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  <front>
    <journal-meta><journal-id journal-id-type="publisher">JSSS</journal-id><journal-title-group>
    <journal-title>Journal of Sensors and Sensor Systems</journal-title>
    <abbrev-journal-title abbrev-type="publisher">JSSS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">J. Sens. Sens. Syst.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2194-878X</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/jsss-7-559-2018</article-id><title-group><article-title>Continuous in-line monitoring of electrolyte concentrations in
extracorporeal circuits for individualization of dialysis treatment</article-title><alt-title>Continuous in-line monitoring of electrolyte concentrations </alt-title>
      </title-group><?xmltex \runningtitle{Continuous in-line monitoring of electrolyte concentrations }?><?xmltex \runningauthor{M. Berger et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Berger</surname><given-names>Marc</given-names></name>
          <email>berger@geml.uni-hannover.de</email>
        <ext-link>https://orcid.org/0000-0002-9647-4803</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Faulstich</surname><given-names>Michael</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Perl</surname><given-names>Thorsten</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Zimmermann</surname><given-names>Stefan</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Institute of Electrical Engineering and Measurement Technology,
Department of Sensors and Measurement Technology, Leibniz Universität
Hannover, 30167 Hannover, Germany</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Anesthesiology, University Göttingen, 37099 Göttingen,
Germany</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Departments of General-, Visceral- and Paediatric Surgery, University
Göttingen, 37099 Göttingen, Germany</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Marc Berger (berger@geml.uni-hannover.de)</corresp></author-notes><pub-date><day>29</day><month>October</month><year>2018</year></pub-date>
      
      <volume>7</volume>
      <issue>2</issue>
      <fpage>559</fpage><lpage>567</lpage>
      <history>
        <date date-type="received"><day>29</day><month>March</month><year>2018</year></date>
           <date date-type="rev-recd"><day>10</day><month>October</month><year>2018</year></date>
           <date date-type="accepted"><day>12</day><month>October</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018.html">This article is available from https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018.html</self-uri><self-uri xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018.pdf">The full text article is available as a PDF file from https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018.pdf</self-uri>
      <abstract>
    <p id="d1e118">One objective of dialysis treatment is to normalize the blood
plasma electrolytes and remove waste products such as urea and creatinine
from blood. However, due to a shift in plasma osmolarity, a rapid or
excessive change of the electrolytes can lead to complications like
cardiovascular instability, overhydrating of cells, disequilibrium syndrome
and cardiac arrhythmias. Especially for critical ill patients in intensive
care unit with sepsis or multi-organ failure, any additional stress has to be
avoided. Since the exchange velocity of the electrolytes mainly depends on
the concentration gradients across the dialysis membrane between blood and
dialysate, it can be controlled by an individualized composition of dialysate
concentrations. In order to obtain a precise concentration gradient with the
individualized dialysate, it is necessary to continuously monitor the plasma
concentrations. However, with in-line sensors, the required hemocompatibility
is often difficult to achieve. In this work, we present a concept for
continuous in-line monitoring of electrolyte concentrations using
ion-selective electrodes separated from the blood flow by a dialysis
membrane, and therefore meeting the fluidic requirements for
hemocompatibility. First investigations of hemocompatibility with
reconfigured human blood show no increased hemolysis caused by the measuring
system. With this concept, it is possible to continuously measure the plasma
concentrations with a relative error of less than 0.5 %.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e128">Dialysis is a life-saving therapy, which is used for purifying the blood in
the case of kidney failure. In dialysis, blood is pumped via an extracorporeal circuit
into a dialyzer consisting of a semipermeable membrane separating blood and
the dialysate. Due to concentration gradients across this membrane, waste
products such as urea and creatinine can be removed by diffusion and the
electrolyte balance can be regulated (Sivalingam and Farrington, 2007).
Critically ill patients in the intensive care unit (ICU) with, e.g., sepsis or
multi-organ failure, often develop acute kidney injury (AKI), characterized by
the rapid loss of kidney function (Zarjou and Agarwal, 2011; Baue et al.,
2000; Bellomo et al., 2012; Bagshaw et al., 2008). The mortality rate of such
patients exceeds 50 % (Ricci et al., 2006). The treatment of AKI related
to critical illness is usually continuous renal replacement
therapy (CRRT) with a duration of up to 72 h (Patel et al., 2010; Patschan
and Müller, 2015; Ricci et al., 2006; Tumlin et al., 2008). Due to the
longer treatment compared to intermitted dialyses (3–4 h every 2–3 days),
CRRT enables a slower removal of waste products and regulation of electrolyte
balance, resulting in a benefit for unstable patients, as a rapid change of
osmotic substances can lead to complications (Patel et al., 2010).</p>
      <p id="d1e131">For instance, an excessive or rapid loss of sodium in the blood, and thus an
abrupt shift in plasma osmolarity, can result in cardiovascular instability,
overhydrating of cells and disequilibrium syndrome with muscle cramps,
fatigue symptoms and headaches. Conversely, an inefficient sodium<?pagebreak page560?> removal
and thus sodium accumulation can cause hypertension, increased thirst and
pulmonary edema (Stiller et al., 2001; Palmer, 2001; Locatelli et al., 2015;
Paula et al., 2004). Another important aspect during the dialysis session is the
potassium concentration. Too low a plasma potassium concentration
(hypokalemia) and too high a plasma potassium concentration
(hyperkalemia) can both lead to cardiac arrhythmias (Kovesdy et al., 2007). However, not
only the absolute concentration can be critical but also the rapid removal of
plasma potassium may trigger arrhythmias (Buemi et al., 2005). A rapid
decline in plasma concentration due to a high gradient between dialysate and
blood during the first hours of the treatment can be caused by a large
mismatch of the potassium concentration in the dialysate. The rapid drop of
potassium in plasma can therefore be avoided by using an exponentially
decreasing dialysate concentration with a fixed concentration gradient
between blood and dialysate of 1.5 mmol L<inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Redaelli et al., 1996).
This leads to a slower potassium removal and prevents arrhythmia. The
concentration of ionized plasma calcium (free calcium) also affects the
cardiovascular system. Increasing the ionized calcium in the dialysate and
thus increasing the plasma concentration leads to an improvement of the left
ventricular contractility, which is particularly interesting for unstable
patients (Henrich et al., 1984; Lang et al., 1988).</p>
      <p id="d1e146">Furthermore, an important marker for dialysis is urea because it represents
the waste products (Keshaviah et al., 1995). For instance, a parameter for
evaluating the efficiency of dialysis is the urea reduction ratio (URR)
according to Eq. (1):

