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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Automated Control of The Color Rendering Index for LED RGBW Modules in Industrial Lighting</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Julia L. Suvorova</string-name>
          <email>usuvorova2106@gmail.com</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Sergey Yu. Arapov</string-name>
          <email>arapov66@yandex.ru</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Svetlana P. Arapova</string-name>
          <email>arapova66@yandex.ru</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Ivan S. Dubinin</string-name>
          <email>ivan_dubinin@inbox.ru</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Sergey A. Moskvichev</string-name>
          <email>serg.from.uktus@gmail.com</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Dilshod Ravshanov</string-name>
          <email>234-56-57@mail.ru</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Tajik technical University</institution>
          ,
          <addr-line>named after academician M. Osimi, Dushanbe</addr-line>
          ,
          <country country="TJ">Tajikistan</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Ural Federal University</institution>
          ,
          <addr-line>Ekaterinburg</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>In this article the method of automatic brightness components control of RGBW LED module using pulse-width modulation is proposed. The method allows the value of color rendering index Ra with values of chromaticity and overall brightness fixed to be adjusted. It enables control of visually perceived saturation of green and red colors of reflecting objects. Experimental verification of the method has shown linearity Ra changes depending on brightness of the white LED.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>Introduction</title>
      <p>green and red color saturation. In this case, visual discomfort is not perceived and Ra reduction may characterize the
increase of saturation level. Thus, Ra can be regarded as one more parameter of lighting control, responsible for the value
of clarification effect, i.e., color saturation.</p>
      <p>The purpose of this work is to develop LED devices management method, enabling the adjustment of such visually
perceived parameters as “brightness of lighting”, “lighting tint (CCT)”, “illuminated objects color saturation (Ra)”.
2</p>
    </sec>
    <sec id="sec-2">
      <title>Method of RGBW Module Spectrum Management</title>
      <p>The RGBW combination of LEDs proves to be the most suitable for achieving the goal. The spectra of individual
components, applied in the research and possible results of their mixing are shown in Fig. 1.</p>
      <p>The use of four LEDs provides a variety of light spectrum options in a single color. More uniform spectrum is closer
to the standard and should have a higher Ra (Fig. 1, b), so, the color adjustment can be performed by changing the
emission output of white LED as the main control parameter. The adjustment is performed with the help of pulse-width
modulation (PWM), preventing the displacement of dominant wavelength.</p>
      <p>The proposed method is based on vector-matrix representation of spectra light sources and colorimetric calculations.
Measured spectra are usually represented as discrete sets of emission power for a pre-fixed number of spectral bands N,
and should be viewed as vectors of N-dimensional space S. If in the processes considered the mutual influence of spectral
zones is excluded, the system of N basis vectors, corresponding to the spectral zones, can be roughly assumed
orthonormal.</p>
      <p>In the space of spectra S the subspace V (three-dimensional hyperplane) can be determined with the basis of the color
matching functions (CMF) of some colorimetric system, for example, XYZ (CIE 1931). According to the hypothesis of
Wyszecki [7, 8], vector, corresponding to illuminant D, as well as any vector of S, can be represented as a sum of two
vectors:
where vector – is orthogonal projection of to V, which is called the fundamental stimulus (or metamere), b – is
orthogonal vector to V, or metameric black. Later, Cohen [9] propose an explicit form of the projection operator of S to
V named R-matrix:</p>
      <p>Spectra sl, obtained from the RGBW LED, сan be found in the subspace L with the basis of spectra components sr, sg,
sb, sw:
where hi – is standard brightness of LED components R, G, B, W, ranging from zero to one and being proportional to
PWM pulse ratio of LEDs power supply.</p>
      <p>Thus, the control problem can be solved by finding a subset of vectors in L, whose projection on V coincides with</p>
      <p>
        It refers to the fact, that the difference of vectors sd and sl must be orthogonal to V, i.e. not perceived by the observer.
