a spring compression.
Moreover, comparison of this results is made with ones obtained by the standard
Least Square Means method (LSQM) [2]. In Section 5, conclusions are given
on abilities of the suggested Interval Analysis approach and its applications in
addition to known estimation procedures [1], [2], [3].
2</p>
      <p>Details of experiment for investigation
of spring parameters
The following experiment is performed.
1. The spring is put under the loading press.
2. The loading is performed by a collection of given forces Fn</p>
      <p>
        fFng; n = 1; N ; Fn 2 [F1; FN ]; 0 &lt; F1;
from the working range [F1; FN ] of the spring.
3. For each force value Fn, the spring compression (length) is measured
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
4. As a result of the test, the following sample is obtained:
      </p>
      <p>
        fsng; n = 1; N :
fFn; sng; n = 1; N :
5. Since of the measuring errors both in the loading force and in the spring
compression, data (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) are corrupted as follows:
n = 1; N ;
Fn = Fn + en; jenj
emax; sn = sn + bn; jbnj
bmax;
where Fn is the loading measurement; Fn is the unknown true value of loading;
en is the additive measuring error of the loading force; emax is the bound (on
modulus) on the loading measuring error; sn is the compression measurement;
sn is the unknown true value of the compression; bn is the additive measuring
error; bmax is the bound (on modulus) on the compression measuring error. It is
assumed that in the neighbor measurements errors are independent.
      </p>
      <p>
        Remark 1. We suppose that
{ measurements (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) are homogeneous, i.e., the bounding values emax and bmax
in (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) are the same in all measuring;
{ sample (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) is authentic i.e., it does not contain outliers.
      </p>
      <p>As a rule, actual description of the spring compression (changing its length
vs the compression force) is unknown for a researcher (Fig. 1). Here, the true
curve is in dashes; true values of the force F and compression s are marked
by circles; the rectangles in dots are regions of possible location of authentic
measurements.</p>
      <p>
        So, for elaboration of algorithms for estimating the compression parameters,
the linear model corresponding to the Hooke's law is used in the form
S(F; a; s0) = aF + s0;
(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
where S(:::) is the current value of the spring compression (length), mm; F is
the loading force, N; a &lt; 0 is the sti ness, mm/N; s0 is the spring initial length,
mm.
      </p>
      <p>
        In the linear model (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ), its parameters s0 and a are assumed to be constant
during the time interval of the spring exploitation.
      </p>
      <p>
        Often in practice, it is possible to show some useful approximate intervals for
the spring parameters in model (
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
aapr = [aapr; aapr]; s0;apr = [s0;apr; s0;apr]:
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
(Here and further in the text, we keep at the standard notations accepted
for the interval variables [9]).
3
      </p>
      <p>Interval approach to estimating
the spring parameters. Problem formulation
Foundations of Interval Analysis and its applications to processing observations
under uncertainty conditions were developed on the basis of the fundamental
pioneering work of L.V. Kantorovich [4].</p>
      <p>Nowadays, e ective theoretical, applied, and numerical methods of the
Interval Analysis have been created both abroad [5], [6] and by Russian researchers
[7], [8]. Special interval algorithms and software were developed for solving
applied problems of estimation of parameters for experimental chemical processes
[10], [11], [12], [13], [14].</p>
      <p>Remind that the essence of the interval methods is in estimating the process
parameters under conditions of a short measurement sample, uncertainty of the
measuring errors probability characteristics and under only interval bounding
onto the error values.</p>
      <p>Introduce the following necessary de nitions (with using the standard on
notations in Interval Analysis [9]).</p>
      <p>The uncertainty set of the spring loading and compression measurement.
Since absence of probability characteristics of measuring errors, uncertainty of
each measurement Fn; sn is formalized (Fig. 2) as a rectangle Hn with the left
F n and right F n, lower sn and upper sn boundaries.</p>
      <p>n = 1; N ; Hn :
7a) F n = [F n; F n];</p>
      <p>where F n = Fn
7b) sn = [sn; sn];
where sn = sn
emax; F n = Fn + emax;
bmax; sn = sn + bmax:</p>
      <p>
        The admissible value of the parameters vector (a; s0) for model (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ),(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
is a pair
(a; s0) : S(n; a; s0) 2 F n
sn for all n = 1; N ;
and corresponding dependence S(n; a; s0) is also called admissible.
      </p>
      <p>
        The Information Set (INFS) is a totality of all admissible values of the
parameter vector for model (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ),(
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) satisfying the following system of interval
inequalities:
      </p>
      <p>
        I(a; s0) = f(a; s0) : S(n; a; s0) 2 F n
sn; n = 1; N g:
(
        <xref ref-type="bibr" rid="ref7">7</xref>
        )
(
        <xref ref-type="bibr" rid="ref8">8</xref>
        )
      </p>
    </sec>
    <sec id="sec-2">
      <title>Uncertainty set of measurement</title>
      <p>H
k
_Fn = Fn_ emax
Hn</p>
      <p>Hn
. . .</p>
    </sec>
    <sec id="sec-3">
      <title>Admissible dependence</title>
      <p>of the linear type with a, s0. . .</p>
      <p>. . .</p>
      <p>F
1</p>
      <p>Fk</p>
      <p>Fn
_
Fn = Fn+ emax
_
sn = sn + bmax
_sn = sn _ bmax</p>
      <p>H</p>
      <p>N</p>
      <p>F, N
FN</p>
      <p>
        The input sample (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) is called consistent in the interval sense if by (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) there
exists at least one admissible value of the parameter vector and corresponding
admissible dependence.