              <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M2" display="block"><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">URR</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>U</mml:mi><mml:mi mathvariant="normal">post</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>⋅</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

        where <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi mathvariant="normal">pre</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the pre-dialysis urea concentration in blood and
<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mi mathvariant="normal">post</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the blood urea concentration measured 5 min after
the end of dialysis. It can be shown that URRs less than 60 % are
associated with a higher mortality in patients during dialysis (Owen et al.,
1993). There are several approaches to determine the efficiency of dialysis
treatment using urea as a marker substance, but all of these methods measure
the urea concentration in the dialysate, making it difficult to continuously
monitor the actual urea concentration in the patient's blood (Lindsay and
Sternby, 2001).</p>
      <p id="d1e212">In order to ensure a precise control of the dialysis treatment by
individualization of the dialysate composition, thus controlling the
concentration gradients across the dialysis membrane, it is necessary to
continuously monitor the electrolyte concentration in the blood. This allows
a precise control of the electrolyte exchange velocity, which mainly depends
on the concentration gradients. As mentioned earlier, there are specific
recommendations for the concentration gradient of potassium. Therefore, we
present a concept for continuous in-line measurement of electrolytes using
ion-selective electrodes (ISEs) that meets the fluidic requirements for
hemocompatibility. First investigations with reconfigured human blood show no
increase in hemolysis. However, it should be noted that further
hemocompatibility tests with blood samples are still ongoing and experimental
proof of hemocompatibility is pending. In addition, this concept can be
extended by a urea sensor to determine the efficiency of dialysis treatment.</p>
</sec>
<sec id="Ch1.S2">
  <title>State of the art and concept</title>
      <p id="d1e221">Since blood parameters such as electrolyte and urea concentrations are of
great medical interest, various monitoring concepts have been developed
(Sharma et al., 2016). There are already devices on the market that can
determine the URR online by evaluating the conductivity of the dialysate
(Diascan<sup>®</sup> Gambro Hospal GmbH; OCM;
Fresenius). Furthermore, the URR can be measured optically by ultraviolet
absorbance or near-infrared spectroscopy in spent dialysate (Gál et al.,
1983; Cho et al., 2008). The disadvantage of these methods is that only the
urea removal can be determined, while it is difficult to derive the current
blood concentration. Enzymatic biosensors also allow the urea
concentration to be measured. One possibility to realize such a biosensor is to immobilize
the enzyme urease on an ammonium- or ammonia-selective electrode. If the
urease is immobilized close to the sensitive layer of the corresponding
electrode, a urea-dependent voltage between the ISE and the reference
electrode is obtained by splitting the urea into ammonia and ammonium ions in
aqueous solutions due to the catalytic effect of the enzyme (Eggenstein et
al., 1999; Dhawan et al., 2009; Koncki, 2007; Marchenko et al., 2015; Singh
et al., 2008). Immobilizing the enzyme on a dialysis membrane can further
improve hemocompatibility of the sensor (Schindler and Schindler, 1983).</p>
      <p id="d1e227">An optical method to determine the concentration of electrolytes such as
sodium and potassium in blood is the flame photometry. Here the blood is
sprayed into a nonluminous flame and the intensity and wavelength of the
emitted light are measured (Domingo and Klyne, 1949). To eliminate the need
for a gas flame, laser-induced breakdown spectroscopy can be used. The
measurement principle is similar to flame photometry, except that the gas
flame is replaced by a strong laser pulse (Knopp et al., 1996). The
disadvantage of this method is the missing in-line measurement capability. An
in-line capable solution to determine blood gases and potassium is the
Proxima System developed by Sphere Medical Ltd..</p>
      <p id="d1e230">Another common method for determining the electrolyte concentrations in
the liquid phase is electrochemical potentiometric measurement using ISEs or
ion-selective field-effect transistors (ISEFETs). For this, a
concentration-dependent voltage is measured between the ISEs and a reference
electrode (Mikhelson, 2013; Cammann, 1979). Schindler et al. developed a flow
cell for ISEs (Schindler and Schindler, 1983; Schindler and Glich, 1981).
However, due to hemoincompatibility, the blood cannot go back into<?pagebreak page561?> the
patient. To reduce the required blood volume, the size of the system can be
reduced with the help of microfluidic devices and miniaturized ISFETs (Liao
et al., 2006; Johnson et al., 2008; Gumbrecht et al., 1990).</p>
      <p id="d1e233">However, for reasons of hemo- and biocompatibility, a direct in-line
measurement with ISEs in blood is usually not possible (Gavalas et al.,
2006). Proteins can adsorb on the ion-selective membrane of the ISEs, leading
to a so-called membrane fouling, causing a time-dependent drift of the sensor
signal (Sharma et al., 2016). More importantly, the adsorbed proteins can
trigger blood coagulation and hemolysis and thus threaten the patient's life,
making direct measurement in blood flow impossible.</p>
      <p id="d1e237">For this reason, Schindler et al. used an individual dialyzer in the
extracorporeal circuit separating the measuring circuit from the direct blood
flow (Schindler and Schindler, 1983). Since each dialyzer produces a certain
amount of hemolysis, it is not recommended to insert a second dialyzer into
the extracorporeal circuit during dialysis treatment. In addition, this
approach requires considerable financial and technical effort.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p id="d1e242">Schematic of the in-line concept for measuring blood parameters
using ISEs in a liquid-filled sensor compartment separated from the blood
flow in the extracorporeal circuit by a dialysis membrane.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f01.png"/>