By considering (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ), the expression (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) can be rewritten as:
(
)
[
]
By considering (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ), the expression (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) can be greatly simplified and represented as:
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
where [ ] – is the matrix, composed of the listed vectors-spectra, h is a vector containing
brightness of components, which can be used to obtain the desired PWM pulse ratio. The addition of extra component h5
in vector h has not essentially modified the task of finding it because of homogeneity. Spectral power distribution in the
spectrum of standard light source is vital as it defines its chromaticity. The brightness of a standard source, determined
by the value h5, may be considered arbitrary, as the equation (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) determines only the ratio of hi component, but not its
absolute value.
      </p>
      <p>
        From (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) follows that the desired vector h* must belong to the kernel of a linear operator, defined by the matrix
whose size is 3×5 elements and the rank is 3. Thus, the dimension of the kernel is 2, and the general solution h*
of the equation (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) can be represented as basis expansion:
[
]
[
]
where values can be easily found applying standard algorithms, and the coefficients and can be arbitrary.
      </p>
      <p>
        To achieve this goal, from the set { } of all solutions of the equation (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) it is necessary to select the only thing,
corresponding to set values of the controlled parameters. This solution should correspond to the set values of controlled
parameters. It should be noted, that one of these parameters called “lighting hue” is already implicitly incorporated in (
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
as CCT, because the calculation of vector is based on it. For the accounting of “brightness” and “color saturation of
illuminated objects (Ra)” it is necessary to address to the meaning of vectors and from (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ).
      </p>
      <p>
        Consider the situation, where . In this case, the emission of white LED in the spectrum of RGBW
LEDs will not exist, as the fourth element in is equal to zero. Therefore a12, a22, a32 are the brightness of RGB LEDs,
which ratio provides a fit to on chromaticity, while their absolute values coincide with the brightness of . In this
case, to adjust the brightness of RGB LEDs, the change of coefficient value in (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) should be used. This change must
occur within the allowable pulse ratio range. If the capacity of quantized pulse ratio is excluded and its maximum value is
equal to one, then:
{
}
      </p>
      <p>Next, consider the vector . It should be noted that a12, a22, a32 are always negative. Therefore, their values indicate
how much should the RGB LEDs brightness be reduced to avoid visually perceptible change of lighting when a unit
brightness W LED is added. Therefore, value should be used to adjust the “uniformity” of RGBW LED spectrum,
which would correspond to a change in Ra and “color saturation of illuminated objects”.</p>
      <p>
        The variation limits of can easily be followed from the obvious non-negativity constraint of the components of
solution in (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ), at a given level of :
      </p>
      <p>
        The final decision is as follows:
where is a normalized value of RGBW LEDs brightness, varied from 0 to 1, is a matrix of elements from
the solution (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) of equation (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ), and are parameters, arbitrarily varied within the constraints (
        <xref ref-type="bibr" rid="ref7 ref8">7–8</xref>
        ), managing Ra
and general lighting brightness.
