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MATERIALS         47
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          solutions  (LiCl,  RH  =  10%;  MgCl2,  RH  =  33%,  NaNO2,  RH   where:
          = 65%, NaCl, RH = 75%; ZnSO4, RH = 87%) providing the   Cs1 capacitance of the empty capacitor [F]
          six specified humidity levels (Table 1).              Cs2 capacitance with the test specimen inserted [F]
            Density was determined for each lamella based on oven-  tg distance between the capacitor electrodes [m]
          dry mass and conditioned volume before measurement. The   td average thickness of the test specimen [m]
          density was not experimentally controlled, but samples were   D1 loss factor of the empty capacitor

          taken  to  more  closely  mimic  industrial  conditions  where  it  is   D2 loss factor of the capacitor with the specimen.
          not possible to experimentally control the density, but only the
          texture of the element, which is, for aesthetic reasons, radial   The  relative  dielectric  constant  was  calculated  indirectly
          as were the samples used in this experiment.       using Equation, while the dielectric loss factor was determined
            After conditioning, specimens were sealed in polyethylene   using Equation. Measurements were conducted at two sample
          bags to prevent moisture exchange prior to measurement. The   temperatures: 20 deg C and 90 deg C.
          steamed group was prepared separately by exposing lamellas   These two temperatures represent room temperature and
          to saturated steam at 90 deg C for 90 min, after which they   the typical temperature used when preheating wood elements
          were cooled in sealed containers to avoid uncontrolled drying.   before bending. A total of 26 electric field frequencies ranging

          This ensured that the steaming treatment primarily affected the   from 0.079 MHz to 25.1
          softening of polymers without inducing large moisture gradients.  MHz were applied which represent lower industrial microwave
                                                             and  radio-frequency  heating  domain.  Before  the  dielectric
          Measuring of Dielectric Properties                 measurements at 90 deg C, the oak lamellas were wrapped
          The  dielectric  properties  were  measured  using  an  Agilent   in aluminium foil and preheated to the target temperature in
          4285A  LCR  metre  and  a  16451B  Dielectric  Test  Fixture  in   a laboratory oven.
          accordance with ASTM D150-22.                         This procedure ensured that the samples maintained their

            Properties  were  measured  at  20  deg  C  and  90  deg  C,   original moisture content and temperature during the test.
          across  six  humidity  levels  and  26  frequencies.  In  this  study,   All measurements were performed with the fibre orientation
          dielectric properties were measured with electric field frequencies   aligned parallel to the electric field (longitudinal direction).
          ranging  from  0.079  MHz  to  25.119  MHz.  During  testing,  the   Each  frequency  sweep  was  repeated  twice  to  verify
          lamella samples were positioned between two capacitor plates.  repeatability;  the  mean  values  were  used  for  statistical
            Before  measurement,  the  capacitance  and  dissipation
          factor  of  the  empty  capacitor  (C1,  D1)  were  recorded  at
          each frequency. The specimen was then placed between the
          electrodes, maintaining a constant spacing of 0.5 mm (verified                                      www.freepik.com

          by micrometre).
             Capacitance and dissipation factor with the sample (C2,
          D2)  were  measured  under  identical  conditions.  The  relative
          dielectric constant (ε′) and dielectric loss tangent (tan δ) were
          calculated according to ASTM D150-22 as:
            ε = 1/(1 − 1(1 − Cs1/Cs2) × tg/td)
            Dt = D2 + εr × (D2 − D1) × (tg/td − 1)
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