      </fig>

      <p id="d1e251">Therefore, we insert the ISEs into a compartment filled with physiological
electrolyte solution, which is separated from the blood flow in the
extracorporeal circuit by a dialysis membrane, which we name “compartment
membrane” in the following, as depicted in Fig. 1. Since the blood and
liquid-filled sensor compartment are separated, the ISEs are no longer in
direct contact with the blood flow. Substances which are larger than the
molecular weight cutoff of the membrane, e.g., proteins and cells, are
retained and do not get into contact with the sensors. However, electrolytes
and urea can diffuse through this membrane, leading to a concentration
equalization between the blood and sensor compartment. This offers the
possibility of obtaining an in-line flow system for continuous determination
of the electrolyte concentrations with less instrumental effort than the
above-mentioned approach by Schindler et al. and a flow concept which meets the
requirements for hemocompatibility.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p id="d1e256">Schematic of the used simulation model with a laminar blood flow in
the extracorporeal circuit. The liquid-filled ISE compartment has a diameter
<inline-formula><mml:math id="M5" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 12.1 mm and a height <inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 5 mm. The diameter <inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of
the ISE is 12 mm; <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> describes the variable distance between
compartment membrane and the sensitive layer of the ISE.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f02.png"/>

      </fig>

</sec>
<sec id="Ch1.S3">
  <title>Simulations</title>
      <p id="d1e315">In order to evaluate the time-dependent behavior of this in-line-measurement
concept, we used a two-dimensional simulation (COMSOL Multiphysics 5.1).
Figure 2 describes the design of the simulation model. In the lower part, the
blood of the extracorporeal circulation flows tangentially along the
compartment membrane. Since turbulent blood flow can lead to hemolysis, a
laminar flow is necessary and the flow geometry of the measuring system has
to be designed accordingly. Thus, a parabolic flow profile is assumed for the
simulation. The liquid-filled compartment with a diameter <inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 12.1 mm
and a height of <inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 5 mm is
located above the compartment membrane that is 28 <inline-formula><mml:math id="M11" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m thick. Each ISE has a
diameter <inline-formula><mml:math id="M12" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 12 mm and is
inserted into the respective compartment. The distance between the ISE and
the compartment membrane is <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. At the beginning of the simulation, the
concentration in the extracorporeal circuit is increased from zero to <inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
in order to obtain the step response of the system. In reality, there are
usually no discontinuities in concentration during dialysis treatment. A step
in concentration only occurs once at the beginning of the measurement, when
the measuring system is introduced into the extracorporeal circuit. In the
first simulation, the electrolyte concentration in the compartment is set to
zero, corresponding to an initial filling of the compartment with pure water,
leading to much higher absolute measurement errors at the beginning of
measurement than a filling with physiological electrolyte solution. However,
this will give the step response of the system. Inside the extracorporeal
circuit, the transport of electrolytes is dominated by convection. In
contrast, through the compartment membrane and inside<?pagebreak page562?> the
compartment, diffusion is the only transport phenomenon. Hence, the diffusion coefficients
of the different electrolytes and urea are important parameters regarding the
time required to reach a concentration equilibrium between blood and the
fluid in the compartment. These are specified with approximately
<inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">K</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M16" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.9 <inline-formula><mml:math id="M17" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for
potassium (Friedman and Kennedy, 1955),
<inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Na</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M22" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.4 <inline-formula><mml:math id="M23" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for sodium
(Vitagliano and Lyons, 1956) and
<inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Ca</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M28" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M29" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M30" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M31" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for calcium
(Lyons and Riley, 1954). The diffusion coefficient for urea is approximately
<inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Urea</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M34" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.4 <inline-formula><mml:math id="M35" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Gosting
and Akeley, 1952). These parameters are used in all simulations for the
liquid phase and the membrane. Due to similar diffusion coefficients of urea
and sodium, only sodium is considered for the following investigation of the
diffusion process. It should be mentioned that the response time of the urea
sensor does not only depend on the velocity of the concentration equalization
between blood and compartment but also on the transport of the urea into the
layer of immobilized urease (here, another dialysis membrane is used to
trap/immobilize the enzymes). Furthermore, the urea biosensor requires time
for the enzymatic conversion of urea into ammonia and ammonium, meaning that
higher response times are expected. The response time of an ISE is only a few
seconds and can therefore be neglected. In addition to the diffusion
coefficient, the distance <inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> between the compartment membrane and the
ISEs has a major effect on the response time, since it mainly defines the
diffusion length and volume of the compartment. Figure 3 shows the step
response of the calcium concentration in the compartment close to the ISE,
after a concentration step in the extracorporeal circuit from zero to
<inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, for the distances <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M42" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.9 mm (blue line) and
<inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M44" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 3.5 mm (black dashed line). Both graphs are normalized to
<inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. Figure 3 indicates the strong effect of the distance <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> on the
required time to achieve a concentration equilibrium between the blood and
sensor compartment. Additional simulations have shown that the impact of the
height <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">k</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be neglected.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p id="d1e711">Comparison of the concentration in the sensor compartment close to
the ISE between <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M49" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.9 mm (blue solid line) and
<inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M51" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 3.3 mm (black dashed line) versus the time <inline-formula><mml:math id="M52" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> after a step in
concentration of the extracorporeal circuit from zero to <inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, normalized
to the highest concentration <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. The diffusion coefficient is
<inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Ca</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M56" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M57" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M58" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M60" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f03.png"/>