3
      </p>
    </sec>
    <sec id="sec-3">
      <title>Experimental Verification</title>
      <p>Experimental stand, which can be described as a lightproof box with neutral gray walls, was assembled to verify the
proposed method (Figure 2).</p>
      <p>The spectral coefficient of walls’ reflection is controlled by spectrophotometer and amounts 20%. The light source
used as a LED module, is made of RGB segments and “warm white” LED strip, designated inside the box on the upper
wall.</p>
      <p>Нigh frequency n-channel FETs (IRLML2502), controlled by PWM outputs of ATmega 328P controller take over the
power supply of R, G, B, W channels. PWM frequency is about 500 Hz, the pulse ratio adjustment step equals 1/256, that
corresponds to 8-bit quantization scale. The controller’s work is implemented under the control of monitoring program
(software package of ArduinoIO). It allows the controller to interact with the outputs from MATLAB environment,
installed on the host computer. Variable resistors are connected to three analog inputs of a controller and used to adjust
CCT, b1 and b2 .</p>
      <p>Spectral irradiance laying in the range of 370–730 nm with a pitch of 3.33 nm, is recorded with the help of
spectrophotometer i1-Pro (X-Rite) integrated with ArgyllCMS software package. While conducting all measurements, a
spectrophotometer in the box is fixed in the same position, the front part of the box is closed by an opaque curtain, and all
the colored objects are removed from the box. The data obtained are expressed in mW/(m2·nm). Random measurement
error is 0.24 mW/(m2·nm) for p = 0.95. Systematic device errors, unfortunately, can not be specified.</p>
      <p>
        The stand calibration involves the consequent measurement of sr, sg, sb, sw ranges while applying a continuous power
(PWM level - 255) to the relevant channels of a light source. Spectrum of standard illuminant of series D, which is
calculated during the experiment as a function of CCT given, is taken as a reference . Matrix X is composed of CMF
from XYZ system (10° CIE 1964), then the matrix from (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) is formed. Further, the matrix , used for
generating PWM levels from (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ), is defined. As brightness hi in (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) varies from 0 to 1, to obtain levels of PWM, in our
case, it should be multiplied by 255.
      </p>
      <p>
        The experiment involved consistent measurements of illumination spectra, depending on b1 coefficient at various
fixed CCT levels and total brightness (b2 ratio). Chromaticity and Ra were determined by spectrum. The values of b1
coefficient were set as a percentage of maximum allowable, complying with certain constraints (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ). The experimental
results are presented in Fig. 3.
As b1 coefficient was changing under the experiments conducted, visually noticeable chromaticity deviations were
observed for both experimental devices. While calculated from the spectra change of chromaticity (Fig. 3, a), they do not
exceed the conventional threshold value of legibility (0.0038 on the chart u'v' 10° CIE 1964) in general. First we tried to
explain this by the fact of CMF CIE 1964 imperfection, by analogy with [10]. However, the substitution in (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) CMF for
the newer, obtained in accordance with the suggestions of CIE Technical Committee 1-36 in 2006, has not led to the
significant improvement.
      </p>
      <p>
        Fig. 3, b shows the dependence of Ra on the value of b1 coefficient. It’s obvious that b1 coefficient (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) is perfectly
correlated with Ra value. When b1 values are about 80% of the maximum, the highest value of Ra is observed, then it
begins to decline and the further increase of white LED proportion in spectrum is meaningless. The visual control of
color reflective objects, placed in the box, has showed the decrease of intensity with the increase of Ra and vice versa.
4
      </p>
    </sec>
    <sec id="sec-4">
      <title>Conclusions</title>
      <p>RGBW LED management method has been developed and tested. It allowed the CCT, brightness, and color rendering
index Ra to be adjusted. The Ra adjustment allows visually perceived color saturation of reflecting objects to be changed
in a lighting zone due to the management of clarification effect.</p>
      <p>
        Optimum limits for the operating parameter are set. The change of b1 coefficient in (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) should be restricted within the
range of 0 to 80 % of the maximum, specified by expression (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ).
      </p>
      <p>During the experiments, a significant change in chromaticity of lighting has been obtained. This is contrary to the
predicted theoretical results. The explanation of this fact requires further research.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          1.
          <string-name>
            <surname>Hunt</surname>
            ,
            <given-names>R.W.G.</given-names>
          </string-name>
          <article-title>The Reproduction of Colour. 6th revised edition</article-title>
          . NJ: John Wiley &amp; Sons,
          <year>2004</year>
          . 724 p.
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          2. CIE 013.3
          <article-title>-1995 Method of Measuring and Specifying Colour Rendering Properties of Light Sources</article-title>
          .
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          3.
          <string-name>
            <surname>Schanda</surname>
            <given-names>J</given-names>
          </string-name>
          .
          <source>The concept of colour rendering revisited // Conference on Colour in Graphics, Imaging, and Vision. Society for Imaging Science and Technology</source>
          ,
          <year>2002</year>
          . Vol.
