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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Comput. Neurosci.</journal-id>
<journal-title>Frontiers in Computational Neuroscience</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Comput. Neurosci.</abbrev-journal-title>
<issn pub-type="epub">1662-5188</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fncom.2017.00045</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Neuroscience</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Hammering Does Not Fit Fitts&#x00027; Law</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Petri&#x0010D;</surname> <given-names>Tadej</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<xref ref-type="author-notes" rid="fn002"><sup>&#x02020;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/134244/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Simpson</surname> <given-names>Cole S.</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
<xref ref-type="author-notes" rid="fn002"><sup>&#x02020;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/386251/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Ude</surname> <given-names>Ale&#x00161;</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/154427/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Ijspeert</surname> <given-names>Auke J.</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/36389/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Biorobotics Laboratory, &#x000C9;cole Polytechnique F&#x000E9;d&#x000E9;rale de Lausanne</institution> <country>Lausanne, Switzerland</country></aff>
<aff id="aff2"><sup>2</sup><institution>Department of Automatics, Biocybernetics and Robotics, Jo&#x0017E;ef Stean Institute</institution> <country>Ljubljana, Slovenia</country></aff>
<aff id="aff3"><sup>3</sup><institution>George W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology</institution> <country>Atlanta, GA, United States</country></aff>
<aff id="aff4"><sup>4</sup><institution>Mechanical Engineering Department, Stanford University</institution> <country>Stanford, CA, United States</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Francisco J. Valero-Cuevas, University of Southern California, United States</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Bastien Berret, University of Paris-Sud, Universit Paris-Saclay, France; J. Michael Herrmann, University of Edinburgh, United Kingdom</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Tadej Petri&#x0010D; <email>tadej.petric&#x00040;ijs.si</email></p></fn>
<fn fn-type="other" id="fn002"><p>&#x02020;These authors have contributed equally to this work.</p></fn></author-notes>
<pub-date pub-type="epub">
<day>29</day>
<month>05</month>
<year>2017</year>
</pub-date>
<pub-date pub-type="collection">
<year>2017</year>
</pub-date>
<volume>11</volume>
<elocation-id>45</elocation-id>
<history>
<date date-type="received">
<day>19</day>
<month>10</month>
<year>2016</year>
</date>
<date date-type="accepted">
<day>15</day>
<month>05</month>
<year>2017</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2017 Petri&#x0010D;, Simpson, Ude and Ijspeert.</copyright-statement>
<copyright-year>2017</copyright-year>
<copyright-holder>Petri&#x0010D;, Simpson, Ude and Ijspeert</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) or licensor are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract>
<p>While movement is essential to human wellbeing, we are still unable to reproduce the deftness and robustness of human movement in automatons or completely restore function to individuals with many types of motor impairment. To better understand how the human nervous system plans and controls movements, neuromechanists employ simple tasks such as upper extremity reaches and isometric force tasks. However, these simple tasks rarely consider impacts and may not capture aspects of motor control that arise from real-world complexity. Here we compared existing models of motor control with the results of a periodic targeted impact task extended from Bernstein&#x00027;s seminal work: hammering a nail into wood. We recorded impact forces and kinematics from 10 subjects hammering at different frequencies and with hammers with different physical properties (mass and face area). We found few statistical differences in most measures between different types of hammer, demonstrating human robustness to minor changes in dynamics. Because human motor control is thought to obey optimality principles, we also developed a feedforward optimal simulation with a neuromechanically inspired cost function that reproduces the experimental data. However, Fitts&#x00027; Law, which relates movement time to distance traveled and target size, did not match our experimental data. We therefore propose a new model in which the distance moved is a logarithmic function of the time to move that yields better results (<italic>R</italic><sup>2</sup> &#x02265; 0.99 compared to <italic>R</italic><sup>2</sup> &#x02265; 0.88). These results support the argument that humans control movement in an optimal way, but suggest that Fitts&#x00027; Law may not generalize to periodic impact tasks.</p>
</abstract>
<kwd-group>
<kwd>motor control</kwd>