      </fig>

      <p id="d1e845">The impact of the diffusion coefficient can be seen in Fig. 4. Here, the
concentrations of potassium (red dashed line), sodium (blue solid line) and
calcium (black dotted line) normalized to <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> are plotted versus the time
after a step in blood concentration from zero to <inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. As expected, a
higher value of the diffusion coefficient results in a faster equalization.
Hence, the equalization rate for potassium is faster than for sodium. The
slowest equalization rate results for calcium.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p id="d1e873">Impact of the different diffusion coefficients <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">K</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> with
1.9 <inline-formula><mml:math id="M64" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for potassium (red dashed line),
<inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Na</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> with 1.4 <inline-formula><mml:math id="M69" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for sodium
(blue solid line) and <inline-formula><mml:math id="M73" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Ca</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> with
0.9 <inline-formula><mml:math id="M74" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for calcium (black dotted line)
on the step response of the concentration in the sensor compartment.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f04.png"/>

      </fig>

      <p id="d1e1037">Both the impact of <inline-formula><mml:math id="M78" display="inline"><mml:mi>D</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are depicted in Fig. 5. Here, the time
<inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">99</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> required for a concentration equalization of 99 % between the
blood and sensor compartment is plotted versus the distance <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the
diffusion coefficients <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">K</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (red dashed line), <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Na</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
(blue solid line) and <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Ca</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (black dotted line) as parameters. Once
again, Fig. 5 illustrates the disproportionality between equalization time
<inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">99</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. Therefore, it is important to reduce <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> as much as
possible in order to improve the response time of the system. However, an
unlimited reduction of <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is not possible as a direct contact between
the sensitive layer of the ISEs and the compartment membrane has to be
avoided. In addition, the ISEs require a minimum volume of liquid sample. In
our first experimental setup <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> was set to 0.9 mm. Hence, this case
will be investigated in the following simulations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p id="d1e1172">Simulation of the required time <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">99</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for 99 % of
concentration equalization between blood and sensor compartment versus the
distance <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for diffusion coefficients
<inline-formula><mml:math id="M92" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">K</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M93" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.9 <inline-formula><mml:math id="M94" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M95" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (red dashed
line), <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Na</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M99" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1.4 <inline-formula><mml:math id="M100" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M101" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M102" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M103" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>
(blue solid line) and
<inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Ca</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M105" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.9 <inline-formula><mml:math id="M106" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M107" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> m<inline-formula><mml:math id="M108" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> s<inline-formula><mml:math id="M109" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (black
dotted line).</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f05.png"/>

      </fig>

      <p id="d1e1380">Since the treatment duration of CRRT is up to 72 h, the exchange velocity of
the electrolyte in the plasma is usually slow. In the following simulation an
exponentially decrease of the blood concentration <inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> in
the extracorporeal circuit is assumed according to Eq. (2) and the
compartment is now prefilled with a physiological electrolyte solution.

