Soft Sensory-Motor System Based on Ionic Solution for Robotic Applications
<p>Diagram of the robot principle: the system designed can perceive the environment as a sensor and actuate in the environment as an actuator using an integrated soft body. The internal mechanical feedback from the body can be combined with external physical stimulation representing a redundancy of the sensory channels, improving the speed and simplifying the perception. The information processed by the perception module can go to the brain and activate the actuator part of the system, but it also can be processed in the sensory-motor coordination module without necessarily passing through the brain, speeding up the dynamic control of the robot.</p> "> Figure 2
<p>Diagram of the principle of functionality regarding soft sensory-motor system based on ionic solution. Three states of the SSMS-IS can be observed, i.e., (<b>A</b>) relaxed, when there is no air inlet in the system <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mi>n</mi> <mi>t</mi> </mrow> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math> and the external pressure is null <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>e</mi> <mi>x</mi> <mi>t</mi> </mrow> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math>; (<b>B</b>) compressed, when there is no air inlet in the system <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mi>n</mi> <mi>t</mi> </mrow> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math> and there is an external pressure <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>e</mi> <mi>x</mi> <mi>t</mi> </mrow> </msub> <mo>≠</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math> in the system; and (<b>C</b>) inflated, when there is air inlet <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mi>n</mi> <mi>t</mi> </mrow> </msub> <mo>≠</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math> in the system and the external pressure is null <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>e</mi> <mi>x</mi> <mi>t</mi> </mrow> </msub> <mo>=</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> </semantics></math>. For each state, differences can be observed in the electric resistance measurement <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>R</mi> <mi>x</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math> for a determined voltage (V) based on the variation in the ionic solution area <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>A</mi> <mi>x</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math> and distance <math display="inline"><semantics> <mrow> <mrow> <mo>(</mo> <mi>L</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> between the positive and negative cupper cable. The variation in the ionic solution area <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>A</mi> <mi>x</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math> is correlated with the variation in external pressure <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>e</mi> <mi>x</mi> <mi>t</mi> </mrow> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math> and internal pressure <math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <mo>Δ</mo> <msub> <mi>P</mi> <mrow> <mi>i</mi> <mi>n</mi> <mi>t</mi> </mrow> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math>.</p> "> Figure 3
<p>(<b>a</b>) Internal components of soft sensory-motor system based on ionic solution: ionic solution, soft diaphragm, copper wire, air tube, and electrode. The internal view is based on the rectangular geometry but can be applied to any design of SSMS-IS. (<b>b</b>) Comparison of the size of the SSMS-IS rectangular design with a 1 cent coin.</p> "> Figure 4
<p>Bioinspired robot design based on the morphology of the isopod Armadilium Vulgare: it was formed by modules that represent the bioinspired segments and each segment of the soft robot should have a sensory motor based on the SSMS-IS to actuate in the environment when expanded and to sense when compressed. Also, it can execute the conglobation movement for self-protection using soft actuators in each segment.</p> "> Figure 5
<p>Details of the robot’s segment with two SSMS-IS elements integrated into an internal interface. Each segment is composed of two pumps to inflate the SSMS-IS, two servo motors to make the pumps made by syringes function, and a soft actuator responsible for generating the conglobation movement bioinspired from Armadillium Vulgare. The SSMS-IS elements are actuated by pumps embedded in the robot.</p> "> Figure 6