<kwd>biomechanics</kwd>
<kwd>upper extremity</kwd>
<kwd>optimal control</kwd>
<kwd>arm movement</kwd>
<kwd>impact</kwd>
<kwd>Fitts&#x00027; Law</kwd>
</kwd-group>
<counts>
<fig-count count="8"/>
<table-count count="6"/>
<equation-count count="4"/>
<ref-count count="54"/>
<page-count count="12"/>
<word-count count="7176"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>Introduction</title>
<p>Movement is essential to human wellbeing. However, the control of movement is a very difficult problem. To produce deft and robust movements, the human nervous system must continuously control over 600 muscles while handling nonlinearities, nonstationarities, delays, noise, and uncertainties (Franklin and Wolpert, <xref ref-type="bibr" rid="B18">2011</xref>). Despite these difficulties, humans move with apparent ease. However, human motor capability may become impaired due to age, illness, or injury. Robotic systems are also faced with many of the same challenges (Egeland et al., <xref ref-type="bibr" rid="B15">1991</xref>; Park, <xref ref-type="bibr" rid="B36">2002</xref>; Guigon et al., <xref ref-type="bibr" rid="B21">2007</xref>; Peters et al., <xref ref-type="bibr" rid="B37">2009</xref>), but meet with much less success than their healthy human counterparts (Yang et al., <xref ref-type="bibr" rid="B52">2011</xref>; Vanderborght et al., <xref ref-type="bibr" rid="B50">2013</xref>). A better understanding of the roles that the nervous and musculoskeletal systems play in producing movement will likely lead to advances in rehabilitation and robotic control.</p>
<p>Many neuromechanists employ simple tasks to study the nervous system in action under controlled conditions. Isometric tasks in which subjects interact with an immoble force sensor and reaching tasks in which the hand is moved from one point to another are commonly used to study sensorimotor learning (Rotella et al., <xref ref-type="bibr" rid="B38">2015</xref>), movement control (Fitts, <xref ref-type="bibr" rid="B16">1954</xref>), and neurophysiology (Shadmehr and Krakauer, <xref ref-type="bibr" rid="B40">2008</xref>) in the upper extremity. Subjects may also be asked to interact with robotic co-workers that can record reaching dynamics (Burdet et al., <xref ref-type="bibr" rid="B9">2001</xref>), generate disturbances, or create force fields (Shadmehr and Mussa-Ivaldi, <xref ref-type="bibr" rid="B41">1994</xref>) during these tasks. When carefully considered, these experiments can provide a wealth of information on how the nervous system controls movement. However, these tasks are greatly simplified from real-world tasks. To study more complex tasks, some researchers have developed simple games, such as conkers, to study sensoriomotor learning (Sternad et al., <xref ref-type="bibr" rid="B44">2011</xref>). However, even these studies simplify real-world tasks and rarely consider certain features of real-world tasks such as impacts.</p>
<p>Despite many possible ways to perform most tasks (Bernstein, <xref ref-type="bibr" rid="B6">1967</xref>), upper extremity movements are highly stereotyped. Researchers note consistent characteristics such as bell-shaped velocity curves (Hollerbach and Atkeson, <xref ref-type="bibr" rid="B25">1987</xref>; Berardelli et al., <xref ref-type="bibr" rid="B5">1996</xref>) and speed-accuracy tradeoffs characterized by Fitts&#x00027; Law (Fitts, <xref ref-type="bibr" rid="B16">1954</xref>; Bootsma et al., <xref ref-type="bibr" rid="B7">2004</xref>; Zhai et al., <xref ref-type="bibr" rid="B54">2004</xref>). Fitts&#x00027; Law expresses the time to complete a reach as a logarithmic function of the size of the target and the distance to the target (see Equation 1). In experiments relating to Fitts&#x00027; Law, the kinematics (the beginning and final position of the arm or cursor) are prescribed and the subject is left to determine the time to reach. In certain periodic movements however, the time to complete an upper extremity movement can be specified and the subject left to determine the kinematics.</p>
<p>Movement is constantly refined by biological processes such as learning and evolution (Todorov, <xref ref-type="bibr" rid="B46">2004</xref>). Because of this constant refinement, many researchers note that optimal control models utilizing cost functions such as minimum variance (Harris and Wolpert, <xref ref-type="bibr" rid="B22">1998</xref>), minimum effort (Crowninshield and Brand, <xref ref-type="bibr" rid="B12">1981</xref>), minimum jerk (Flash and Hogan, <xref ref-type="bibr" rid="B17">1985</xref>), and minimum torque change (Uno et al., <xref ref-type="bibr" rid="B48">1989</xref>) can be excellent models for the nervous system. In fact, many of the observed stereotypical behaviors discussed in the previous paragraph can be explained by optimality principles. Optimal control models have been used to reproduce human-like behaviors such as reaches (Todorov and Li, <xref ref-type="bibr" rid="B47">2005</xref>), walking (Anderson and Pandy, <xref ref-type="bibr" rid="B3">2001</xref>), and jumps (Anderson and Pandy, <xref ref-type="bibr" rid="B2">1999</xref>; Ong et al., <xref ref-type="bibr" rid="B35">2016</xref>). Though occasionally studied (C&#x000F4;t&#x000E9; et al., <xref ref-type="bibr" rid="B11">2008</xref>; M&#x000FC;ller and Sternad, <xref ref-type="bibr" rid="B32">2009</xref>), one activity that remains conspicuously unmodeled is Bernstein&#x00027;s hammering task (Bernstein, <xref ref-type="bibr" rid="B6">1967</xref>; M&#x000FC;ller and Sternad, <xref ref-type="bibr" rid="B32">2009</xref>) that inspired much research into motor control and learning.</p>