              <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M111" display="block"><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">end</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mfenced close=")" open="("><mml:mn mathvariant="normal">0.9</mml:mn></mml:mfenced><mml:mo>⋅</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:msup><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>

        where <inline-formula><mml:math id="M112" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> is the time in hours, <inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">end</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the limit of
<inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> as <inline-formula><mml:math id="M115" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> approaches infinity, representing the average of
normal blood concentration in healthy humans, and <inline-formula><mml:math id="M116" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the
difference between <inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">end</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at the
beginning of the simulation which decreases with 10 % h<inline-formula><mml:math id="M119" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.</p>
      <?pagebreak page563?><p id="d1e1546">For potassium <inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">end</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is approximately 4.5 mmol L<inline-formula><mml:math id="M121" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. As a worst
case scenario, we assume that <inline-formula><mml:math id="M122" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> for potassium has a
maximum of 9 mmol L<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at the beginning of the dialysis course,
resulting in a <inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 4.5 mmol L<inline-formula><mml:math id="M125" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Figure 6 shows
<inline-formula><mml:math id="M126" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> (red dashed line) and the corresponding concentration
of the compartment <inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (solid red line). The distance <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
between the compartment membrane and the ISE is 0.9 mm. <inline-formula><mml:math id="M129" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> starts
at 4.5 mmol L<inline-formula><mml:math id="M130" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> at the beginning of the simulation since the
compartment is now prefilled with a physiological electrolyte solution. Then,
the compartment concentration increases up to the <inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>.
After the intersection of both concentrations at approximately 21 min,
<inline-formula><mml:math id="M132" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> follows the blood concentration. The corresponding absolute
error <inline-formula><mml:math id="M133" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> for potassium is shown in Fig. 7a (red solid line) and is
calculated according to Eq. (3):

              <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M134" display="block"><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>F</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

        At the beginning of the simulation, <inline-formula><mml:math id="M135" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> starts at <inline-formula><mml:math id="M136" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>4.5 mmol L<inline-formula><mml:math id="M137" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.
After the intersection, where <inline-formula><mml:math id="M138" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M139" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0 mmol L<inline-formula><mml:math id="M140" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, the absolute error
overshoots to a maximum error of only <inline-formula><mml:math id="M141" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M142" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.018 mmol L<inline-formula><mml:math id="M143" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
then decreases exponentially to zero. The corresponding relative error <inline-formula><mml:math id="M144" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>
for potassium according to Eq. (4) is depicted in Fig. 7b (red solid line).

              <disp-formula id="Ch1.E4" content-type="numbered"><mml:math id="M145" display="block"><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>F</mml:mi><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>⋅</mml:mo><mml:mn mathvariant="normal">100</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi></mml:mrow></mml:math></disp-formula>

        The required accuracies and error bands are obtained from the guidelines of
the German Medical Association (Bundesärztekammer, 2014). For potassium,
an error band of <inline-formula><mml:math id="M146" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>4.5 % has to be ensured, resulting in a settling
time of approximately 7.5 min after starting the treatment/measurement.
After the overshoot, the maximum relative error <inline-formula><mml:math id="M147" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> is just about
<inline-formula><mml:math id="M148" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.2 % for the rest of the treatment.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><caption><p id="d1e1894">Response of the sensor compartment potassium
concentration <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (solid line) to a time-dependent blood
potassium concentration <inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> for a distance <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of
0.9 mm. The initial compartment concentration is 4.5 mmol L<inline-formula><mml:math id="M152" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The
difference <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> between the initial value of
<inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M155" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 9 mmol L<inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and end value of
<inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M158" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 4.5 mmol L<inline-formula><mml:math id="M159" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> decreases exponentially with
10 % per hour.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f06.png"/>

      </fig>

      <p id="d1e2035">The same observation can be applied for sodium. Here, however,
<inline-formula><mml:math id="M160" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">end</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the initial concentration in the compartment
are 140 mmol L<inline-formula><mml:math id="M161" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and <inline-formula><mml:math id="M162" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is 40 mmol L<inline-formula><mml:math id="M163" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, resulting in an
initial blood concentration <inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> of 180 mmol L<inline-formula><mml:math id="M165" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.
Compared to potassium, the intersection of both <inline-formula><mml:math id="M166" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is approximately 4 min later at 25 min. The corresponding
absolute error <inline-formula><mml:math id="M168" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> and relative error <inline-formula><mml:math id="M169" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> for sodium are depicted in Fig. 7a
and b (blue solid line), respectively. The absolute error <inline-formula><mml:math id="M170" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> starts at
<inline-formula><mml:math id="M171" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>40 mmol L<inline-formula><mml:math id="M172" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. After the intersection point at 25 min, <inline-formula><mml:math id="M173" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula>
overshoots, causing a maximum absolute error <inline-formula><mml:math id="M174" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> of approximately
<inline-formula><mml:math id="M175" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.2 mmol L<inline-formula><mml:math id="M176" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The settling time after starting the
treatment/measurement is about 7.2 min for the required accuracy of
<inline-formula><mml:math id="M177" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>3 %. After the overshoot, the maximum relative error <inline-formula><mml:math id="M178" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> is just
<inline-formula><mml:math id="M179" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.1 % for the rest of the treatment.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><caption><p id="d1e2238">Resulting absolute error <inline-formula><mml:math id="M180" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> between <inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
exponentially decreasing <inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> with 10 % h<inline-formula><mml:math id="M183" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for a
distance <inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M185" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.9 mm <bold>(a)</bold> and the corresponding relative
error <inline-formula><mml:math id="M186" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> (solid line) <bold>(b)</bold> for potassium (red line), sodium (blue
line) and calcium (black line). The dashed lines in <bold>(b)</bold> are the
required accuracy of <inline-formula><mml:math id="M187" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>3 % for sodium, <inline-formula><mml:math id="M188" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>4.5 % for potassium
and <inline-formula><mml:math id="M189" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>7.5 % for calcium.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f07.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p id="d1e2352">Photo of the measuring chamber consisting of two parts made of PEEK.
The lower part has the hose connections for the extracorporeal circuit. The
upper part contains the compartment for the ISEs and the hose connections for
the compartment.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f08.png"/>

