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   <subfield code="a">10.1007/s00419-010-0414-y</subfield>
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   <subfield code="a">(NATIONALLICENCE)springer-10.1007/s00419-010-0414-y</subfield>
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   <subfield code="a">Watching quiet human stance to shake off its straitjacket</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[Michael Günther, Otto Müller, Reinhard Blickhan]</subfield>
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   <subfield code="a">The single-inverted pendulum (SIP) model is still the paradigm describing dynamics and control of quiet human stance in the sagittal plane. We used two methods to verify this paradigm. First, in an experimental approach we acquired kinematic data of both legs of ten subjects at high spatial resolution while quietly standing on two force platforms. We calculated all leg joint angles, the belonging joint torques using inverse dynamics and estimates of joint stiffnesses. Some linear correlations and regressions of both local (joint) and global (COM, COP: centre of mass respectively pressure) variables predicted by the SIP model were investigated. All three verification criteria applied to mean values extracted from experimental data revealed that the SIP is not a valid model for quiet human stance. As a second method, we used computer synthesis to demonstrate that a double-inverted pendulum (DIP) model enters a stable attractor when just the &quot;hip” joint torque is regulated, whereas no torque is applied to the &quot;ankle” joint. Here, angle and torque fluctuations are necessary because such a DIP strategy is of inevitable dynamic character. The two predicted eigenfrequencies of this regulated DIP model approximate the upper and lower limits of the main part of measured power spectra of quiet human stance. We suggest this dynamic necessity to be representative of the biological constraints under which a mechanically unstable inverted multi-segment chain must be stabilised.</subfield>
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   <subfield code="a">Springer-Verlag, 2010</subfield>
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   <subfield code="a">Biomechanical model</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Posture control</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Inverse dynamics</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">Inverted pendulum</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">Double pendulum</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">(Time) sequence : An array of values of measured variables (positional or force components) sampled discretely versus time</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">Trial : Acquisition of one (consistent and synchronised) data set containing all (time) sequences of the measured variables</subfield>
   <subfield code="2">nationallicence</subfield>
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   <subfield code="a">N : Number of trials (60)</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">f s : Sampling frequency of the kinematic data (115.5Hz)</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">f h : High-pass cutoff-frequency of the kinetic data ($${\frac{1}{8}\,{\rm Hz}}$$)</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">SIP : (Single)-inverted pendulum</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">DIP : Double-inverted pendulum</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Segment : A fraction of whole body mass located between joints (right and left foot, shank, thigh plus HAT)</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">HAT : Segment including head, arms, and trunk</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">COM : Centre of mass</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">COP : Centre of pressure</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">HAT-COM : COM of the HAT-segment</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">GRF : Ground reaction force</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">DOF : Degree of freedom</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">s.d. : Standard deviation</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">min : Minimum</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">max : Maximum</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">$${\mathcal{M}}$$ : Body mass</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">g : Gravitational acceleration</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">h : Distance between ankle joint and COM</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Θcom : Moment of inertia for the body rotating around its COM ($${\approx \frac{1}{5}\cdot \mathcal{M}\cdot h^{2}}$$)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Θ : Body moment of inertia for rotation around ankle joint ($${=\mathcal{M}\cdot h^{2} + \Theta_{\rm com}}$$)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">K : Rotational &quot;ankle stiffness” of the SIP model (i.e., unit: Nm/rad)</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">K ankle : Sum of real, measured right and left ankle stiffnesses</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">K crit : Critical &quot;ankle stiffness” ($${= \mathcal{M}\cdot g\cdot h}$$)</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">K eff : Effective stiffness for the SIP model (= K − K crit)</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">ω : Angular eigenfrequency of the SIP model $${\left(=\sqrt{\frac{K - K_{\rm crit}}{\Theta}}\, = \,\sqrt{\frac{K_{\rm eff}}{\Theta}}\right)}$$</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">ν : Eigenfrequency of the SIP model $${\left(= \frac{\omega}{2 \pi}\right)}$$</subfield>
   <subfield code="2">nationallicence</subfield>
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  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">$${\tau_{\rm acc}^{2}}$$ : $${= \frac{\Theta}{K_{\rm crit}}\, = \,\left(\frac{K}{K_{\rm crit}} - 1\right) \cdot \frac{1}{\omega^{2}}\, = \,\frac{K_{\rm eff}}{K_{\rm crit}}\cdot \frac{1}{\omega^{2}}}$$</subfield>
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   <subfield code="a">Günther</subfield>
   <subfield code="D">Michael</subfield>
   <subfield code="u">Orthopädische Klink, Biomechaniklabor, Eberhard-Karls-Universität, Hoppe-Seyler-Straße 3, 72076, Tübingen, Germany</subfield>
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   <subfield code="a">Müller</subfield>
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   <subfield code="a">Blickhan</subfield>
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   <subfield code="u">Institut für Sportwissenschaft, Lehrstuhl für Bewegungswissenschaft, Friedrich-Schiller-Universität, Seidelstraße 20, 07749, Jena, Germany</subfield>
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   <subfield code="t">Archive of Applied Mechanics</subfield>
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