2016
DOI: 10.1039/c6ra22872k
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Piezo-resistive and thermo-resistance effects of highly-aligned CNT based macrostructures

Abstract: Recent advances in assembling Carbon NanoTubes (CNTs) into macrostructures with outstanding properties, such as high tensile strength, high conductivity and porosity, and strong corrosive resistance, have underpinned potentially novel applications.

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Cited by 21 publications
(13 citation statements)
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References 67 publications
(63 reference statements)
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“…Nowadays, among various sensors to detect human motion and monitor health condition, piezoresistive sensors (PRSs), which are typical sensors that transduce the external pressure into the resistance signal, have been widely used in wearable devices due to their advantages of cost‐efficient fabrication and simple structure . Normal PRSs with conductive polymers or particles are proved suitable sensing materials, but these materials are confronted with low sensitivity and poor stability especially in low‐pressure regimes. Different from the conventional PRSs, conductive porous sponges or foams have been developed, which are considered as alternative materials owing to their synergistic effect of high conductivity of active materials and excellent mechanical property of porous scaffold.…”
Section: Introductionmentioning
confidence: 99%
“…Nowadays, among various sensors to detect human motion and monitor health condition, piezoresistive sensors (PRSs), which are typical sensors that transduce the external pressure into the resistance signal, have been widely used in wearable devices due to their advantages of cost‐efficient fabrication and simple structure . Normal PRSs with conductive polymers or particles are proved suitable sensing materials, but these materials are confronted with low sensitivity and poor stability especially in low‐pressure regimes. Different from the conventional PRSs, conductive porous sponges or foams have been developed, which are considered as alternative materials owing to their synergistic effect of high conductivity of active materials and excellent mechanical property of porous scaffold.…”
Section: Introductionmentioning
confidence: 99%
“…The resistance variations of hotwires were then converted to the velocity of ion wind by comparing the heat transfer coefficient of forced convection, from generated ion winds with that of natural convection from a still air [ 44 ], where is the thermal conductivity, Ra is the Rayleigh number, d is the effective diameter of the hotwire, and is the Reynolds number. The process was carried out using an subroutine C-code, which has been detailed in our recent publications [ 45 , 46 , 47 , 48 ]. The average velocities calculated from output voltage are plotted in Figure 7 b.…”
Section: Resultsmentioning
confidence: 99%
“…The voltage of hotwires is used to determine the average velocity of flow at local areas around hotwire positions by comparing the heat transfer coefficient of forced convection(0.24 + 0.56 0.45 ⁄ ) with one by the natural convection (1.02 0.1 ) ⁄ of air with , Ra and d the thermal conductivity, Rayleigh number, effective diameter of the hotwire, respectively; and the Reynolds number of air flow. The calculation is carried out using our subroutine C-code whose details can be found in our recent publications [45], [46].…”
Section: Characterization Of Vortex Flow Using Hotwire Anemometrymentioning
confidence: 99%