      </fig>

      <p id="d1e2361">For calcium, <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">end</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the initial concentration in the
compartment is 1.2 mmol L<inline-formula><mml:math id="M191" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">Δ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is 1.3 mmol L<inline-formula><mml:math id="M193" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
resulting in an initial <inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> of 2.5 mmol L<inline-formula><mml:math id="M195" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. The
lowest diffusion coefficient <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">Ca</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> causes the latest intersection
of the two concentrations <inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at
36.5 min. After this intersection point, the absolute error <inline-formula><mml:math id="M199" display="inline"><mml:mi>F</mml:mi></mml:math></inline-formula> overshoots
and has a maximum value of only 9.7 <inline-formula><mml:math id="M200" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>mol L<inline-formula><mml:math id="M201" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, which can be
seen in Fig. 7a (black solid line). Furthermore, the required error band of
<inline-formula><mml:math id="M202" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>7.5 % can be reached within 10.7 min after starting the
treatment/measurement. The maximum relative error <inline-formula><mml:math id="M203" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> for calcium is just
<inline-formula><mml:math id="M204" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>0.4 % for the rest of the treatment.</p>
      <p id="d1e2526">In summary, the relative error <inline-formula><mml:math id="M205" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> after the intersection point of
<inline-formula><mml:math id="M206" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mi mathvariant="normal">blood</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">sim</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mi mathvariant="normal">comp</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is lower than 0.4 % for
calcium, 0.2 % for potassium and 0.1 % for sodium. Due to the
different accuracies required, the settling time varies from 7.2 min for
sodium to 7.5 min for potassium and 10.7 min for calcium after starting the
treatment/measurement. This improves the current standard of discrete
laboratory analyses significantly, which obtain the results with a delay of
several hours. It has to be mentioned that such short settling times of just
a few minutes can be neglected for a treatment duration of 72 h.</p>
</sec>
<?pagebreak page564?><sec id="Ch1.S4">
  <title>Experimental setup</title>
      <p id="d1e2569">The demonstrator of the in-line measuring system is similar to the simulation
model. Figure 8 shows a photo of the flow cell. The schematic cross section
is depicted in Fig. 9. The cell is made of the thermoplastic material PEEK
and consists of two components. Two hose connections are located at the lower
part of the measurement system on the left and right side, allowing the
system to be easily integrated into the extracorporeal circuit independently
of the dialysis apparatus used. The lower part is designed to minimize
turbulent flows as much as possible by avoiding an abrupt change in the
cross section of the flow geometry in order to reduce the mechanical stress
on the blood cells and thus prevent hemolysis. The compartment membrane made
of regenerated cellulose with a molecular weight cutoff from 10 up to
20 kDa, and a thickness of 28 <inline-formula><mml:math id="M208" display="inline"><mml:mi mathvariant="normal">µ</mml:mi></mml:math></inline-formula>m (RCT NatureFlex-NP from Reichelt
Chemietechnik) separates the ISEs from the extracorporeal circuit. The ISEs
and the reference electrode are placed in the upper part of the system. Via
two hose connections in the upper part, the sensor compartment can be
prefilled with a physiological electrolyte solution. Furthermore, the ISEs
can be calibrated this way. The potassium ISE (201/K) and calcium ISE (201/CA) were purchased
from Amel in Italy. As a reference electrode, the InLab Reference electrode
from Mettler Toledo was used. For sodium measurement, the
polymer membrane electrode from Metrohm was used. The concentration-dependent voltage
between the ISEs and reference electrode is recorded by a potentiostat from
PalmSens (Polypotentiostat EmStat3 4WE).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9"><caption><p id="d1e2581">Schematic depiction of the cross section of the measuring system.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f09.png"/>