          <year>2002</year>
          . P.
          <volume>37</volume>
          -
          <fpage>41</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          4.
          <string-name>
            <surname>Li</surname>
            <given-names>C.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Luo</surname>
            <given-names>M.R.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Li</surname>
            <given-names>C</given-names>
          </string-name>
          .
          <article-title>Evaluation of light sources based on visual colour rendering // Color</article-title>
          and Imaging Conference.
          <source>Society for Imaging Science and Technology</source>
          ,
          <year>2008</year>
          . Vol.
          <year>2008</year>
          . P.
          <volume>201</volume>
          -
          <fpage>204</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          5.
          <string-name>
            <surname>Park</surname>
            <given-names>Y.</given-names>
          </string-name>
          <article-title>Approach to CRI (Colour Rendering Index) for full colour RGB LED source lighting // Color</article-title>
          and Imaging Conference.
          <source>Society for Imaging Science and Technology</source>
          ,
          <year>2010</year>
          . Vol.
          <year>2010</year>
          . P.
          <volume>371</volume>
          -
          <fpage>374</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          6.
          <string-name>
            <surname>Arapova</surname>
            <given-names>S.P.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Arapov</surname>
            <given-names>S.Yu.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Solodova</surname>
            <given-names>M.S.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Sergeev</surname>
            <given-names>A.P.</given-names>
          </string-name>
          <article-title>Automated laboratory light source for color rendering research in the colorimetric lighting /</article-title>
          / Proceedings of international scientific conference
        </mixed-citation>
      </ref>
      <ref id="ref7">
        <mixed-citation>
          7. “Transmission,
          <article-title>processing and perception of textual and graphical information”</article-title>
          (Ekaterinburg,
          <fpage>19</fpage>
          -
          <lpage>20</lpage>
          march
          <year>2015</year>
          ).
          <source>Ekaterinburg: UrFU</source>
          ,
          <year>2015</year>
          . P.
          <volume>34</volume>
          -
          <fpage>46</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref8">
        <mixed-citation>
          8.
          <string-name>
            <surname>Wyszecki</surname>
            <given-names>G</given-names>
          </string-name>
          . Evaluation of metameric colors // J. Opt.
          <source>Soc. Am. A</source>
          .
          <year>1958</year>
          . Vol.
          <volume>48</volume>
          . P.
          <volume>451</volume>
          -
          <fpage>454</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref9">
        <mixed-citation>
          9.
          <string-name>
            <surname>Stiles</surname>
            <given-names>W.S.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Wyszecki</surname>
            <given-names>G</given-names>
          </string-name>
          . Counting metameric object colors // J. Opt.
          <source>Soc. Am. A</source>
          .
          <year>1962</year>
          . Vol.
          <volume>52</volume>
          . P.
          <volume>313</volume>
          -
          <fpage>319</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref10">
        <mixed-citation>
          10.
          <string-name>
            <surname>Cohen</surname>
            <given-names>J.B.</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Kappauf</surname>
            <given-names>W.E.</given-names>
          </string-name>
          <article-title>Metameric color stimuli, fundamental metamers, and Wyszecki's metameric blacks //</article-title>
          <source>Am J Psychol</source>
          .
          <year>1982</year>
          . Vol.
          <volume>95</volume>
          . P.
          <volume>537</volume>
          -
          <fpage>564</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref11">
        <mixed-citation>
          11.
          <string-name>
            <surname>Csuti</surname>
            <given-names>P</given-names>
          </string-name>
          ,
          <string-name>
            <surname>Schanda</surname>
            <given-names>J</given-names>
          </string-name>
          <article-title>A better description of metameric experience of LED clusters /</article-title>
          / Light Engng.
          <year>2010</year>
          . Vol.
          <volume>18</volume>
          . № 1. P.
          <volume>44</volume>
          -
          <fpage>50</fpage>
          .
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>