<p>Here we extend Bernstein&#x00027;s hammering task into a targeted periodic impact task. We recorded impact forces and upper extremity kinematics in hammering. In order to examine how hammering strategies might change with different conditions, we used a set of hammers with different physical properties (hammer face area and mass) and prescribe different hammering frequencies. We hypothesized that hammering impact velocity and maximal height attained are the result of a tradeoff between maximizing task performance (quantified here as a maximal impact velocity) and minimizing effort (Crowninshield and Brand, <xref ref-type="bibr" rid="B12">1981</xref>; Nelson, <xref ref-type="bibr" rid="B33">1983</xref>). In order to test whether the mechanics of this task adhere to current theories in optimal human motor control, we implemented a feedforward optimal controller (Todorov, <xref ref-type="bibr" rid="B46">2004</xref>) on a planar torque-driven 3-segment dynamical model of the upper extremity holding a hammer (<bold>Figure 8</bold>) using model parameters from Winter (<xref ref-type="bibr" rid="B51">2009</xref>). Our results show that humans appear to select optimal impact velocities that reflect a tradeoff between accomplishing the task and minimizing effort that do not adhere to Fitts&#x00027; Law.</p>
</sec>
<sec sec-type="methods" id="s2">
<title>Methods</title>
<sec>
<title>Subjects</title>
<p>Ten healthy male volunteers (age &#x0003D; 27.6 &#x000B1; 3.6 years, height &#x0003D; 176.9 &#x000B1; 5 cm, weight &#x0003D; 77.7 &#x000B1; 11.2 kg) participated in the study. All subjects were right-handed and had no known neuromotor or sensory disorders (self-reported). Prior to their participation, subjects were informed of the course of study and gave their written informed consent in accordance with the code for ethical conduct in research at the Swiss Federal Institute of Technology (EPFL). This study was approved by the EPFL Human Research Ethics Committee (HREC No.: 008-2015/17.08.2015).</p>
</sec>
<sec>
<title>Experimental protocol</title>
<p>Each subject was asked to step in front of a table on top of which was a wooden board mounted on a force plate (Kistler Instrument AG, Winterhur, Switzerland) as shown in Figure <xref ref-type="fig" rid="F1">1</xref>. Subjects were given one of four differently sized and weighted hammers (Table <xref ref-type="table" rid="T1">1</xref>) and asked to drive a pre-started nail, i.e., a nail that had previously been driven to the point at which it would stand on its own, into the wooden board while matching their hammer strikes to the clicks of a metronome. Please note that subjects were not explicitly instructed to strike with their maximum impact speed but were allowed to self-select the best impact speed for their skill level. The metronome was set to one of five frequencies: 1, 2, 3, 4, or 5 Hz. The hammer used and metronome frequency for each trial were randomized. Note that subjects were not allowed to do a training trial first, but we assume that the random trial order cancels any learning effects. Subjects were allowed to use their nondominant hands to stabilize the wooden board. In each trial, the forces on the wooden board and the kinematic motion (14 Prime Series cameras, OptiTrac, USA) of the upper extremity and hammer were recorded at 1 kHz and 250 Hz, respectively. After completing the experimental trials, subjects were asked to subjectively rank each of the hammers in order from most to least preferred.</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Experimental setup of the study. Each subject was asked to stand in front of a table on top of which a wooden board was placed on a force plate. Subjects were given one of four differently sized and weighted hammers at random and asked to drive a nail into the wooden board. The hammering frequency was controlled by asking each subject to match their hammer strikes with the clicks of a metronome. The forces on the wooden board were recorded by the force plate and the kinematic motion of the subjects&#x00027; arms and of the hammer were recorded using an optical motion capture system.</p></caption>
<graphic xlink:href="fncom-11-00045-g0001.tif"/>
</fig>
<table-wrap position="float" id="T1">
<label>Table 1</label>
<caption><p>Specifications of the hammers used in these experiments.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Hammer</bold></th>
<th valign="top" align="center"><bold>Face size [cm &#x000D7; cm]</bold></th>
<th valign="top" align="center"><bold>Weight [kg]</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Small heavy</td>
<td valign="top" align="center">1.4 &#x000D7; 1.4</td>
<td valign="top" align="center">0.402</td>
</tr>
<tr>
<td valign="top" align="left">Small light</td>