      </fig>

      <p id="d1e2590">In order to investigate the dynamic behavior of the measuring system, we
simulate the extracorporeal circuit with a synthetic electrolyte solution,
which was pumped from a reservoir into the in-line measuring system via a
hose system and then back into the reservoir with a flow rate of
100 mL min<inline-formula><mml:math id="M209" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> by a peristaltic pump (Ecoline VC-380 from ISMATEC). A
magnetic stirrer (IKA RCT basic) continuously mixed the reservoir. All
chemicals (potassium chloride, sodium chloride and calcium chloride
dihydrate) were bought from Sigma-Aldrich Germany.</p>
      <p id="d1e2605">Hemolysis is an important characteristic of hemocompatibility that needs to
be investigated. Therefore, we have built up a further circulation system
filled with reconfigured human blood at a flow rate of 100 mL min<inline-formula><mml:math id="M210" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>.
In order to determine the amount of hemolysis produced by the measuring
system, the circulation system was first used without the measuring
system for 2 h. After that, the measuring system was integrated into the
circulation system filled with new reconfigured blood. Free hemoglobin was
used as a marker for hemolysis. The different increase of free hemoglobin in
the circulatory system with and without the sensor provides<?pagebreak page565?> information about
the hemolysis produced by the measuring system.</p>
</sec>
<sec id="Ch1.S5">
  <title>Results</title>
      <p id="d1e2627">In order to validate the simulation results, we measured the step response of
the continuous in-line monitoring system with a synthetic electrolyte
solution consisting of the three electrolytes potassium chloride, sodium
chloride and calcium chloride in DI (deionized) water. To prevent the ISEs and reference
electrode from being exposed to DI water for a longer period of time, the
entire extracorporeal circuit and sensor compartment is prefilled with a very
low concentrated electrolyte solution (10<inline-formula><mml:math id="M211" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> mol L<inline-formula><mml:math id="M212" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) of sodium
chloride, potassium chloride and calcium chloride. It should be noted that
these low concentrations are not expected in the later application with real
blood. To obtain the step response of the in-line measuring system, the
concentrations are raised from zero to
<inline-formula><mml:math id="M213" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M214" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M215" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> mol L<inline-formula><mml:math id="M216" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
<inline-formula><mml:math id="M217" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M218" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M219" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> mol L<inline-formula><mml:math id="M220" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for sodium and potassium and
<inline-formula><mml:math id="M221" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">Ca</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M222" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M223" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> mol L<inline-formula><mml:math id="M224" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> for calcium inside the
reservoir. The distances <inline-formula><mml:math id="M225" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> between dialyses membrane and ISEs are
approximately 0.9 mm. Figure 10 shows the corresponding step response for
potassium (red solid line) and sodium (blue solid line) normalized to
<inline-formula><mml:math id="M226" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M227" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> and calcium (black solid line)
normalized to <inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:msub><mml:mi>c</mml:mi><mml:mrow><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">Ca</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, respectively. As shown before, the
differences of the equalization time are caused by the different diffusion
coefficients resulting in the fastest equalization for potassium and the
slowest equalization for calcium. Furthermore, Fig. 10 compares the measured
and simulated step responses for a distance <inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of 0.9 mm. It can be
seen that the measured step responses are very similar to the simulated
curves. Hence, the simulated error analysis applies to the demonstrator of
the in-line measuring system. It should be mentioned that ISEs are not
perfectly selective to particular ion species, resulting in
cross-sensitivities to other ion species described by the selectivity
coefficient <inline-formula><mml:math id="M230" display="inline"><mml:mrow><mml:msub><mml:mi>k</mml:mi><mml:mrow><mml:mi mathvariant="normal">A</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">B</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> between the target ion A and the interfering ion
B in the Nikolsky–Eisenman equation. Due to the different charge number of, e.g., calcium and potassium, the Nikolsky–Eisenman equation results in a
nonlinear 3 <inline-formula><mml:math id="M231" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3 equation system for the three electrolytes of
interest. Since manufacturers obtain the selectivity coefficients <inline-formula><mml:math id="M232" display="inline"><mml:mi>k</mml:mi></mml:math></inline-formula> for
each ISE, interferences can be corrected between all measured ions using
Newton's method. Furthermore, ISEs are actually sensitive to ion activities
and not to ion concentrations. The activity coefficient relates the activity
to the concentration. In particular, the activity deviates from the
concentration at high electrolyte concentrations. However, if the calibration
solutions have similar activities to blood, it is possible to neglect the
effect of the concentration-dependent variation of the activity coefficient
since the blood concentration can only vary within a limited range. For
instance, in the worst case the concentration of potassium can vary between
1.5 and 9 mmol L<inline-formula><mml:math id="M233" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, for sodium between 120 and 180 mmol L<inline-formula><mml:math id="M234" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> and
for ionized calcium between 0.6 and 2.5 mmol L<inline-formula><mml:math id="M235" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. It should be noted
that ISEs only determine the ionized calcium and not the complexed calcium.
In this particular application, the impact of the temperature of the
measuring medium on the sensor signal can also be neglected, as the
temperature of the blood can only vary within a narrow range. In the worst
case the body temperature can be between 33 and 41 <inline-formula><mml:math id="M236" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. In addition,
the temperature of the extracorporeal circuit is controlled to reduce the
fluctuation of the temperature even further. During a 72 h CRRT it is
possible that the sensor signal has a drift over the time. However, it is
conceivable to recalibrate the ISEs via the hose connection of the sensor
compartment and thus guarantee high-precision measurements of the
concentrations. At a flow rate of 100 mL min<inline-formula><mml:math id="M237" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> within the
extracorporeal circuit, the standard deviation of the voltage between the ISE
and the Ag/AgCl reference electrode is about
1.33 <inline-formula><mml:math id="M238" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 10<inline-formula><mml:math id="M239" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> V, leading to a standard deviation of the
concentration of 0.05 % for monovalent ions and 0.1 % for divalent
ions, which has to be considered in the overall error. This low standard
deviation is achieved by averaging the measurement signal using an averaging
time of 1 s. In addition, we use a metal housing for shielding, which
considerably reduces the noise and thus the standard deviation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10"><caption><p id="d1e2977">Comparison between the measured step response (solid lines) and the
simulated response (dotted lines) for potassium (red line), sodium (blue
line) and calcium (black line). The distance <inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:msub><mml:mi>h</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> between the ISEs and
compartment membrane is about 0.9 mm.</p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://jsss.copernicus.org/articles/7/559/2018/jsss-7-559-2018-f10.png"/>