      </p>
      <p>
        The tube of admissible dependencies T b(F ) (Fig. 3) is a totality of all
admissible values of the dependence on the loading force F . For model (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) and
the information set I(s0; a), the tube boundaries are calculated with taking into
account the loading force F interval
      </p>
      <p>F 2 [F1; FN ] :
T b(F ) = min(a;s0)2I(a;s0) S(F; a; s0);</p>
      <p>T b(F ) = max(a;s0)2I(a;s0) S(F; a; s0):</p>
      <p>
        Problem of estimation is formulated as follows: by means of the Interval
Analysis methods to construct the Information Set (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) of the spring coe cients
values consistent with the given data (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) and to build the tube (
        <xref ref-type="bibr" rid="ref10">10</xref>
        ) of the
admissible values of the spring compression.
      </p>
      <p>
        For the linear model (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ), fast procedures for constructing the Information Set
(
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) with exact description of its boundaries have been elaborated and applied to
solving many practical problems [10], [11], [12], [13], [14]. Due to direct using the
linearity of model (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ), these procedures are more fast and give exact description
of the Information Set in comparison with even very powerful procedures of the
SIVIA-type [5].
      </p>
      <p>
        Remark 2. As it will be shown below, formal application of the standard
Least Square Means method (LSQM) [2] and corresponding point-wise estimate
of the parameters ((aSQ; s0;SQ) for the linear model) demonstrate to be useful for
(
        <xref ref-type="bibr" rid="ref10">10</xref>
        )
      </p>
      <sec id="sec-3-1">
        <title>Upper boundary of the tube</title>
        <p>Hk</p>
      </sec>
      <sec id="sec-3-2">
        <title>Lower boundary of the tube</title>
        <p>
          Tube of admissible dependences
analysis of the input sample (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) and for qualitative comparison with the results
on the basis of Interval Analysis.
        </p>
        <p>
          Elaborated engineering interval procedures
For simplicity of narration, consider a practical case when for all n
F n &lt; F n+1 and sn &gt; sn+1:
(
          <xref ref-type="bibr" rid="ref11">11</xref>
          )
For other mutual location of uncertainty sets, computation formulas are derived
in the similar way.
        </p>
        <p>Consider a pair of uncertainty sets Hn and Hk, n = 2; N , k = n 1, with
their corner points 1, 2, 3, 4 and 5, 6, 7, and 8 (Fig. 4a). For each pair, the bunch
of admissible dependences is introduced. The bunch is bounded by the lines
LI and LIII with the extremal values of parameters a min; s0;max and amax; s0;min
and by the lines LII and LIV with the intermediate values of parameters aII; s0;II
and aIV; s0;IV, correspondingly.</p>
        <p>
          Under conditions (
          <xref ref-type="bibr" rid="ref10">10</xref>
          ), parameters of these lines are computed as follows:
LI : a min = (sn
LIII : amax = (sn
LII : aII = (sn
LIV : aIV = (sn
sk)=(F n
sk)=(F n
sk)=(F n
sk)=(F n
        </p>
        <p>F k); s0;max = sk + aminF k;</p>
        <p>F k); s0;min = sk + amaxF k;
F k); s0;II = sk + aIIF k;</p>
        <p>
          F k); s0;IV = sk + aIVF k:
(
          <xref ref-type="bibr" rid="ref12">12</xref>
          )
        </p>
        <p>III</p>
        <p>Fk</p>
        <p>Hk
2
3
lines with intermediate
values of parameters a, s0
Note that for homogeneous sample (Remark 1) aII = aIV.</p>
        <p>
          From Figure 4a it is seen that in the case of mutual location (
          <xref ref-type="bibr" rid="ref11">11</xref>
          ) of the pair
Hn and Hk, the bunch of admissible dependencies is completely determined
by the diagonals \2{4" and \6{8". This allows to use techniques elaborated for
one-dimensional uncertainty sets of measurements [10], [13], [14].
