1976
DOI: 10.21236/ada029402
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Mass Distribution of the Human Body using Biostereometrics

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Cited by 21 publications
(8 citation statements)
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“…The global inertia tensor (body + balance pole) is changed as a function of the medio-lateral shifts of the pole carried out by the active stabilization actions, but since the range of such displacement is very small (of the order of cm), the tensor will be assumed to be constant. The moment of inertia of the pole is neglected for rotations around its longitudinal axis and is computed by the following formula for any axis through the CoM of the pole, perpendicular to it: For the body itself, the available numerical estimates of the human body inertia tensor [ 30 , 31 ] are usually expressed in terms of a reference frame centred in the body CoM. For computing the inertia tensor related to a frame centred on the feet, at contact with the supporting wire, it is possible to use the parallel axis theorem, ending up with the following equation for the global inertia tensor: …”
Section: Methodsmentioning
confidence: 99%
“…The global inertia tensor (body + balance pole) is changed as a function of the medio-lateral shifts of the pole carried out by the active stabilization actions, but since the range of such displacement is very small (of the order of cm), the tensor will be assumed to be constant. The moment of inertia of the pole is neglected for rotations around its longitudinal axis and is computed by the following formula for any axis through the CoM of the pole, perpendicular to it: For the body itself, the available numerical estimates of the human body inertia tensor [ 30 , 31 ] are usually expressed in terms of a reference frame centred in the body CoM. For computing the inertia tensor related to a frame centred on the feet, at contact with the supporting wire, it is possible to use the parallel axis theorem, ending up with the following equation for the global inertia tensor: …”
Section: Methodsmentioning
confidence: 99%
“…It is not easy to find realistic anthropometric and biomechanical parameters to be used in model simulation. They are scattered in a number of publications/reports (Herron et al, 1976 ; Roaas and Gunnarb Andresson, 1982 ; Zatsiorsky and Seluyanov, 1983 ; De Leva, 1996 ; NASA-STD-3000, 2000 ; Pavol et al, 2002 ; Hersch and Billard, 2008 ; Paquette et al, 2009 ). The following simulations were carried out by extracting data from the mentioned literature, summarized in Morasso et al ( 2014 ).…”
Section: The Body-schema and Whole-body Reachingmentioning
confidence: 99%
“…The human subject operating Mina v2 in the current experiments is a male, is 1.78 m tall, and has a total mass of 82.8 kg. This mass is similar to that of Subject 2 from a literature study (Herron et al, 1976 ), which is used to estimate the mass distribution of the operator's body segments. The link and mass parameters for the equivalent DH model of the combined human-exoskeleton system were calculated accordingly (Table 2 ).…”
Section: Resultsmentioning
confidence: 89%
“…Lower body link lengths are directly measured from the human operator and used as a reference for modeling the exoskeleton's links such that Mina v2 and its pilot have identical link and foot lengths. The mass distribution of the human body is based on reference data from a biostereometric survey of six male subjects (Herron et al, 1976 ). The masses of human pelvis, torso, arm, and head segments are combined into one point mass located perpendicular to the pelvic link.…”
Section: Combined Human-exoskeleton System: Models and Parametersmentioning
confidence: 99%