a motorized sliding sled apparatus for measuring the...

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Pressure and shear generally receive the majority of attention in the nursing literature when it comes to treating and preventing pressure ulcers. Pressure is a vertical force exerted by gravity pulling on the body. It is generally expressed at a bony prominence where it compresses soft tissue, causing capillary closure leading to ischemia and subsequent cell death. Shear is a horizontal force that acts in concert with pressure to distort tissues and cause narrowing of blood vessels. When sufficient shear is applied, the internal diameter of the capillaries becomes inadequate for blood to flow through them. 1 Shear is thought to be up to 10X more destructive than pressure alone because of its ability to cut off large areas of vasculature. 1,2 However, shear requires a third element, friction, to exert its destructive effect on skin and subcutaneous tissues. 1 Friction causes the body to remain adherent to the support surface while the underlying tissues move. 3 Without friction there would be no shear, as the body would simply glide along the support surface. Friction is also involved in skin chafing, particularly when moisture is involved. Chafing occurs when the skin repeatedly rubs against another object causing an abrasion injury. This type of injury is usually limited to the epidermis, and is most frequently seen on elbows and heels of patients that are restless. Chafing and abrasion injuries are often reported as a “sheet burn.” 4 While the importance of friction in the causation of pressure ulcers and chafing injuries is recognized in the nursing literature, relatively little attention has been given to understanding how topically applied products may influence frictional forces on the skin. Therefore an apparatus was constructed for in vivo studies of skin friction (drag) based on DaVinci’s classic sliding sled experiments. The apparatus has proven to be useful in studying the influence of various topically applied products on skin frictional properties. A computer-controlled sliding sled apparatus based on DaVinci’s classic sliding sled experiments has been constructed that provides reproducible measurements of skin frictional properties. The sliding sled apparatus can be used to compare the effect of application of topically applied products on the skin. Two barrier film products produced very different skin friction measurements. Barrier film A dried quickly to a relatively smooth, lower friction surface compared to barrier film B. Barrier film B remained tacky two minutes after application, resulting in a jerky motion of the sled as it traversed the skin, and a 257% higher coefficient of friction compared to barrier film A. Acknowledgements: Poster design by Lutz Consulting LLC This study was supported by 3M Health Care To describe a new motorized sliding sled apparatus based on DaVinci’s classic sliding sled experiments that was constructed for in vivo studies of skin friction properties. This presentation will also summarize data generated during development of the device comparing the effect of two barrier films on skin friction properties. Overview To learn more about the effects of skin care products on frictional properties of the skin, we constructed an apparatus for in vivo studies based on DaVinci’s classic sliding sled experiments. Test Apparatus The device consisted of two sandwiched support plates that maintained a parallel path for the sliding sled as it moved across the skin (Figure 1). The upper plate had a linear guide with two moveable blocks, one of which was motorized and under PC control using PWM signals. A rack and pinion system converted rotary motion of the servo motor into linear motion. For this series of experiments, the traverse path was 18.8 mm at 5.25 mm/sec. The other block, which was exposed through a slot in the lower base plate, presented a 32 x 48 mm surface that dragged against the skin (Figure 2). The 48 mm length was comprised of 3 sections, each 16 mm in length, with the center section running parallel to the skin and the leading and trailing edges sloped at 25 degrees. The precise angle to which the sled was pushed against the skin could be varied by inserting or removing shims. The sliding sled was covered with a 55:45 cotton-polyester sheet representative of hospital bedding. This test material was replaced prior to each run. A miniature load cell placed between the interfacing surfaces of the sliding blocks allowed for real time measurement of the compression and tension forces resulting from pushing