Flexible Normal-Tangential Force Sensor with Opposite Resistance Responding for Highly Sensitive Artificial Skin

2018 ◽  
Vol 28 (18) ◽  
pp. 1707503 ◽  
Author(s):  
Chunhong Mu ◽  
Yuanqiang Song ◽  
Wutong Huang ◽  
Ao Ran ◽  
Rujie Sun ◽  
...  
2008 ◽  
Vol 24 (1) ◽  
pp. 43-50 ◽  
Author(s):  
Adriana V. Savescu ◽  
Mark L. Latash ◽  
Vladimir M. Zatsiorsky

This article proposes a technique to calculate the coefficient of friction for the fingertip– object interface. Twelve subjects (6 males and 6 females) participated in two experiments. During the first experiment (the imposed displacement method), a 3-D force sensor was moved horizontally while the subjects applied a specified normal force (4 N, 8 N, 12 N) on the surface of a sensor covered with different materials (sandpaper, cotton, rayon, polyester, and silk).Thenormal forceand thetangential force(i.e., the force due to the sensor motion) were recorded. Thecoefficient of friction(µd) was calculated as the ratio between the tangential force and the normal force. In the second experiment (the beginning slip method), a small instrumented object was gripped between the index finger and the thumb, held stationary in the air, and then allowed to drop. The weight (200 g, 500 g, and 1,000 g) and the surface (sandpaper, cotton, rayon, polyester, and silk) in contact with the digits varied across trials. The same sensor as in the first experiment was used to record thenormal force(in a horizontal direction) and thetangential force(in the vertical direction). Theslip force(i.e., the minimal normal force or grip force necessary to prevent slipping) was estimated as the force at the moment when the object just began to slip. The coefficient of friction was calculated as the ratio between the tangential force and the slip force. The results show that (1) the imposed displacement method is reliable; (2) except sandpaper, for all other materials the coefficient of friction did not depend on the normal force; (3) theskin–sandpapercoefficient of friction was the highest µd= 0.96 ± 0.09 (for 4-N normal force) and theskin–rayonrayon coefficient of friction was the smallest µd= 0.36 ± 0.10; (4) no significant difference between the coefficients of friction determined with the imposed displacement method and the beginning slip method was observed. We view the imposed displacement technique as having an advantage as compared with the beginning slip method, which is more cumbersome (e.g., dropped object should be protected from impacts) and prone to subjective errors owing to the uncertainty in determining the instance of the slip initiation (i.e., impeding sliding).


2014 ◽  
Vol 26 (17) ◽  
pp. 2659-2664 ◽  
Author(s):  
Lucie Viry ◽  
Alessandro Levi ◽  
Massimo Totaro ◽  
Alessio Mondini ◽  
Virgilio Mattoli ◽  
...  

2014 ◽  
Vol 22 (3) ◽  
pp. 3578 ◽  
Author(s):  
Yuan Gong ◽  
Cai-Bin Yu ◽  
Ting-Ting Wang ◽  
Xiu-Ping Liu ◽  
Yu Wu ◽  
...  

Author(s):  
Nouha Al Cheikh ◽  
Caroline Coutier ◽  
Jean Brun ◽  
Christophe Poulain ◽  
Henri Blanc ◽  
...  

2012 ◽  
Vol 24 (8) ◽  
pp. 700-702 ◽  
Author(s):  
Kit Man Chung ◽  
Zhengyong Liu ◽  
Chao Lu ◽  
Hwa-Yaw Tam

2020 ◽  
Vol 7 (1) ◽  
Author(s):  
An Hoang-Thuy Nguyen ◽  
Manh-Cuong Nguyen ◽  
Seongyong Cho ◽  
Anh-Duy Nguyen ◽  
Hyewon Kim ◽  
...  

Abstract This paper presents a straightforward, low-cost, and effective integration process for the fabrication of membrane gate thin film transistors (TFTs) with an air gap. The membrane gate TFT with an air gap can be used as the highly sensitive tactile force sensor. The suspended membrane gate with an air gap as the insulator layer is formed by multiple photolithography steps and photoresist sacrificial layers. The viscosity of the photoresist and the spin speed was used to modify the thickness of the air gap during the coating process. The tactile force was measured by monitoring the drain current of the TFT as the force changed the thickness of the air gap. The sensitivity of the devices was enhanced by an optimal gate size and low Young’s modulus of the gate material. This simple process has the potential for the production of small, versatile, and highly sensitive sensors.


2014 ◽  
Vol 26 (17) ◽  
pp. 2610-2610 ◽  
Author(s):  
Lucie Viry ◽  
Alessandro Levi ◽  
Massimo Totaro ◽  
Alessio Mondini ◽  
Virgilio Mattoli ◽  
...  

Author(s):  
Yusuke Miyazaki ◽  
Kazuki Iida ◽  
Motomu Nakashima ◽  
Takeo Maruyama ◽  
Kaohru Yamanobe

To improve competitive skills, it is important to clarify the relationship between the propulsion motion (the propulsive force in the use of racing wheelchairs optimized for athletes) and aerodynamic drag, which can change during propulsive motion. Therefore, the purpose of this research was to construct a novel force sensor system that is attachable to racing wheelchairs for individual athletes and usable in a wind tunnel facility to examine differences in the push-rim force characteristics of athletes based on the measured results. The system was composed of four two-dimensional component force sensors, batteries, and radio transmitters. From the output of the four two-dimensional component sensors, tangential and radial components of the push-rim force were measured. Three top-class long-distance wheelchair athletes participated in this study, which required each athlete to push a racing wheelchair at 5.56 m/s on a wheelchair roller system in a wind tunnel facility. The force sensor system was mounted on the participants’ individual racing wheelchairs. The measured tangential force waveforms were classified as either bimodal or unimodal depending on the athletes’ propulsion styles. Although two athletes showed similar propulsion style characteristics, the athlete with more years of experience showed better propulsive work efficiency and repeatability. Therefore, a difference in skill for applying propulsive force during the push phase, which is difficult to estimate by kinematic analysis, could be estimated by using the force sensor system.


2015 ◽  
Vol 26 (11) ◽  
pp. 115203 ◽  
Author(s):  
Guoyu Tang ◽  
Jue Wei ◽  
Wei Zhou ◽  
Meichao Yang ◽  
Mingyu Wu ◽  
...  

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