<p>Robot morphology adaptation. From <a href="#sensors-24-02900-t001" class="html-table">Table 1</a>, (<b>a</b>) State 1, when both SSMS-ISs in the soft robot shield are disabled; (<b>b</b>) State 2, when one SSMS-IS is enabled; (<b>c</b>) State 3, when one SSMS-IS is enabled; and (<b>d</b>) State 4, when both SSMS-ISs are enabled.</p> "> Figure 7
<p>Three SSMS-IS designs were investigated: toroidal, semi-toroidal, and rectangular geometries. They were fabricated using silicon rubber RPRO 20 (Reschimica<sup>®</sup>).</p> "> Figure 8
<p>Fabrication procedure for different SSMS-IS designs: (<b>a</b>) SSMS-IS manufacturing process for toroid geometry; (<b>b</b>) SSMS-IS manufacturing process for semi-toroid geometry; and (<b>c</b>) SSMS-IS manufacturing process for rectangular geometry.</p> "> Figure 9
<p>Design of the electrolyte volume for each mold: (<b>a</b>) toroidal electrolyte volume = 1272.35 mm<sup>3</sup>; (<b>b</b>) semi-toroidal electrolyte volume = 1276.74 mm<sup>3</sup>; and (<b>c</b>) rectangular electrolyte volume = 1270.67 mm<sup>3</sup>.</p> "> Figure 10
<p>Elastomer parts for each SSMS-IS design: (<b>a</b>) toroidal; (<b>b</b>) semi-toroidal; and (<b>c</b>) rectangular. The diaphragm’s thickness for each SSMS-IS was 1 mm to guarantee less resistance during mechanical expansion.</p> "> Figure 11
<p>(<b>a</b>) Circuit diagram regarding the acquisition data for the resistance variation in the SSMS-IS. (<b>b</b>) Setup of the tests composed of controllers, pump, resistance divider circuit, SSMS-IS, and battery.</p> "> Figure 12
<p>(<b>a</b>) Test setup for evaluating external pressure over different designs of SSMS-IS; (<b>b</b>) test setup for toroidal SSMS-IS; (<b>c</b>) test setup for semi-toroidal SSMS-IS; and (<b>d</b>) test setup for rectangular SSMS-IS.</p> "> Figure 13
<p>(<b>a</b>) Setup to test the response of both sensors simultaneously on the interface for external force input in the vertical direction as shown by the yellow arrow; (<b>b</b>) robot without external input force; and (<b>c</b>) vertical load pressing the shield in the vertical direction as shown by the yellow arrow in the picture, emulating an external input force over the robot.</p> "> Figure 14
<p>Robot module system configuration: one microcontroller; two SSMS-ISs; two servomotors; two air pumps connected with SSMS-IS; and a lithium-ion battery. The measurements performed by the microcontroller can be communicated with the PC.</p> "> Figure 15
<p>Resistance changes vs. pressure for toroidal geometry of the sensor: (<b>a</b>) sensitivity within the sensing range of external pressure of 0–79.08 mmHg and (<b>b</b>) drift in toroidal sensor for approximately 15 min.</p> "> Figure 16
<p>Resistance changes vs. pressure for semi-toroidal geometry of the sensor: (<b>a</b>) sensitivity within the sensing range of external pressure of 0–79.08 mmHg and (<b>b</b>) drift in semi-toroidal sensor for approximately 15 min.</p> "> Figure 17
<p>Resistance changes vs. pressure for the rectangular geometry of the sensor: (<b>a</b>) sensitivity within the sensing range of external pressure of 0–79.08 mmHg and (<b>b</b>) drift in rectangular sensor for approximately 15 min.</p> "> Figure 18
<p>Resistance changes vs. internal pressure for toroidal geometry of the sensor: (<b>a</b>) sensitivity within the sensing range of external pressure of 0–477.81 mmHg and (<b>b</b>) results of cyclic loading of the sensor for 3000 cycles of internal pressure at 224.61 mmHg.</p> "> Figure 19
<p>Resistance changes vs. internal pressure for semi-toroidal geometry of the sensor: (<b>a</b>) sensitivity within the sensing range of external pressure of 0–477.81 mmHg and (<b>b</b>) results of cyclic loading of the sensor for 3000 cycles of internal pressure at 224.61 mmHg.</p> "> Figure 20
<p>Resistance changes vs. internal pressure for rectangular geometry of the sensor: (<b>a</b>) sensitivity within the sensing range of external pressure of 0–477.81 mmHg and (<b>b</b>) results of cyclic loading of the sensor for 3000 cycles of internal pressure at 224.61 mmHg.</p> "> Figure 21