and pulling the sled. Data acquisition software exported both raw voltages from the load cell and steps made by the servo motor to an EXCEL spreadsheet using a PLX-DAQ macro. Converting imported values to Load (grams) and Distance (mm) was achieved using appropriate calibration factors. Each experiment was run at least in triplicate. Validation studies using rigid substrates in vitro showed that the resulting curves were in keeping with Amonton’s laws and could be used to reliably evaluate both the static and dynamic coefficient of friction. We found from our studies of human skin in vivo that the mechanical properties of the skin dramatically influence the results, and Amonton’s laws no longer provided an adequate description of the frictional forces. Nevertheless, the apparatus has proven to be an effective tool for studying the influence of topically applied products on the frictional properties of the skin. Hydration & Skin Friction It is well documented that as skin becomes increasingly hydrated, there is a corresponding increase in skin frictional properties. 5 Thus, skin that is over-hydrated from sweat or incontinence is more susceptible to the destructive forces of shear and chafing. Figure 3 shows the results of a validation experiment to demonstrate sensitivity of the current device to measuring changes in skin frictional properties resulting from hydration. Skin friction was measured at four different hydration levels: 1) dry, 2) moist (hydrated with a few drops of water), 3) wet (5 minute exposure to a wet paper towel), and 4) soaked (10 minutes of complete immersion in water). The data clearly show sensitivity of the device to measuring changes in skin hydration level. Tacky vs. Non-Tacky Films Barrier films are often used clinically to help prevent maceration of the skin and to protect areas prone to abrasion injury. However, little is known about the effects of barrier films on skin friction properties. Therefore, an experiment was conducted to compare frictional properties of two barrier films two minutes after application to the skin. Barrier film A was a product known for its fast- drying properties, and barrier film B was a product known to be much slower drying. Figure 4 shows triplicate frictional drag force measurements over the two treated sites on a single subject two minutes after application of the barrier films. Barrier film A is dry to the touch and provides a relatively smooth surface over which the sled can move. However, barrier film B is still tacky to the touch two minutes after application. This is evident by an approximately four-fold higher coefficient of friction and a jerky motion of the sled as it attempts to move across the skin surface. In a second experiment, skin friction measurements were taken from the volar forearms of nine subjects before and two minutes after application of the two barrier films. The results of this experiment (Figure 5) show similar data to the previous experiment. The mean (SD) coefficient of friction for barrier film B two minutes after application was 1062.1 (272) grams, which was 257% higher than barrier film A, 412.4 (98.5) grams (p<0.0001). An interesting observation was that barrier film A showed a small but significant (p<0.0001) increase in skin friction compared to untreated skin, indicating that the clinical effectiveness observed for this product may be related more to protection of the skin from hydration and abrasion forces rather than an actual reduction in the coefficient of friction. However, it is clear that compared to barrier film B there is a significant reduction in skin friction. Methods Objective Results Conclusions A Motorized Sliding Sled Apparatus for Measuring the Coefficient of Friction of Human Skin in vivo Gary Grove, cyberDERM Clinical Studies, Broomall, PA Aram Grigoryan, cyberDERM Special Projects Group, Media, PA Tim Houser, cyberDERM Special Projects Group, Media, PA Jonn Damia, cyberDERM Special Projects Group, Media, PA Nancy Atwood, Clinical Research Specialist, 3M Health Care, St. Paul, MN Background Figure 1: Schematic drawing of the sliding sled device used to measure friction forces on the skin. The device consists of a supportive struc- ture that maintains a parallel path for a sliding sled connected to a motorized unit via a load cell. Skin Surface Motorized Unit Support Plate & Linear Track Load Cell Sliding Sled Unit Electronics & PC Interface Test material Figure 2: Photograph of the sliding sled device as it measures compression and tension forces resulting from friction as the sled moves across the surface of the skin. The device can measure the effect of various skin treatments on skin friction. References Fontaine R, Risley S, Castellino R. A quantitative analysis of pressure and shear in the effectiveness of support surfaces. J 1. Wound Ostomy Continence Nurs 1998;25(5):233-9. Zhang M, Roberts VC. The effect of shear forces externally applied to skin surface on underlying tissues. J Biomed Eng 2. 