<td valign="top" align="center">1.4 &#x000D7; 1.4</td>
<td valign="top" align="center">0.218</td>
</tr>
<tr>
<td valign="top" align="left">Big heavy</td>
<td valign="top" align="center">2.2 &#x000D7; 2.2</td>
<td valign="top" align="center">0.394</td>
</tr>
<tr>
<td valign="top" align="left">Big light</td>
<td valign="top" align="center">2.2 &#x000D7; 2.2</td>
<td valign="top" align="center">0.217</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec>
<title>Data processing</title>
<p>Statistical analyses were performed using the Statistics and Machine Learning Toolbox in Matlab. We calculated the hammer velocity, average maximal heights of the hammer, average times required for the hammer to go from maximal height to impact, and average maximal impact forces during hammering for each subject. We then used these average values from each subject for statistical analyses. We investigated the effects of time to impact, maximum height of the movement, and maximal force normalized with the hammer weight using two-way repeated-measures ANOVA with independent variables [hammers(4)&#x000D7;(frequency(5)]. The effect of maximum height of the movement, and maximal force normalized with the hammer weight for each combination of hammers and frequency was further determined using one-way repeated measures ANOVA. The differences between maximal heights and the differences between the normalized maximum forces at impact were tested with <italic>post-hoc t</italic>-tests with Bonferroni correction. The level of statistical significance used was 0.05 for all statistical tests.</p>
</sec>
<sec>
<title>Modeling</title>
<p>In order to determine whether human hammering strategies adhere to Fitts&#x00027; Law (Fitts, <xref ref-type="bibr" rid="B16">1954</xref>; Bootsma et al., <xref ref-type="bibr" rid="B7">2004</xref>; Zhai et al., <xref ref-type="bibr" rid="B54">2004</xref>), we attempted to fit Fitts&#x00027; model,</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M1"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi>a</mml:mi><mml:mo>&#x0002B;</mml:mo><mml:mi>b</mml:mi><mml:mo>&#x000B7;</mml:mo><mml:mi>l</mml:mi><mml:mi>o</mml:mi><mml:msub><mml:mrow><mml:mi>g</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>D</mml:mi><mml:mo>/</mml:mo><mml:mi>W</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>with data collected in our experiment. In this formulation, the movement time, <italic>T</italic><sub><italic>f</italic></sub>, is a function of the distance from the hammer at peak height to the nail, <italic>D</italic>, and the face width of the hammer, <italic>W</italic>. The values of <italic>a</italic> and <italic>b</italic> were selected using a least squares difference regression.</p>
<p>In order to examine whether the human nervous system uses optimality principles to control hammering movements, we employed a feedforward optimal controller on two joints (shoulder and elbow) while the wrist was maintained at a desired position with an impedance controller. The human arm holding a hammer was modeled as a 3 link torque-driven robot operating in the saggital plane (<bold>Figure 8</bold>, right-hand column) whose parameters were computed based on data from Winter (<xref ref-type="bibr" rid="B51">2009</xref>) (see Appendix for more details) and whose dynamics are given by</p>
<disp-formula id="E2"><label>(2)</label><mml:math id="M2"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mo>&#x003C4;</mml:mo><mml:mo>&#x0002B;</mml:mo><mml:mstyle mathvariant='bold'><mml:mi>J</mml:mi></mml:mstyle><mml:mi>T</mml:mi><mml:msub><mml:mrow><mml:mstyle mathvariant='bold'><mml:mi>F</mml:mi></mml:mstyle></mml:mrow><mml:mrow><mml:mi>e</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle mathvariant='bold'><mml:mi>H</mml:mi></mml:mstyle><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>q</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>q</mml:mi></mml:mrow><mml:mo>&#x000A8;</mml:mo></mml:mover><mml:mo>&#x0002B;</mml:mo><mml:mstyle mathvariant='bold'><mml:mi>h</mml:mi></mml:mstyle><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mover accent="true"><mml:mrow><mml:mi>q</mml:mi></mml:mrow><mml:mo>&#x002D9;</mml:mo></mml:mover></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>&#x0002B;</mml:mo><mml:mi>g</mml:mi><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>where &#x003C4; is a vector of joint torques, <italic>q</italic>, <inline-formula><mml:math id="M3"><mml:mover accent="true"><mml:mrow><mml:mi>q</mml:mi></mml:mrow><mml:mo>&#x002D9;</mml:mo></mml:mover></mml:math></inline-formula>, and <inline-formula><mml:math id="M4"><mml:mover accent="true"><mml:mrow><mml:mi>q</mml:mi></mml:mrow><mml:mo>&#x000A8;</mml:mo></mml:mover></mml:math></inline-formula> are vectors describing the joint angular position, velocity, and acceleration respectively, <italic><bold>H</bold></italic>(<italic>q</italic>) is the inertia matrix, <inline-formula><mml:math id="M5"><mml:mstyle mathvariant='bold'><mml:mi>h</mml:mi></mml:mstyle><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>q</mml:mi><mml:mo>,</mml:mo><mml:mover accent="true"><mml:mrow><mml:mi>q</mml:mi></mml:mrow><mml:mo>&#x002D9;</mml:mo></mml:mover></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math></inline-formula> consists of the Coriolis, centrifugal, and viscous friction force vectors, <italic>g</italic> is the gravity force vector, <italic>F</italic><sub><italic>e</italic></sub> is a vector representing external forces (zero throughout the simulation), and <italic><bold>J</bold><sup>T</sup></italic> is the transpose of the Jacobian matrix. The model was simulated in Matlab using a time step of 0.001 s beginning at the instant after one impact and terminating at the time of the next impact.</p>
