A deformable smart skin for continuous sensing based on electrical impedance tomography

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Abstract

In this paper, we present a low-cost, adaptable, and flexible pressure sensor that can be applied as a smart skin over both stiff and deformable media. The sensor can be easily adapted for use in applications related to the fields of robotics, rehabilitation, or costumer electronic devices. In order to remove most of the stiff components that block the flexibility of the sensor, we based the sensing capability on the use of a tomographic technique known as Electrical Impedance Tomography. The technique allows the internal structure of the domain under study to be inferred by reconstructing its conductivity map. By applying the technique to a material that changes its resistivity according to applied forces, it is possible to identify these changes and then localise the area where the force was applied. We tested the system when applied to flat and curved surfaces. For all configurations, we evaluate the artificial skin capabilities to detect forces applied over a single point, over multiple points, and changes in the underlying geometry. The results are all promising, and open the way for the application of such sensors in different robotic contexts where deformability is the key point.

Figures

  • Figure 1. Example of bipolar adjacent pattern. Two electrodes are selected as the driving ones, while all the others are used to measure the electric potentials generated between adjacent pairs. The injection and measurement pattern is than switched by changing the driving electrodes until a full cycle is completed. Electric potentials measured at the driving electrodes are commonly not taken in order to ensure stability in the acquired data. In the image, dark-grey lines indicate iso-potential areas, while the current flow is shown in blue.
  • Figure 2. Schematic overview of the driving and readout electronics. The image depicts the configuration for a generic channel and its components. By using this configuration, a single channel can be set as: (i) current source; (ii) current sink (ground electrode); or (iii) used to measure the electric potentials with respect to an external common ground. The process is controlled by the two independent de-multiplexers connected at each channel. DAQ: data acquisition board. In the figure, Q1 is the NPN transistor, Q2 and Q3 respectively the P-MOSFET and N-MOSTEF, U1 is the INA118, U2 is the OPA827, and U3 is the TLV2371.
  • Figure 3. Smart skin with wiring. (a) The conductive textile is attached over a stretchable foam that allows better discrimination between normal forces and stretching, and creates an insulation layer that allows the artificial skin to be applied over different materials. The current version of the system uses only eight channels that are connected by alligator clip to the measurement system. (b) Possible application scenario attached over a dummy doll arm.
  • Figure 4. Schematic view of the experimental setup. The artificial skin is connected by wire to the ad-hoc developed driving/read-out circuit. This is connected to a microcontroller that sets the status of the different channel and functions as a digital acquisition board. The whole system is then connected to a laptop on which the main program and the inverse solver are running.
  • Figure 5. Electric potentials measured at Electrode 3 (E3) in an eight-channel configuration. Measurements were taken using an adjacent pattern, in both excitation and acquisition phases. The positive peaks correspond when the electrode is “close” to ground nodes. On the contrary, the negative peak occurs when E3 is used as a current sink. Error bars show the variability of measurements calculated over 10 samples.
  • Figure 6. Electric potentials measured at Electrode 6 (E6) in an eight-channel configuration. Measurements were taken using an adjacent pattern in both excitation and acquisition phases. The positive peaks correspond when the electrode is “close” to ground nodes. On the contrary, the negative peak occurs when E6 is used as a current sink. Error bars show the variability of measurements calculated over 10 samples.
  • Figure 7. Electric potentials measured at each electrode pair by using an adjacent pattern in both excitation and acquisition phases. The measurements were taken when no load was applied over the artificial skin.
  • Figure 8. Electric potential measurements acquired when a probe is acting in the region facing Electrode 2 (E2). The values are grouped according to which electrode is used as ground following an adjacent pattern (highlighted in the top part of the figure). The shaded portion of the graph corresponds to the configuration when E2 is one of the driving electrodes. The major noticeable differences are the ones wherein E2 is involved in the measurements.

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CITATION STYLE

APA

Visentin, F., Fiorini, P., & Suzuki, K. (2016). A deformable smart skin for continuous sensing based on electrical impedance tomography. Sensors (Switzerland), 16(11). https://doi.org/10.3390/s16111928

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