1993;15(6):451-6. Stewart TP. Support Systems. In: Parish LC, Witkowski JA, Crissey JT, editors. The decubitus ulcer in clinical practice. London: 3. Springer; 1997. p. 145-68. Bryant R, Nix D. Mechanical forces: Pressure, shear, and friction. In: Acute & Chronic Wounds: Current Management Concepts. 4. Third ed: Mosby; 2007. p. 205-34. Cottenden AM, Wong WK, Cottenden DJ, Farbrot A. Development and validation of a new method for measuring friction 5. between skin and nonwoven materials. Proc Inst Mech Eng [H] 2008;222(5):791-803. Test Products Barrier Film A: Cavilon™ No Sting Barrier Film (3M) Barrier Film B: Sureprep® No-Sting Skin Barrier (Medline Industries) * Figure 4: Triplicate drag force measurements of the sled moving across the volar forearm on skin that has been treated with two different barrier films. Barrier film A dries quickly to a smooth surface with a relatively low frictional drag force. Barrier film B is slow to dry and leaves a tacky film even two minutes after application. This is evident by a four-fold higher drag force, and a jerky motion of the sled as it traverses the volar forearm. Barrier Film A Barrier Film B Triplicate Skin Friction Measurements 2 Minutes after Application of Barrier Films Friction Drag Force (grams) 1200 1000 800 400 600 200 0 0 25 5 10 15 20 mm Traversed by Sliding Sled Figure 3: Friction drag force of the sled moving across the surface of the volar forearm on skin that has been wetted to varying degrees. Skin friction increases with increasing levels of hydration. This is consistent with numerous other investigations of skin friction. 5 800 800 800 800 700 800 700 800 700 800 700 800 700 800 700 800 600 700 800 600 700 800 600 700 800 600 700 800 600 700 800 600 700 800 500 600 700 800 500 600 700 800 500 600 700 800 500 600 700 800 400 500 600 700 800 400 500 600 700 800 400 500 600 700 800 400 500 600 700 800 400 500 600 700 800 300 400 500 600 700 800 300 400 500 600 700 800 300 400 500 600 700 800 300 400 500 600 700 800 300 400 500 600 700 800 300 400 500 600 700 800 200 300 400 500 600 700 800 200 300 400 500 600 700 800 200 300 400 500 600 700 800 200 300 400 500 600 700 800 100 200 300 400 500 600 700 800 100 200 300 400 500 600 700 800 100 200 300 400 500 600 700 800 100 200 300 400 500 600 700 800 100 200 300 400 500 600 700 800 100 200 300 400 500 600 700 800 0 100 200 300 400 500 600 700 800 0 100 200 300 400 500 600 700 800 0 100 200 300 400 500 600 700 800 0 100 200 300 400 500 600 700 800 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry 0 100 200 300 400 500 600 700 800 0 5 10 15 20 25 Soaked Wet Moist Dry Dry Moist Wet Soaked Friction Drag Force (grams) 100 0 200 300 400 500 600 700 800 0 25 5 10 15 20 Effect of Moisture on Skin Friction mm Traversed by Sliding Sled Figure 5: Mean (n=9 subjects) frictional drag force of the sled moving 18.8 mm across the surface of the volar forearm at a rate of 5.25 mm/second. Measurements were taken before and two minutes after application of two barrier films. Barrier film A dries more quickly than barrier film B and provides a much smoother surface over which the sled can move. This is evident by a 257% lower coefficient of friction for barrier film A compared to barrier film B. 1400 1200 1300 1400 1100 1200 1300 1400 Product A 1000 1100 1200 1300 1400 Product A Product B 900 1000 1100 1200 1300 1400 Product A Product B 800 900 1000 1100 1200 1300 1400 Product A Product B 700 800 900 1000 1100 1200 1300 1400 Product A Product B 600 700 800 900 1000 1100 1200 1300 1400 Product A Product B 400 500 600 700 800 900 1000 1100 1200 1300 1400 Product A Product B 300 400 500 600 700 800 900 1000 1100 1200 1300 1400 Product A Product B 200 300 400 500 600 700 800 900 1000 1100 1200 1300 1400 Product A Product B 100 200 300 400 500 600 700 800 900 1000 1100 1200 1300 1400 Product A Product B 0 100 200 300 400 500 600 700 800 900 1000 1100 1200 1300 1400 P T 2 Mi P T Product A Product B 0 100 200 300 400 500 600 700 800 900 1000 1100 1200 1300 1400 Pre-Treatment 2 Minutes Post-Treatment Product A Product B Effect of Barrier Film Application on Skin Friction Barrier Film B Barrier Film A 1400 1300 1200 1100 1000 900 800 700 600 500 400 300 200 100 0 Friction Drag Force (grams) Pre-Treatment 2 Minutes Post-Treatment