<p>Human hammering is a difficult control task due to the need to balance energy transfer to the nail with accuracy. We hypothesize that the human nervous system determines an optimal tradeoff between maximal impact velocity (complete the task in the most effective manner) and minimal effort (Crowninshield and Brand, <xref ref-type="bibr" rid="B12">1981</xref>; Nelson, <xref ref-type="bibr" rid="B33">1983</xref>; Missenard and Fernandez, <xref ref-type="bibr" rid="B30">2011</xref>). We thus determine the optimal joint torques by minimizing the cost function,</p>
<disp-formula id="E3"><label>(3)</label><mml:math id="M6"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>C</mml:mi><mml:mi>o</mml:mi><mml:mi>s</mml:mi><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mo>-</mml:mo><mml:mo>&#x003B1;</mml:mo></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mfrac><mml:mrow><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:msubsup><mml:mrow><mml:mo>&#x003C4;</mml:mo></mml:mrow><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mo>&#x003C4;</mml:mo></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>-</mml:mo><mml:mo>&#x003B1;</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>-</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mrow><mml:mi>y</mml:mi></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>C</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mo>&#x01E8F;</mml:mo></mml:mrow><mml:mrow><mml:mi>m</mml:mi><mml:mi>a</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>where &#x003C4;<sub><italic>i,j</italic></sub> represents joint torques for <italic>i</italic> &#x0003D; 1, &#x02026;, <italic>n</italic> joints over <italic>j</italic> &#x0003D; 1, &#x02026;, <italic>T</italic> discretized time points, <italic>y</italic><sub><italic>T</italic></sub> and <italic>y</italic><sub><italic>T</italic>&#x02212;1</sub> are the vertical positions of the hammer head at the last and second-to-last time points of the simulation, 0 &#x02264; &#x003B1; &#x02264; 1 was designed as an expertise factor to represent the tradeoff in relative emphasis between impact velocity and effort (large &#x003B1; places more emphasis on energy transfer to the nail and a small &#x003B1; places more emphasis on effort conservation), <italic>C</italic><sub>&#x003C4;<sub><italic>max</italic></sub></sub> is a scaling factor representing maximal effort (i.e., if maximal torque is applied for the duration of the simulation), and <italic>C</italic><sub>&#x01E8F;<sub><italic>max</italic></sub></sub> is a scaling factor representing the maximum achievable impact velocity. We compute <italic>C</italic><sub>&#x003C4;<sub><italic>max</italic></sub></sub> as the discrete integral of the joint torque limits (whichever direction has the larger magnitude) over the length of the simulation and <italic>C</italic><sub>&#x01E8F;<sub><italic>max</italic></sub></sub> by simulating a hammer trajectory in which &#x003B1; &#x0003D; 1 and <italic>C</italic><sub>&#x01E8F;<sub><italic>max</italic></sub></sub> &#x0003D; 1. Because maximum effort and final velocity depend on the length of the simulation, we computed unique values of <italic>C</italic><sub>&#x01E8F;<sub><italic>max</italic></sub></sub> and <italic>C</italic><sub>&#x003C4;<sub><italic>max</italic></sub></sub> for each hammering frequency. We constrain the model so that the hammer hits the same place in subsequent impacts ((<italic>x</italic><sub>0</sub>, <italic>y</italic><sub>0</sub>) &#x0003D; (<italic>x</italic><sub><italic>T</italic></sub>, <italic>y</italic><sub><italic>T</italic></sub>)) and there is no initial velocity ((&#x01E8B;<sub>0</sub>, &#x01E8F;<sub>0</sub>) &#x0003D; (0, 0)). We match the initial posture (location of (<italic>x</italic><sub>0</sub>, <italic>y</italic><sub>0</sub>) relative to the simulated shoulder) to the average posture used by our subjects determined by inverse kinematics. The terms, <italic>C</italic><sub>&#x003C4;<sub><italic>max</italic></sub></sub> and <italic>C</italic><sub>&#x01E8F;<sub><italic>max</italic></sub></sub>, are scaling factors included to facilitate direct comparison of the two terms making up the cost function, minimum effort and maximum final impact velocity. In order to determine whether the parameter, &#x003B1;, is constant within or across individuals, contours of constant &#x003B1; were generated and compared with experimental results. The optimal joint torques were determined using the interior point method implemented with the Matlab Optimization Toolbox.</p>
</sec>
</sec>
<sec sec-type="results" id="s3">
<title>Results</title>
<sec>
<title>Experimental results</title>