      </fig>

      <p id="d1e2997">The circulation system filled with reconfigured human blood was used to
determine the amount of hemolysis caused by the measuring system at a flow
rate of 100 mL min<inline-formula><mml:math id="M241" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>. Due to increasing hemolysis of reconfigured
blood in the circulation system, the value of free hemoglobin rises
continuously during the 2 h measurement. The different amount of free
hemoglobin in reconfigured blood between the circulation system with and
without the measuring system is therefore a measure of the hemolysis produced
by the measuring system. We observed no difference in increasing free
hemoglobin between the setup with or without the sensor. Therefore, we exclude significant hemolysis in this first experiment.</p><?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page566?><sec id="Ch1.S6" sec-type="conclusions">
  <title>Conclusion</title>
      <p id="d1e3019">In this work, we presented the concept and preliminary investigations of a
concept for a continuous in-line monitoring of electrolytes during CRRT that
meets the fluidic requirements for hemocompatibility. First investigations of
hemocompatibility show no increased hemolysis caused by the measuring system.
However, it should be noted that hemocompatibility does not only mean
hemolysis. Further tests with real blood (e.g., blood clotting) are still
ongoing and experimental proof of hemocompatibility is pending. In this study, the ISEs
used are separated from direct blood flow using a dialysis membrane
(compartment membrane), preventing the adsorption of, e.g., proteins on the
sensor surface. The dynamics of the in-line measuring system is an important
factor affecting the resulting measurement error. By reducing the volume of
the compartment containing the ISEs, the system dynamics can be improved.
With this measuring system, the required accuracy is reached 10.7 min after
starting the measurement for calcium, after 7.5 min for potassium and after
7.2 min for sodium. After this short settling time caused by the initial
concentration step that only occurs at the beginning of the
treatment/measurement, the presented concept enables a continuous in-line
measurement with a relative error less than 0.5 % for calcium, 0.25 %
for potassium and 0.15 % for sodium, significantly improving the current
method of laboratory analysis, which obtains the results with a delay of
several hours. Due to the continuous monitoring, the concentration gradients
between blood and dialysate can be determined precisely and thus the exchange
velocity of electrolytes can be controlled by individualizing the dialysate
composition, resulting in a benefit especially for critically ill patients in
the ICU, since a rapid change of osmotic substances can lead to complications.
Furthermore, the in-line system provides the possibility to be extended by a
urea sensor to determine the efficiency of dialysis treatment.</p>
      <p id="d1e3022">In further work, we will investigate this concept in a clinical study. In
addition, we will reduce the size of the measurement system by using
miniaturized sensors like ion-selective field-effect transistors (ISFETs).
Furthermore, we will investigate the urea sensor. In this study, we use a very simple
approach in which the enzyme is retained by another dialysis membrane and
thus immobilized close to an ammonium electrode. Hence, the use of toxic
chemicals for immobilization can be avoided.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability">

      <p id="d1e3029">All underlying research data are given in this paper. There is no supplementary or
additional underlying material.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e3035">The authors declare that they have no conflict of
interest.</p>
  </notes><notes notes-type="sistatement">

      <p id="d1e3041">This article is part of the special issue “Dresden Sensor
Symposium 2017”. It is a result of the Dresden Sensor Symposium 2017,
Dresden, Germany, 4–6 December 2017.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e3047">This research is sponsored by the German Federal Ministry of Education and Research (BMBF)
under grant 13GW0085B.<?xmltex \hack{\newline\newline}?>
Edited by: Winfried Vonau <?xmltex \hack{\newline}?>
Reviewed by: two anonymous referees</p></ack><ref-list>
    <title>References</title>

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    <!--<article-title-html>Continuous in-line monitoring of electrolyte concentrations in extracorporeal circuits for individualization of dialysis treatment</article-title-html>
<abstract-html><p>One objective of dialysis treatment is to normalize the blood
plasma electrolytes and remove waste products such as urea and creatinine
from blood. However, due to a shift in plasma osmolarity, a rapid or
excessive change of the electrolytes can lead to complications like
cardiovascular instability, overhydrating of cells, disequilibrium syndrome
and cardiac arrhythmias. Especially for critical ill patients in intensive
care unit with sepsis or multi-organ failure, any additional stress has to be
avoided. Since the exchange velocity of the electrolytes mainly depends on
the concentration gradients across the dialysis membrane between blood and
dialysate, it can be controlled by an individualized composition of dialysate
concentrations. In order to obtain a precise concentration gradient with the
individualized dialysate, it is necessary to continuously monitor the plasma
concentrations. However, with in-line sensors, the required hemocompatibility
is often difficult to achieve. In this work, we present a concept for
continuous in-line monitoring of electrolyte concentrations using
ion-selective electrodes separated from the blood flow by a dialysis
membrane, and therefore meeting the fluidic requirements for
hemocompatibility. First investigations of hemocompatibility with
reconfigured human blood show no increased hemolysis caused by the measuring
system. With this concept, it is possible to continuously measure the plasma
concentrations with a relative error of less than 0.5&thinsp;%.</p></abstract-html>
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