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Pressure and shear generally receive the majority of attention in the nursing literature when it comes to treating and preventing pressure ulcers. Pressure is a vertical force exerted by gravity pulling on the body. It is generally expressed at a bony prominence where it compresses soft tissue, causing capillary closure leading to ischemia and subsequent cell death. Shear is a horizontal force that acts in concert with pressure to distort tissues and cause narrowing of blood vessels. When sufficient shear is applied, the internal diameter of the capillaries becomes inadequate for blood to flow through them.1 Shear is thought to be up to 10X more destructive than pressure alone because of its ability to cut off large areas of vasculature.1,2

However, shear requires a third element, friction, to exert its destructive effect on skin and subcutaneous tissues.1 Friction causes the body to remain adherent to the support surface while the underlying tissues move.3 Without friction there would be no shear, as the body would simply glide along the support surface. Friction is also involved in skin chafing, particularly when moisture is involved. Chafing occurs when the skin repeatedly rubs against another object causing an abrasion injury. This type of injury is usually limited to the epidermis, and is most frequently seen on elbows and heels of patients that are restless. Chafing and abrasion injuries are often reported as a “sheet burn.” 4

While the importance of friction in the causation of pressure ulcers and chafing injuries is recognized in the nursing literature, relatively little attention has been given to understanding how topically applied products may influence frictional forces on the skin. Therefore an apparatus was constructed for in vivo studies of skin friction (drag) based on DaVinci’s classic sliding sled experiments. The apparatus has proven to be useful in studying the influence of various topically applied products on skin frictional properties.

A computer-controlled sliding sled apparatus based on DaVinci’s �classic sliding sled experiments has been constructed that provides reproducible measurements of skin frictional properties.The sliding sled apparatus can be used to compare the effect of �application of topically applied products on the skin.Two barrier film products produced very different skin friction �measurements. Barrier film A dried quickly to a relatively smooth, lower friction �surface compared to barrier film B.Barrier film B remained tacky two minutes after application, �resulting in a jerky motion of the sled as it traversed the skin, and a 257% higher coefficient of friction compared to barrier film A.

Acknowledgements:Poster design by Lutz Consulting LLC

This study was supported by 3M Health Care

To describe a new motorized sliding sled apparatus based on DaVinci’s classic sliding sled experiments that was constructed for in vivo studies of skin friction properties. This presentation will also summarize data generated during development of the device comparing the effect of two barrier films on skin friction properties.

OverviewTo learn more about the effects of skin care products on frictional properties of the skin, we constructed an apparatus for in vivo studies based on DaVinci’s classic sliding sled experiments.

Test ApparatusThe device consisted of two sandwiched support plates that maintained a parallel path for the sliding sled as it moved across the skin (Figure 1). The upper plate had a linear guide with two moveable blocks, one of which was motorized and under PC control using PWM signals. A rack and pinion system converted rotary motion of the servo motor into linear motion. For this series of experiments, the traverse path was 18.8 mm at 5.25 mm/sec. The other block, which was exposed through a slot in the lower base plate, presented a 32 x 48 mm surface that dragged against the skin (Figure 2). The 48 mm length was comprised of 3 sections, each 16 mm in length, with the center section running parallel to the skin and the leading and trailing edges sloped at 25 degrees. The precise angle to which the sled was pushed against the skin could be varied by inserting or removing shims. The sliding sled was covered with a 55:45 cotton-polyester sheet representative of hospital bedding. This test material was replaced prior to each run.A miniature load cell placed between the interfacing surfaces of the sliding blocks allowed for real time measurement of the compression and tension forces resulting from pushing and pulling the sled. Data acquisition software exported both raw voltages from the load cell and steps made by the servo motor to an EXCEL spreadsheet using a PLX-DAQ macro. Converting imported values to Load (grams) and Distance (mm) was achieved using appropriate calibration factors. Each experiment was run at least in triplicate.Validation studies using rigid substrates in vitro showed that the resulting curves were in keeping with Amonton’s laws and could be used to reliably evaluate both the static and dynamic coefficient of friction. We found from our studies of human skin in vivo that the mechanical properties of the skin dramatically influence the results, and Amonton’s laws no longer provided an adequate description of the frictional forces. Nevertheless, the apparatus has proven to be an effective tool for studying the influence of topically applied products on the frictional properties of the skin.

Hydration & Skin FrictionIt is well documented that as skin becomes increasingly hydrated, there is a corresponding increase in skin frictional properties.5 Thus, skin that is over-hydrated from sweat or incontinence is more susceptible to the destructive forces of shear and chafing.Figure 3 shows the results of a validation experiment to demonstrate sensitivity of the current device to measuring changes in skin frictional properties resulting from hydration. Skin friction was measured at four different hydration levels: 1) dry, 2) moist (hydrated with a few drops of water), 3) wet (5 minute exposure to a wet paper towel), and 4) soaked (10 minutes of complete immersion in water). The data clearly show sensitivity of the device to measuring changes in skin hydration level.

