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  • Research Article
  • Open Access

Evaluation of effects caused by individual differences in human shape that affect the safe utilization of wearable robots

Contributed equally
ROBOMECH Journal20185:20

  • Received: 20 April 2018
  • Accepted: 24 August 2018
  • Published:


When using a wearable robot, the interaction force applied to the area of contact may cause skin injuries over time. Therefore, validating the contact safety of wearable robots is important for their practical application. Because previous studies indicated that the repetitive share stress of the wearable robots increased the risk of blister generation, analysis of stress distribution, which is affected by the contact state, was viewed as very important. However, the effect of variability of the shape of the human body on the shear stress applied to the contact area is rarely analyzed, even though uneven contact between human tissue and the robotic cuff can cause stress concentration. In this study, a system for safety verification and validation of the robotic cuff was developed, and the interaction force exerted on the contact area of a variably shaped human tissue dummy when rubbed by a robotic cuff was measured. As a result, the maximum interaction force occurred when the robotic cuff moved over the convex part of the surface. Furthermore, the magnitude of the interaction force corresponded to the gradient. Thus, the shear stress increased by approximately 10% as the height of the iliac spine, which originally mimicked the anterior superior iliac spine, changed by 1 mm. This variability suggests that the stress concentration caused by the unevenness of human tissue plays an important role in the risk of blister.


  • Wearable robot
  • Contact safety
  • Indevidual difference
  • Skin shape
  • Stress concentration


Recently, the use of wearable robots has been on the increase in society. For example, the usage of such robots has expanded from rehabilitation in hospitals [1] to daily living assistance in society [2, 3]. Accordingly, the safe usage of such robots is now being discussed with several manufacturers proposing safety test methods for their wearable robots [4, 5]. Further, the international standard IS0-13482:2014 [6], which was enacted for the safe usage of personal care robots, also determines the safety requirements and the safety test methods.

Because a wearable robot is directly attached to the human body and exerts assistive torque and force through the contact area, regardless of the part to which it is attached [710], the contact safety of the wearable robot has to be considered carefully. In particular, blister generation around the contact area is a major concern from the viewpoint of contact safety because skin blisters occur under repetitive rubbing [11, 12]. To assess the risk of blister generation, it is important to estimate the interaction force at the contact area because the magnitude of the shear force critically affects the endurance time of blister generation [13, 14]. Thus, in previous studies, the interaction force exerted at the contact area of the upper-limb [15] and the lower-limb [16] during human–robot interaction was measured.

To examine the contact safety, meaning by estimating the risk of blister generation at the contact surface between human skin surface and a cuff of a physical assistant robot, we previously proposed the safety test process shown in Fig. 1. In this process, first, the relative motion between the robotic cuff and human skin and the interaction force exerted at the contact area of the robotic cuff is measured [17, 18]. Then, the relative motion and interaction force are reproduced by a 6-degree of freedom manipulator on dummy tissue [19]. The risk of blister generation when using a wearable robot is then assessed by turning the shear force applied to the dummy tissue into a threshold curve of the safety [14], which is drawn as the relationship between the shear force and endurance time.
Fig. 1
Fig. 1

Wounds risk evaluation process [19]

However, the interaction force, which strongly affects blister generation, does not become an even distribution because of the unevenness of the shape of the contact area. In particular, the surface shape and physical parameters such as stiffness of the human body vary among individuals [20, 21] because of the variance of musculoskeletal frame and amount of fat. However, the effect of such contact area unevenness was not considered sufficiently. Because such uneven contact causes stress concentration owing to the distribution of the form resistance and friction force [22], the risk of blister generation under uneven contact increases compared to even contact. Thus, estimation of the effect of variance of the surface shape of the human body on the shear force applied to the contact area is necessary for accurate assessment of the risk of blister generation due to human–robot interaction.

To measure the shear force exerted during the surface rubbing motion on various surface shapes, a device whose surface shape could be deformed to a certain extent was developed. Further, the surface deformability of the mechanism used for this device was validated by our group [23]. However, changes in the reaction force exerted on the contact surface caused by differences in contact surface shape were not measured and evaluated. Consequently, by rubbing the surface generated by the device using a manipulator, as shown in Fig. 2, the effect of surface unevenness, which differs among individuals, on the shear force was determined in this study. First, the design of the surface deformation device was described. Then, after evaluation of the physical parameters of the device, the surface shapes, which consist of the baseline shape obtained from an actual human and shapes that slightly differ from the baseline shape, were determined. Then, the shear force exerted on the robotic cuff was measured via a rubbing test using this device and the manipulator. This is the newly developed system which was designed to experimentally test and evaluate the effect of the shape of robotic cuff and skin surface on the contact force for the safety verification and validation of the robotic cuff. Thus, this study constitutes the first step in the evaluation of the effect of individual differences in people’s shapes on the safety design of wearable robots.
Fig. 2
Fig. 2

