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Li et al. Soft Sci. 2025, 5, 13  https://dx.doi.org/10.20517/ss.2024.60          Page 5 of 11

               the fibrous temperature sensor clearly demonstrated the core-shell structure that comprises a sensing core
               and a protective layer [Figure 1B]. Through this impregnation plant, the fibrous temperature sensors could
               be fabricated on a large scale with a high degree of automation [Figure 1C]. Moreover, they could be
               stitched and embroidered using a commercial sewing machine [Figure 1D].


               The sensing mechanism of the fibrous temperature sensor is intricately linked to the temperature-
               dependent  conductive  behavior  of  the  ionic  liquid,  1-ethyl-3-methylimidazolium  bis
               (trifluoromethanesulfonyl) imide salt. This behavior is governed by the Vogel-Tammann-Fulcher (VTF)
               law, which describes the temperature dependence of the viscosity and the ionic conductivity of the
               liquid [35-37] . As the temperature increases, the ionic mobility within the liquid also increases due to the
               decreased viscosity. This enhanced mobility allows ions to move more freely, leading to an increase in
               conductivity. The VTF law captures this non-Arrhenius temperature dependence of conductivity, where the
               conductivity does not increase linearly with temperature but rather follows a more complex exponential
               relationship. This change in conductivity is directly measured by the sensor, providing a means to correlate
               resistance changes with temperature fluctuations. In order to study the electrical characteristics of the
               developed fibrous temperature sensors, The I-V characteristic curves of the fibrous temperature sensor at
               different temperatures were measured. Under a fixed voltage of 10 V, the current exhibited a increase from
               0.185 μA at 0 °C to 2.526 μA at 100 °C [Figure 2A]. The resistance of fibrous sensors decreased gradually
               with increased temperature from 0 to 100 °C, exhibiting a notable negative temperature coefficient behavior
               in Figure 2B. The response time and recovery time of the fibrous temperature sensor were also investigated
               and measured by a conventional method. The results are shown in Figure 2C. The response time and
               recovery time of the sensor were calculated to be 6 and 8 s, respectively, which showed that the temperature
               sensor has a rapid response to temperature variations and is beneficial for real-time skin temperature
               monitoring. To achieve an effective measurement of human body temperature, the response curve of the
               fibrous temperature sensor from 25 to 40 °C was investigated in detail. The heating and cooling curves
               between 25 and 40 °C were measured for the fibrous temperature sensor [Figure 2D]. The results indicated
               that the sensor display high resilience during the heating and cooling process. As shown in Figure 2E, the
               fibrous temperature sensor exhibited good linearity and high sensitivity (|ΔR|/R /ΔT = 2.61%/°C), indicating
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               that the sensor’s resistance change is proportional to the temperature variation within the tested range of 25
               to 40 °C. This linear relationship is crucial for the accurate and reliable monitoring of body temperature, as
               it enables the sensor to provide precise temperature readings based on the measured resistance changes.
               Compared to the existing fibrous temperature sensors, the temperature sensor we prepared has excellent
               temperature sensing performance with the highest sensitivity in temperatures ranging from 25 to 40 °C [
               Figure 2F and Supplementary Table 1].

               Subsequently, the resistance of the fibrous temperature sensor to external interference, including pressing,
               bending, twisting, pH, and humidity, was investigated. The temperature response of the sensor was
               examined under a range of compressive forces from 0 to 10 N. This was done to simulate the effects of
               mechanical stress that the sensor might encounter in practical applications. The results showed that the
               fibrous temperature sensor maintains its original performance across the entire range of applied forces,
               demonstrating its robustness under mechanical stress [Figure 3A]. We also assess the sensor’s temperature
               detection capabilities under different bending angles varying from 0° to 360° at room temperature. This test
               was crucial to evaluate the sensor’s flexibility and durability. The evaluations confirmed that the fibrous
               temperature sensor can withstand severe bending without affecting its detection results, highlighting its
               flexibility and reliability [Figure 3B]. Moreover, the sensor was twisted to varying degrees, and its resistance
               was monitored throughout the process. The results show that the fibrous temperature sensor can withstand
               twisting without compromising its temperature-sensing capabilities [Supplementary Figure 1A].
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