Tacky vs. Non-Tacky Films Barrier films are often used clinically to help prevent maceration of the skin and to protect areas prone to abrasion injury. However, little is known about the effects of barrier films on skin friction properties. Therefore, an experiment was conducted to compare frictional properties of two barrier films two minutes after application to the skin. Barrier film A was a product known for its fast-drying properties, and barrier film B was a product known to be much slower drying.Figure 4 shows triplicate frictional drag force measurements over the two treated sites on a single subject two minutes after application of the barrier films. Barrier film A is dry to the touch and provides a relatively smooth surface over which the sled can move. However, barrier film B is still tacky to the touch two minutes after application. This is evident by an approximately four-fold higher coefficient of friction and a jerky motion of the sled as it attempts to move across the skin surface.In a second experiment, skin friction measurements were taken from the volar forearms of nine subjects before and two minutes after application of

the two barrier films. The results of this experiment (Figure 5) show similar data to the previous experiment. The mean (SD) coefficient of friction for barrier film B two minutes after application was 1062.1 (272) grams, which was 257% higher than barrier film A, 412.4 (98.5) grams (p<0.0001). An interesting observation was that barrier film A showed a small but significant (p<0.0001) increase in skin friction compared to untreated skin, indicating that the clinical effectiveness observed for this product may be related more to protection of the skin from hydration and abrasion forces rather than an actual reduction in the coefficient of friction. However, it is clear that compared to barrier film B there is a significant reduction in skin friction.

Methods

Objective

Results

Conclusions

A Motorized Sliding Sled Apparatus for Measuring the Coefficient of Friction of Human Skin in vivoGary Grove, cyberDERM Clinical Studies, Broomall, PAAram Grigoryan, cyberDERM Special Projects Group, Media, PA

Tim Houser, cyberDERM Special Projects Group, Media, PAJonn Damia, cyberDERM Special Projects Group, Media, PA

Nancy Atwood, Clinical Research Specialist, 3M Health Care, St. Paul, MN

Background

Figure 1: Schematic drawing of the sliding sled device used to measure friction forces on the skin. The device consists of a supportive struc-ture that maintains a parallel path for a sliding sled connected to a motorized unit via a load cell.

Skin Surface

MotorizedUnit

Support Plate & Linear Track

LoadCell Sliding Sled Unit

Electronics & PC Interface

Test material

Figure 2: Photograph of the sliding sled device as it measures compression and tension forces resulting from friction as the sled moves across the surface of the skin. The device can measure the effect of various skin treatments on skin friction.

ReferencesFontaine R, Risley S, Castellino R. A quantitative analysis of pressure and shear in the effectiveness of support surfaces. J 1. Wound Ostomy Continence Nurs 1998;25(5):233-9.

Zhang M, Roberts VC. The effect of shear forces externally applied to skin surface on underlying tissues. J Biomed Eng 2. 1993;15(6):451-6.

Stewart TP. Support Systems. In: Parish LC, Witkowski JA, Crissey JT, editors. The decubitus ulcer in clinical practice. London: 3. Springer; 1997. p. 145-68.

Bryant R, Nix D. Mechanical forces: Pressure, shear, and friction. In: Acute & Chronic Wounds: Current Management Concepts. 4. Third ed: Mosby; 2007. p. 205-34.

Cottenden AM, Wong WK, Cottenden DJ, Farbrot A. Development and validation of a new method for measuring friction 5. between skin and nonwoven materials. Proc Inst Mech Eng [H] 2008;222(5):791-803.

Test ProductsBarrier Film A: Cavilon™ No Sting Barrier Film (3M)

Barrier Film B: Sureprep® No-Sting Skin Barrier (Medline Industries)*

Figure 4: Triplicate drag force measurements of the sled moving across the volar forearm on skin that has been treated with two different barrier films. Barrier film A dries quickly to a smooth surface with a relatively low frictional drag force. Barrier film B is slow to dry and leaves a tacky film even two minutes after application. This is evident by a four-fold higher drag force, and a jerky motion of the sled as it traverses the volar forearm.

Barrier Film A

Barrier Film B

Triplicate Skin Friction Measurements 2 Minutes after Application of Barrier Films

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Figure 3: Friction drag force of the sled moving across the surface of the volar forearm on skin that has been wetted to varying degrees. Skin friction increases with increasing levels of hydration. This is consistent with numerous other investigations of skin friction.5

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Figure 5: Mean (n=9 subjects)frictional drag force of the sled moving 18.8 mm across the surface of the volar forearm at a rate of 5.25 mm/second. Measurements were taken before and two minutes after application of two barrier films. Barrier film A dries more quickly than barrier film B and provides a much smoother surface over which the sled can move. This is evident by a 257% lower coefficient of friction for barrier film A compared to barrier film B.

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