Safety test with variable shape dummy

Three-dimensional (3D) skin-shape reproduction system

Skin-shape reproduction device

A 3D skin-shape reproduction device, shown in Fig. 3, was previously developed [23]. It consists of 18 DC motors (RE30, Maxon Motor, Switzerland), 18 cables aligned in a grid, and a silicon rubber sheet. Shape reproduction proceeds as follows: First, the deformable rubber sheet is inflated by air injected from the bottom of the deformable area, with inflation of the rubber sheet restricted by adding tension to each cable by winding them up using the motors. A variety of surface shapes can be reproduced by adjusting the length of each cable. In our previous study, it was confirmed that this device can reproduce a variety of deformation patterns [23].
Fig. 3
Fig. 3

Upper part of the variable shape human tissue dummy

Fig. 4
Fig. 4

Skin-shape reproduction process

Shape reproduction process

Skin-shape reproduction is achieved via the process shown in Fig. 4. First, an objective shape, which corresponds to the deformation part of the human dummy, is obtained. Next, the length of each cable is calculated as the length of the pathways, which connect the ends of each cable, on the surface of the objective shape. The calculated lengths become the target value of each cable. Then, after initial pressure and pretension are applied to the device, the tension of the cables is optimized to achieve the target length.

Validity of generated surface shape and elasticity as a human dummy

Reproduction of human pelvis

The validity of the surface shape of the device was tested by comparing the surface shape of the device and the target shape obtained from a human. In this study, the part around the anterior superior iliac spine (ASIS), in which the bone is pointed, as shown in Fig. 5, was set to the target shape. Fig. 6 shows the reproduction area and the reference coordinates. The reproduction area is defined as the area surrounded by the red line considering the wound risk and the configuration or the general wearable robot. An example of the shape reproduction is shown in Fig. 7. The figure shows dummy skin made from urethane gel, which mimics the characteristics of human tissue, fixed onto a rubber sheet. Thus, the bumps of the surface of the membrane formed by cables does not affect the surface shape of the device. The values for the mechanical parameters of the device were set as displayed in Table 1. The size of the surface and the distances between cables were designed to set in a convex of the human body.
Fig. 5
Fig. 5

Example of human shape (pelvis) [24]

Fig. 6
Fig. 6

Human shape reproduction area and coordinates

Fig. 7
Fig. 7

Shape reproduced with dummy skin

Confirmation of shape reproducibility

For the validation check of the shape reproduced using the device, the displacement and curvature of the device and target shape were compared in Figs. 8 and 9. The shape of the device was measured using a 3D scanner. In the figures, the comparison was conducted at y = 5 mm and x = 5 mm, where the curvature was largest. The graphs show that the device reproduced the feature of the target shape-in this case, the local bulge. Thus, in this study, the reproduced shape was determined as the baseline shape. Then, shapes slightly deformed from the baseline shape were used to evaluate the effect of the difference of unevenness.
Table 1

Conditions of the shape reproduction parameter values

Young’s modulus (rubber sheet)

5.4 MPa

Young’s modulus (cable)

1.5 GPa

Dummy skin hardness

0 (Asker C)

Poisson’s ratio


Rubber sheet thickness

2.0 mm

Dummy skin thickness

3.0 mm

Deformation area (x-direction)

90 mm

Deformation area (y-direction)

90 mm

Number of cables (x-direction)


Number of cables (y-direction)


Interval of cables

10 mm

Fig. 8
Fig. 8

Displacement comparison results. a Displacement comparison (y = 5), b displacement comparison (x = 5)

Fig. 9
Fig. 9

Curvature comparison results. a Curvature comparison (y = 5), b curvature comparison (x = 5)

Elasticity of the deformed surface

Because the device comprised the musculoskeletal system and surface tissue of a human, the deformed surface has to reproduce the mechanical properties of human bone, muscle, and fat. Thus, the elasticity in the normal direction and the shear modulus of the device were measured.

