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As shown in "First prototype" section, the strain measured by the prototype sensor is smaller than the theoretical values above T g.
Substituting the strain measured by the prototype sensor into the linear approximation formula in Fig. 5, we calculated the applied force.
Substituting the strain measured by the prototype sensor into the linear approximation formula in Fig. 5, we calculated the applied force and compared it with that obtained by the load cell when a random force was applied.
Substituting the strain measured by the prototype sensor into the linear approximation formula in Fig. 5, we calculated the applied force Fig. 7 Comparison of two forces measured by first prototype sensor and load cell when a random force was applied (T > T g).
Substituting the strain measured by the prototype sensor into the linear approximation formula in Fig. 11a, we calculated the applied force Fig. 14 Comparison of two forces measured by second prototype sensor and load cell when a random force was applied (T > T g, h T = 0.05 mm).
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The performances of the prototype sensor are characterized by cyclic voltammetry and fixed potential amperometry techniques.
The prototype sensor is tested by monodisperse aerosols with particle sizes ranging from 200 nm to 2000 nm.
The concept design and the prototype sensor had been validated by experimental studies in laboratory.
The prototype sensor dimensions were decided by considering the average size of the lower jaw and curvature near the lower jaw and neck of the subjects in the tests (see "Experiments and data acquisition" section below).
The prototype sensor was automatically displaced using an automatic stage Fig. 4 Thermographic image of the prototype force sensor using an SMP sheet heated above T g.
The prototype sensor is a Kapton®-based three-layered structure.
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