<p>Subjects were adept at matching hammering frequency with most of those dictated by the metronome. The hammering frequencies achieved by the subjects for metronome frequencies 1, 2, 3, 4, and 5 Hz were 0.99 &#x000B1; 0.01, 2.02 &#x000B1; 0.01, 3.01 &#x000B1; 0.03, 4.01 &#x000B1; 0.01, and 4.71 &#x000B1; 0.04 Hz respectively (mean &#x000B1; standard error). Hammering frequencies of 5 Hz were too fast for our subjects to reliably match. A hammering frequency of 1 Hz was uncomfortably slow for most subjects. To compensate, many subjects developed a strategy of pausing after each impact before initating an up-and-down hammering motion at a more comfortable frequency (Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F3">3</xref>).</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Vertical movement for all hammers and frequencies. The normalized vertical position of the hammer head was plotted with respect to time. Solid lines indicate the average trajectory while shading represents standard error. The black dashed line indicates the optimal behavior of the model using an estimated &#x003B1; parameter for frequencies 1, 2, 3, 4, and 5 Hz. The root mean squared error (RMSE) of the model for each case has a root mean squared error of <italic>RMSE</italic> &#x0003C; 0.1.</p></caption>
<graphic xlink:href="fncom-11-00045-g0002.tif"/>
</fig>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Speeds for all hammers and frequencies. The speed (magnitude of the velocity vector) of the hammer head was plotted with respect to time. Solid lines indicate the average speeds while shading represents standard deviation. The black dashed line indicates the optimal behavior of the model using an estimated &#x003B1; parameter for frequencies 1, 2, 3, 4, and 5 Hz. The root mean squared error (RMSE) of the model for each case has a root mean squared error of <italic>RMSE</italic> &#x0003C; 0.1 m/s.</p></caption>
<graphic xlink:href="fncom-11-00045-g0003.tif"/>
</fig>
<p>Vertical trajectories (Figure <xref ref-type="fig" rid="F2">2</xref>) and speeds (Figure <xref ref-type="fig" rid="F3">3</xref>) exhibited by the subjects in hammering showed very few differences between the different hammers. However, decreasing the hammering frequency increased the variability in these movements. Rather than the single bell-shaped speed profile characteristic of reaching movements, subjects showed a bell-shaped speed profile for raising the hammer and another truncated bell-shaped speed profile for the descending motion (Figure <xref ref-type="fig" rid="F3">3</xref>).</p>
<p>Analysis of variance showed significant effects of both hammers [<italic>F</italic><sub>(1.61, 14.5)</sub> &#x0003D; 4.95, <italic>p</italic> &#x0003D; 0.03] and frequencies [<italic>F</italic><sub>(1.14, 20.25)</sub> &#x0003D; 22.35, <italic>p</italic> &#x0003C; 0.01] on the time to impact from maximum height. There was no significant interaction [<italic>F</italic><sub>(1.73, 16.05)</sub> &#x0003D; 2.56, <italic>p</italic> &#x0003D; 0.11] between the effects of hammers and frequencies on the time to impact from maximum height. The diagram in Figure <xref ref-type="fig" rid="F4">4</xref> shows the means and standard errors (SEM) of time to impact for all hammers and frequencies.</p>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Means and standard errors (SEM) of time to impact for all hammers and frequencies. The time from maximal height to impact was statistically the same for all hammers at each hammering frequency despite some statistically different maximal heights (Figure <xref ref-type="fig" rid="F5">5</xref>). The time to impact decreases and becomes less variable as the hammering frequency increases.</p></caption>
<graphic xlink:href="fncom-11-00045-g0004.tif"/>
</fig>
<p>Analysis of variance showed significant effects of hammers and frequencies on the normalized maximal heights. Significant effects of both hammers [<italic>F</italic><sub>(2.91, 26.2)</sub> &#x0003D; 22.8, <italic>p</italic> &#x0003C; 0.01], frequencies [<italic>F</italic><sub>(1.77, 15.99)</sub> &#x0003D; 53.09, <italic>p</italic> &#x0003C; 0.01] and interaction between hammers and frequencies [<italic>F</italic><sub>(4.14, 37.26)</sub> &#x0003D; 2.71, <italic>p</italic> &#x0003D; 0.04] were observed. Further analysis of the effects of hammers on normalized maximal heights showed significant effects of hammers [<italic>F</italic><sub>(3, 27)</sub> &#x0003D; 6.46&#x02212;11.08, <italic>p</italic> &#x0003C; 0.01] in all frequencies. <italic>Post-hoc t</italic>-tests showed that Big Light and Small Heavy maximal heights were statistically different from any of the others [<italic>t</italic><sub>(9)</sub> &#x0003D; 2.97&#x02212;5.75, <italic>p</italic> &#x0003C; 0.01]. The diagram in Figure <xref ref-type="fig" rid="F5">5</xref> shows the means and standard errors (SEM) of normalized maximal heights for all hammers and frequencies.</p>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>Means and standard errors (SEM) of the normalized maximal height of all hammers and frequencies. The normalized vertical height of the hammer head decreases as hammering frequency increases. Big Light and Small Heavy maximal heights were statistically different from any of the others (<sup>&#x0002A;</sup><italic>p</italic> &#x0003C; 0.05).</p></caption>