The elasticity in the normal direction was measured using the manipulator shown in Fig. 10. In this method, the contactor attached to the robotic cuff was pushed into the reproduced body. Then, the reaction force applied to the contactor was measured using a force sensor. In this experiment, the area of the contactor was 64 mm2 and the indentation force was measured up to a depth of 5 mm. As a result, the normal stress per indentation depth was calculated as 64.0 kPa/mm. Although the elasticity in the normal direction around ASIS was not reported previously, the rigidity of the relaxed muscle with a large deformation was estimated at approximately 5.5 kPa/mm using the strain–stress diagram [25]. This suggested that the device was much stiffer than the soft tissue of a human and was closer to that of the part with the thin tissue supported by bone.
Fig. 10
Fig. 10

Measurment of the elasticity in normal direction of the reproduced shape

The transverse elasticity was also measured, as shown in Fig. 11. In this experiment, the robotic cuff was moved along the shear direction using the manipulator, which was preloaded to avoid slippage. The reaction force in the shear direction was measured with a force sensor. The area of the contactor was approximately 1750 mm2 and the deformation in the shear direction was up to 5 mm. The shear modulus was calculated by dividing the shear stress by the shear strain. The shear strain was calculated by dividing the motion distance of the cuff by the thickness of the deformable part of the device. The shear modulus of the device, 7.48 kPa, was relatively close to that of human muscle, 5.40 kPa [26].
Fig. 11
Fig. 11

Transverse modulus evaluation of the reproduced shape

Effect of surface shape variability on interaction force

Evaluation process using the surface deformation device

The evaluation of the effect of surface shape variability on the interaction force exerted during rubbing motions was conducted using the surface deformation device and the manipulator. As mentioned above, the baseline shape was designed from the 3D shape data around ASIS, acquired from a human. Then, surface shapes with slightly different gradients from the baseline shape, were designed from the baseline shape. The interaction force when the robotic cuff rubbed these surfaces using the manipulator was measured and compared to each other.

Design of the surface shape variance

It was hypothesized that the shear force on human skin increases when the cuff is over the convex because of larger form resistance and friction. In this study, three shapes, plotted in Fig. 12, were used to evaluate the effect of shape variance. These shapes were designed by modifying the ASIS (\(x=5\) mm and \(y=-10\) mm) part of the baseline shape to increase or decrease its height by ± 1 mm, as shown in Fig. 12.
Fig. 12
Fig. 12

Target shapes for the experiment

Experimental protocol

Because the interaction force exerted when rubbing on the uneven surface is affected by the normal force of the robotic cuff, the normal force of the manipulator was controlled to 20 N, which was the value exerted at the cuff when using a wearable robot in the previous study [17]. The surface of the robotic cuff was covered by a 40 mm × 40 mm × 15 mm sponge sheet, determined by considering the softness of the cuff used in commercial wearable robots. In this study, initially, the center of the robotic cuff was set at \(x=5\) mm and the front edge was set at \(y=-15\) mm. Then, the robotic cuff rubbed the surface along the y-direction, keeping the force in the z-direction constant, as shown in Fig. 13. During the rubbing motion, the position of the robotic cuff and interaction force exerted on it was measured. This process was repeated 10 times for each condition.
Fig. 13
Fig. 13

The rubbing motion using the manipulator

Result of experiment

The recorded shear force on the different surface shapes is shown in Fig. 14. This result suggests that the interaction force in the shear direction increases with gradient. As hypothesized, this is probably caused by the increase of the form resistance as the gradient increases. Consequently, the interaction forces increase when the robotic cuff moved over the convex part of the surface.
Fig. 14
Fig. 14

Interaction force pattern in the shear direction

The maximum shear forces and stresses observed in the experiments are shown in Table 2. The maximum shear stress changed approximately 10–20% even when the height changed 1 mm, as shown in Fig. 12.
Table 2

Maximum shear forces and stresses in the experiments


Maximum shear force (N)

Maximum shear stress (kPa)

Gradient (large)



Actual human shape



Gradient (small)




Relationship between surface shape and interaction force

The exerted shear force shown in Fig. 14 and Table 2 suggests that there is a relationship between the pattern of unevenness and the interaction force. First, the interaction forces among the different surface shapes did not differ until around \(y=-8\) mm, although the shape under the robotic cuff differed, as shown in Fig. 12. This was probably because the effect of the variance of the surface shape was absorbed by the deformation of the sponge of the robotic cuff. The shear modulus may also have contributed to this easing. Then, the interaction force started to show the difference among gradient values, as stated above.

When the front edge of the robotic cuff reached approximately \(y=5\) mm, the increase rate of the interaction force started to decline. In this phase, the partial contact of the robotic cuff, a part of which separated from the surface of the device, was observed. Because the normal force of the robotic cuff is controlled to a constant value, the robotic cuff moved upward when getting over the convex. Finally, the interaction force of the baseline shape and large gradient shape started to decrease after \(y=10\) mm. Although the shear force did not increase, the partial contact probably causes stress concentration, which could not be observed even using this measurement system.

