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MODELING THE ONSET OF SLIP DURING WALKING MODELING THE ONSET OF SLIP DURING WALKING

MODELING THE ONSET OF SLIP DURING WALKING - PDF document

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Uploaded On 2020-11-23

MODELING THE ONSET OF SLIP DURING WALKING - PPT Presentation

Philip S Requejo1 Judith M Burnfield2 and Jason Leach3 1Pathokinesiology Laboratory Rancho Los Amigos National Rehabilitation Center Downey CA 2Movement Sciences Center Madonna Rehabilitatio ID: 822051

slip walking model heel walking slip heel model floor cofu surface toe horizontal center results simulation trials force determined

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MODELING THE ONSET OF SLIP DURING WALKIN
MODELING THE ONSET OF SLIP DURING WALKINGPhilip S. Requejo1, Judith M. Burnfield2, and Jason Leach31Pathokinesiology Laboratory, Rancho Los Amigos National Rehabilitation Center, Downey, CA 2Movement Sciences Center, Madonna Rehabilitation Hospital, Lincoln, NE3The Rockport Company, Ronks, PAIntroductionPurpose Significance SignificanceExperimentationResultsDiscussionReferencesSlips are a leading cause of falls and injuries in the home and work 1. During walking, the forces generated by the body are U) increases or the friction that is available from the floor A) decreases2. In the research setting, a person's COFU during walking is calculated from force plate U is defined as the ratio between the shear and vertical A of the floor surface can be measured using a device called a Ultimately, the onset and The objective of this work was to ping in order to determine the interaction between human (center of mass (CM) velocity; COFU) and environmental factors (COFA) on slip outcome using anexperimentation and dynamic simulation The reduction of deaths from falls has Both greater horizontal CM velocity 1. Berg et al (1997). Age and Ageing, 2. Hanson et al (1999). Ergonomics, A two-dimensional 8-segment model The model was implemented using a y) were determined from the shoe testing results. The coefficient of friction A) range of the horizontal contact force model (Fx=COFA*Fy) were determined from experimental results and subsequently varied Model Model A simulation study was performed to assess A). At each simulated condition, the stance leg heel horizontal displacement Simulation 04008001200-0.00200.0020.0040.006yf(m)Fy(N)Hqixy(CMx, CMy)heell toel heelr toer llllllllThe peak COFU during non-slip walking trials ( ) was m = 0.246 (± .014) while m = 0.88. The m = 0.17. In this m=0.1) and highest heel m )Experimental kinematic (120Hz, VICON), kinetic (1200Hz, AMTI), and video data were recorded simultaneously as a healthy 30 year old female (height 1.59 m; mass 65.7 kg) normal and reduced floor surface slip resistance. walking shoes (Rockport model MWT18) for use multiple non-slip walking trials, WD-40 was applied to the surface of the from kinematic data. The peak COFU value during weight acceptance was determined speed matched non-slip walking trials. The A of the clean and contaminated floor surface (English XL). To determine the material properties associated with the shoes, ten separate pairs were tested (MTS 858 Test System). The average vertical force-testing were modeled using an exponential function:with k= 3.8x108 (heel), 8.4x108 (toe) and C= 2.0 x107 (heel), 9.0 x107 (toe). 2.451.850=++&yfffkyCyyF