<graphic xlink:href="fncom-11-00045-g0005.tif"/>
</fig>
<p>Similarly, analysis of variance showed significant effects of hammers and frequencies on the impact forces normalized by hammer mass. Significant effects of both hammers [<italic>F</italic><sub>(2.06, 23.42)</sub> &#x0003D; 32.07, <italic>p</italic> &#x0003C; 0.01], frequencies [<italic>F</italic><sub>(1.34, 12.07)</sub> &#x0003D; 6.84], but no significant effect of interaction between hammers and frequencies [<italic>F</italic><sub>(4.39, 39.55)</sub> &#x0003D; 0.69, <italic>p</italic> &#x0003D; 0.63] were observed. Further analysis of the effects of hammers on the impact forces normalized by hammer mass showed significant effects of hammers [<italic>F</italic><sub>(3, 27)</sub> &#x0003D; 11.8&#x02212;17.97, <italic>p</italic> &#x0003C; 0.01] in all frequencies. <italic>Post-hoc t</italic>-tests showed that Small Heavy was statistically different than Small Light [<italic>t</italic><sub>(9)</sub> &#x0003D; 4.71&#x02212;5.65, <italic>p</italic> &#x0003C; 0.01] and Big Heavy [<italic>t</italic><sub>(9)</sub> &#x0003D; 5.4&#x02212;6.61, <italic>p</italic> &#x0003C; 0.01], and Big Heavy was statistically different than Big Light [<italic>t</italic><sub>(9)</sub> &#x0003D; 3.04&#x02212;3.91, <italic>p</italic> &#x0003C; 0.01] for all frequencies. The diagram in Figure <xref ref-type="fig" rid="F6">6</xref> shows the means and standard errors (SEM) of impact forces normalized by hammer mass for all hammers and frequencies. The number of impacts needed to totally drive in the nail under each condition&#x02013;a function of impact velocity&#x02013;are reported in the appendix (Table <xref ref-type="table" rid="T6">A2</xref>).</p>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>Means and standard errors (SEM) of the normalized maximal impact forces for all hammers and frequencies. Impact forces normalized by hammer mass varied between hammers. The heavy hammers generally had lower impact forces per unit mass than the lighter hammers across hammering frequencies. The Small Heavy hammer had the lowest normalized impact forces across conditions. The Big Light hammer produced the highest normalized impact forces, though the Big Heavy hammer produced the largest absolute impact forces. The Small Light and Big Heavy hammers were similar with statistical differences only found at 2 Hz (<sup>&#x0002A;</sup><italic>p</italic> &#x0003C; 0.05).</p></caption>
<graphic xlink:href="fncom-11-00045-g0006.tif"/>
</fig>
</sec>
<sec>
<title>Modeling results</title>
<p>Fitts&#x00027; Law accurately predicted the movement time from the maximum height to impact (<italic>R</italic><sup>2</sup> &#x02265; 0.88). However, despite the high value of <italic>R</italic><sup>2</sup>, the accepted formulation for Fitts&#x00027; Law does not appear to follow the contours of the experimental data (Figure <xref ref-type="fig" rid="F7">7</xref>, light gray traces). Therefore, we propose a slightly altered model that reverses the relationship between movement time and distance to move and was able to improve upon Fitts&#x00027; predictions (<italic>R</italic><sup>2</sup> &#x02265; 0.99),</p>
<disp-formula id="E4"><label>(4)</label><mml:math id="M7"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>D</mml:mi><mml:mo>=</mml:mo><mml:mi>W</mml:mi><mml:mo>/</mml:mo><mml:mn>2</mml:mn><mml:mtext>&#x000A0;</mml:mtext><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>a</mml:mi><mml:mo>&#x0002B;</mml:mo><mml:mi>b</mml:mi><mml:mo>&#x000B7;</mml:mo><mml:mi>l</mml:mi><mml:mi>o</mml:mi><mml:msub><mml:mrow><mml:mi>g</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>f</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>where <italic>D</italic> is the maximal height of the hammer, <italic>T</italic><sub><italic>f</italic></sub> is the time from the maximal height to impact in milliseconds, <italic>W</italic> is the minimum width of the hammer face (our hammers were square, so both face length and width were the same), and <italic>a</italic> and <italic>b</italic> are parameters fit to the data using a least squares difference regression (Table <xref ref-type="table" rid="T2">2</xref>).</p>
<fig id="F7" position="float">
<label>Figure 7</label>
<caption><p>Relationship between time to impact and maximal height for all four hammers. The average normalized height was plotted with respect to average time to impact for each hammer. Fitts&#x00027; Law was fit to the experimental data and overlayed on the experimental data (gray curves, <italic>R</italic><sup>2</sup> &#x02265; 0.88, <italic>RMSE</italic> &#x02264; 0.24). Because Fitts&#x00027; Law appears to have opposite curvature to the experimental data, a modified model was developed (Equation 4) and overlayed on the experimental results (colored traces, <italic>R</italic><sup>2</sup> &#x02265; 0.99, <italic>RMSE</italic> &#x02264; 0.02).</p></caption>
<graphic xlink:href="fncom-11-00045-g0007.tif"/>
</fig>
<table-wrap position="float" id="T2">
<label>Table 2</label>
<caption><p>Parameter estimations for Equation (4) and the original Fitts&#x00027; Law Equation (1).</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>New model</bold></th>