        </p>
        <p>
          For each pair Hk and Hn, the partial information set G(a; s0)k;n of
parameters is determined by the computed apex points (
          <xref ref-type="bibr" rid="ref11">11</xref>
          ). Note (Fig. 4b) that
it is a convex four-apex polygon with linear boundaries.
lines with the extremal
values of parameters s0,a
5
8
        </p>
        <p>Hn
6 (amax,s0min)</p>
        <p>L</p>
        <p>I
7</p>
        <p>L
(aIIVV,s0,IV)</p>
        <p>LII (aII,s0,II)
LIII (amin,.s.0.max)</p>
        <p>F, N</p>
        <p>
          Having constructed the collection of partial information sets fGk;n(a; s0)g,
n = 2; N , k = n 1, it becomes possible to calculate the desirable information
set I(a; s0) (
          <xref ref-type="bibr" rid="ref9">9</xref>
          ) of admissible values of the compression parameters for the whole
sample (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) of measurements
        </p>
        <p>
          I(a; s0) = Tn=2;N; k=n 1 Gk;n(a; s0):
(
          <xref ref-type="bibr" rid="ref13">13</xref>
          )
. . .
        </p>
        <p>
          _
a
_
a
acnt
a, mm/N
a priori
rectangle
aapr s0,apr
_
s0
s0,cnt
s0
_
(
          <xref ref-type="bibr" rid="ref14">14</xref>
          )
(15)
        </p>
        <p>
          This procedure is implemented by some appropriate standard program of
intersection of convex polygons. Image of the information set I(a; s0) is presented in
Fig. 5 (shadowed by red). It is determined by the apex points I, II, III, and IV
(a; s0)I; :::; (a; s0)IV:
The information set (
          <xref ref-type="bibr" rid="ref12">12</xref>
          ) can be compared with the a priori data rectangle
aapr s0;apr (
          <xref ref-type="bibr" rid="ref6">6</xref>
          ), and there is possibility of its enhancing (Fig. 5).
        </p>
        <p>For practical using, the following parameters' values are given to a researcher:
{ exact description of the information set I(a; s0);
{ unconditional interval in parameter a : [a; a];
{ unconditional interval in parameter s0 : [s0; s0];
{ central point acnt = 0:5(a + a); s0;cnt = 0:5(s0 + s0):
4</p>
        <p>Model example. Results of estimation
of spring parameters
For computations, the following input model data are given:
{ the initial true length of the spring s0 = 120 mm;
{ the sti ness true value a = 0:1020 mm/N;
{ number of measurements N = 5;
{ the true loading forces are fFn g = f196; 392; 588; 784; 980g N;
{ the true values of compression are fsng = f100; 80; 60; 40; 20g mm;
{ the bound on the loading force measurement emax = 40 N;
{ the bound on the compression measuring bmax = 2 mm;
{ corrupted measured values of the loading forces are fFng = f221:9; 364:2;
611:4; 778:2; 983:5g N;
{ corrupted measured values of compression are fsng = f98:28; 78:22; 61:34;
41:90; 18:02g mm.</p>
        <p>After procession, the resultants information set I(a; s0) is presented in Fig.6.
It is a convex polygon with ve apices. It has sizes: a = 0:1189 mm/N, a =
0:0905 mm/N, s0 = 112:76 mm, s0 = 128:317 mm.</p>
        <p>The information set central point is acnt = 0:1047 mm/N, s0;cnt = 120:53
mm.</p>
        <p>Formal estimation of the input corrupted sample by the Least Squares Means
method gave the point aSQ = 0:1009 mm/N, s0;SQ = 119:31 mm; and
estimation of the standard deviation is = 3:12 mm.</p>
        <p>Central point</p>
        <p>LSQM-point</p>
        <p>It is seen (Fig. 6) that since of the outliers absence, both the true point and
the LSQM one are inside the information set.</p>
        <p>Picture of the compression process and results of procession are also shown
in Fig. 7. Note that formal application of the standard rule \ 3 " gives
approximate very wide \corridor" around the LSQM-line.</p>
        <p>In a contrast, application of the described interval approach allows one to
build signi cantly narrow tube of admissible dependences. Moreover, it is seen
that uncertainty sets of measurements have been enhanced: their inadmissible
parts are cut o by the tube.</p>
        <p>Underline that due to admissibility of the true and the LSQM points (Fig. 6),
corresponding line dependencies are whole inside the tube (Fig. 7).
rseaeumtirceann</p>
        <p>Mu
o
L
e
l
b
i
iss ise
2
9
3
The Interval Analysis methods was applied to estimation of spring parameters
in the compression process under conditions of absence of probability data for
the measuring errors.</p>
        <p>Important case was investigated when errors are both in the loading force
measurements and in ones of the spring compression (length).</p>
        <p>Investigations are ful lled on the basis of the wide used Hooke's law with the
linear dependence of spring compression vs the loading force.</p>
        <p>It was shown that under mentioned conditions Interval Analysis approach
gives guaranteed estimation of the process parameters and better estimation of
the tube of admissible dependencies.</p>
        <p>Moreover, simulation results show that using simultaneously, the interval and
standard statistical approaches complement each other; and this allows one to
perform more detailed analysis and qualitative comparison of the estimation
results.</p>
        <p>Acknowledgments. The work was supported by Act 211 Government of the
Russian Federation, contract no. 02.A03.21.0006.</p>
      </sec>
    </sec>
  </body>
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