<p>Robot time response for two states over external pressure inputs. Initially, the robot was in a relaxed state, and after subjecting the robot to 3 levels of loads (1.8 N, 2.4 N, and 2.9 N), the levels of force due to the variation in the electric resistance of the SSMS-IS was detected. In the second moment of the test, the robot was in the actuated state, and after subjecting the robot to 3 levels of loads (1.8 N, 2.4 N, and 2.9 N), the levels of force due to the variation in the electric resistance of the SSMS-IS was detected, indicating that, even in the actuated state, the robot can sense differences in external forces using a unique device to actuate and to sense simultaneously.</p> "> Figure 22
<p>Boxplot for the soft robot response for each load applied in each performed state. For the relaxed state, each SSMS-IS in the robot could detect the external loads by the variation in the electric resistance. Also, when the value of the load was increased, the variation in the resistance proportionally increased. For the actuated state, each SSMS-IS in the robot could also detect the external loads by the variation in the electric resistance. When the value of the load was increased, the variation in the resistance also proportionally increased, indicating that in both states, relaxed and actuated, the robot can measure different external load values, and the variation in the internal resistance is proportional to the variation in the load.</p> "> Figure 23
<p>Mechanical deformation for each system design (toroidal, semi-toroidal, and rectangular) for each state of the system: relaxed, compressed, and inflated. The differences in the mechanical elasticity constraints for each SSMS-IS design can be noticed during the states of expansion and compression.</p> ">
Abstract
:1. Introduction
2. Materials and Methods
2.1. SSMS-IS Design
2.2. Robot Design
2.3. Fabrication
3. Results
3.1. Performance for External Input Pressure of Different Designs of SSMS-IS
3.2. Performance for Internal Input Pressure of Different Designs of SSMS-IS
3.3. Performance of SSMS-IS in the Robot Application
4. Discussion
5. Conclusions
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Conflicts of Interest
Nomenclature
Symbol | Description | Unit |
External pressure | N·m−2 | |
Internal pressure | N·m−2 | |
L | Length between electrodes | mm |
A | Area of the electrolyte between electrodes | mm2 |
R | Electric resistance | Ω |
Electrical resistivity | - | |
V | Voltage between electrodes | kg·m2·s−3·A−1 |
External force | N | |
Abbreviation | Description | |
SSMS-IS | Soft sensory-motor system based on ionic solution | - |
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Robot Body State | SSMS-IS#1 | SSMS-IS#2 |
---|---|---|
State 1 | Disabled | Disabled |
State 2 | Disabled | Enabled |
State 3 | Enabled | Disabled |
State 4 | Enabled | Enabled |
Test Performance | Toroidal | Semi-Toroidal | Rectangular |
---|---|---|---|
Linear external sensitivity % variation | ~20% | ~35% | ~45% |
Linear external sensitivity range | 0–41.87 mmHg | 0–27.91 mmHg | 0–46.52 mmHg |
Linear internal sensitivity % variation | ~45% | ~55% | ~85% |
Linear internal sensitivity range | 0–477.81 mmHg | 0–97.06 mmHg | 0–477.81 mmHg |
Drift | ~35% | ~35% | ~10% |
Durability | 3000 cycles | 3000 cycles | 3000 cycles |
Variance (σ2) | Median | |||||
---|---|---|---|---|---|---|
Load | Force | Relaxed | Actuated | Relaxed | Actuated | |
SSMS-IS#1 | 1 | 1.8 N | 0.0051 | 5.7350 × 10−4 | 0.29435 | 0.48666 |
2 | 2.4 N | 0.0005 | 0.0008 | 0.12351 | 0.46279 | |
3 | 2.9 N | 0.0010 | 0.0010 | 0.07426 | 0.43887 | |
SSMS-IS#2 | 1 | 1.8 N | 0.0169 | 6.9240 × 10−4 | 0.46279 | 0.53425 |
2 | 2.4 N | 0.0092 | 0.0014 | 0.46279 | 0.53425 | |
3 | 2.9 N | 0.0086 | 0.0025 | 0.46279 | 0.51048 |
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Santos, S.R.d.; Rohmer, E. Soft Sensory-Motor System Based on Ionic Solution for Robotic Applications. Sensors 2024, 24, 2900. https://doi.org/10.3390/s24092900
Santos SRd, Rohmer E. Soft Sensory-Motor System Based on Ionic Solution for Robotic Applications. Sensors. 2024; 24(9):2900. https://doi.org/10.3390/s24092900
Chicago/Turabian StyleSantos, Sender Rocha dos, and Eric Rohmer. 2024. "Soft Sensory-Motor System Based on Ionic Solution for Robotic Applications" Sensors 24, no. 9: 2900. https://doi.org/10.3390/s24092900
APA StyleSantos, S. R. d., & Rohmer, E. (2024). Soft Sensory-Motor System Based on Ionic Solution for Robotic Applications. Sensors, 24(9), 2900. https://doi.org/10.3390/s24092900