Because the target of this study was to identify the increase of the wounds risk caused by the variance of surface shape when using the wearable robot, some features of the contact state between the robot and human, such as the shape and stiffness of the robotic cuff, viscoelasticity of the wearer’s tissue, and the loading pattern of the robotic cuff on the surface, were simplified. Thus, more precise experimentation and analysis is required for practical validation testing of the wearable robot. However, the necessity of considering the surface shape and its variance based on the human were expounded in this study.

Effect of surface shape variance from the viewpoint of contact safety

When evaluating the risk that appears after several exposures to the hazard, the method using the threshold curve is commonly used. By using the threshold curve, the endurance time, which is the threshold time of acceptable risk, can be estimated under specific loading conditions. Thus, using the curve that evaluates the wounds risk caused by continuous rubbing [27], the endurance time under various surface shapes was estimated and compared.

The shear force exerted in rubbing motions increases with the normal force. According to previous study [17], the normal force exerted when using a wearable robot seldom exceeded 50 N. Thus, in this section, considering the severe condition when using the wearable robot, a rubbing motion under 50 N of normal force was assumed. In addition, because of the limitation of the specification of the device, it was difficult to keep the surface shape under such a large compression force. Thus, the shear force under the normal force of 50 N was estimated by increasing the pattern of the interaction force observed in the experiment mentioned above proportionally.

The estimated maximum shear stress and the endurance time under such a condition area displayed in Fig. 15 and Table 3. The risk curve displayed here was obtained from the rubbing test using porcine skin and human skin [27]. These results suggest that the endurance time significantly changes even when the surface shape changes only slightly. In addition, the risk curve used in this study did not include the effect of local stress concentration. As mentioned above, it suggests that the stress concentration occurs over the large convex. Moreover, the existence of stress concentration was verified by visualizing the pressure distribution on the surface of the device. A tactile sensor sheet (I-SCAN, Nitta Corporation, Japan), which could measure the normal force exerted on square cells lined on the surface, was used. By putting this flexible sheet on the uneven surface, the concentration of normal force was roughly observed via a rubbing test. The observed force concentration made the endurance time short, as shown in the risk curve.

For the safety design of the cuff of the wearable robot, the increase and concentration of shear force around the convex will cause a problem. Thus, it seems better to use maximum pressure instead of mean value when evaluating the contact force under the robotic cuff. Furthermore, the shape of robotic cuff should probably be designed to decrease the pressure exerted around the body convex. One option is to support the interaction force with a flat area of the body surface. In addition, the contact between flat cuff and body convex such as the situation of this study was not suitable from the view of contact safety. Thus, the area of robotic cuff, which contacts the body convex, should have sufficient indentation to avoid force concentration. However, it should be noted that the index to evaluate the body convex, which could be used to estimate the range of individuality, was not determined yet.
Fig. 15
Fig. 15

Threshold curve for blister generation [27]

Table 3

Change of safety condition caused by the change of shapes under the 50 N indentation force


Maximum shear stress (kPa)

Endurance time (s)

Gradient (large)



Actual human shape



Gradient (small)


\(\text{1.32 } \times \text{10 }^{\text{3 }}\)


The effect of surface shape variance of the human body on the interaction force at the contact area when using a wearable robot was estimated in this study. For this purpose, a device that can mimic the unevenness and variance of the human shape, was developed. Then, the performance of the device was confirmed by comparing the characteristics of the device to that of an actual human. Because of the greater unevenness and individuality of the surface shape, the experiment, which mimicked the contact between the human body and the cuff of the wearable robot, targeted the ASIS of the human. The result of the rubbing test using the device and the robotic cuff attached to the manipulator suggests that the interaction force applied to the surface changed approximately 10% as the height at the iliac spine changed ±1 mm. Furthermore, this difference probably affects the endurance time, which is an index of the contact safety, significantly under the severe condition. Thus, this study suggests that considering the individual difference in the characteristics of human tissue and surface is important for the safety design of a wearable robot.



Authors’ contributions

YS and YA designed and developed the device and control algorithm. Experimental protocol and analysis were planed and proceeded by them. YY proposed the idea of device and drew grand design of this study. He contributed to improve the validity of experimental condition and analysis. SO contributed to design experiment and analysis method for validating the device. All authors read and approved the final manuscript.


This study is based on the results of research and development of Japan Agency for Medical Research and Development (Project to Promote the Development and Introduction of Robotic Devices for Nursing Care).

Competing interests

The authors declare that they have no competing interests.

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Authors’ Affiliations

Department of Mechanical Science and Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan


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