<th valign="top" align="center"><bold><italic>a</italic></bold></th>
<th valign="top" align="center"><bold><italic>b</italic></bold></th>
<th valign="top" align="center"><bold>SSE</bold></th>
<th valign="top" align="center"><bold>RMSE</bold></th>
<th valign="top" align="center"><bold><italic>R</italic><sup>2</sup></bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Small heavy</td>
<td valign="top" align="center">&#x02212;135</td>
<td valign="top" align="center">30.6</td>
<td valign="top" align="center">0.0005</td>
<td valign="top" align="center">0.015</td>
<td valign="top" align="center">0.99</td>
</tr>
<tr>
<td valign="top" align="left">Small light</td>
<td valign="top" align="center">&#x02212;150</td>
<td valign="top" align="center">34.5</td>
<td valign="top" align="center">0.0001</td>
<td valign="top" align="center">0.007</td>
<td valign="top" align="center">0.99</td>
</tr>
<tr>
<td valign="top" align="left">Big heavy</td>
<td valign="top" align="center">&#x02212;119</td>
<td valign="top" align="center">25.4</td>
<td valign="top" align="center">0.0012</td>
<td valign="top" align="center">0.020</td>
<td valign="top" align="center">0.99</td>
</tr>
<tr>
<td valign="top" align="left">Big light</td>
<td valign="top" align="center">&#x02212;103</td>
<td valign="top" align="center">24.4</td>
<td valign="top" align="center">0.0008</td>
<td valign="top" align="center">0.016</td>
<td valign="top" align="center">0.99</td>
</tr>
<tr style="border-top: thin solid #000000;">
<td valign="top" align="left"><bold>Fitts&#x00027; model</bold></td>
<td valign="top" align="center"><bold><italic>a</italic></bold></td>
<td valign="top" align="center"><bold><italic>b</italic></bold></td>
<td valign="top" align="center"><bold>SSE</bold></td>
<td valign="top" align="center"><bold>RMSE</bold></td>
<td valign="top" align="center"><italic>R</italic><sup>2</sup></td>
</tr>
<tr style="border-top: thin solid #000000;">
<td valign="top" align="left">Small heavy</td>
<td valign="top" align="center">223</td>
<td valign="top" align="center">100</td>
<td valign="top" align="center">776</td>
<td valign="top" align="center">16</td>
<td valign="top" align="center">0.93</td>
</tr>
<tr>
<td valign="top" align="left">Small light</td>
<td valign="top" align="center">201</td>
<td valign="top" align="center">99</td>
<td valign="top" align="center">871</td>
<td valign="top" align="center">17</td>
<td valign="top" align="center">0.92</td>
</tr>
<tr>
<td valign="top" align="left">Big heavy</td>
<td valign="top" align="center">226</td>
<td valign="top" align="center">118</td>
<td valign="top" align="center">1,350</td>
<td valign="top" align="center">21</td>
<td valign="top" align="center">0.93</td>
</tr>
<tr>
<td valign="top" align="left">Big light</td>
<td valign="top" align="center">197</td>
<td valign="top" align="center">117</td>
<td valign="top" align="center">1,841</td>
<td valign="top" align="center">24</td>
<td valign="top" align="center">0.88</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The optimal feedforward model was able to accurately reproduce the motions of the arm during hammering (Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F3">3</xref>, dashed lines, <italic>RMSE</italic> &#x02264; 0.1) using the cost function given by Equation (3). This model allows for the generation of optimal hammering trajectories by selecting just one parameter, &#x003B1;. This model also shows that subjects use roughly the same value of &#x003B1; for each hammer, despite the different properties of the different hammers (Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F3">3</xref>, &#x003B1; values in each row are very similar). The superpositioning of experimental data with computed contours of constant &#x003B1; values (Figure <xref ref-type="fig" rid="F8">8</xref>) showed that in practice subjects do not use a constant value of &#x003B1; for all hammering frequencies, but rather emphasize lower effort at slower hammering frequencies and energy transfer to the nail at faster hammering frequencies.</p>
<fig id="F8" position="float">
<label>Figure 8</label>
<caption><p>Comparison between experimental results and constant contours of &#x003B1;. A map showing the maximal height attained and time to impact generated using constant values of &#x003B1; (Equation 3) was overlayed on experimental results from two different hammers. Solid colored lines (yellow and orange) indicate mean experimental results while dashed lines indicate the standard error. A direct comparison shows that subjects emphasize effort conservation (low values of &#x003B1;) at low hammering frequencies (greater time between impacts) and energy transfer to the nail (high values of &#x003B1;) at high hammering frequencies (less time between impacts) rather than a constant relationship for all hammering speeds. The plots on the right hand side show examples of arm trajectories using different values of &#x003B1;. The specific values used are marked on the left hand plot by a white square, rhombus, and triangle for the top, middle, and bottom plots, respectively.</p></caption>
<graphic xlink:href="fncom-11-00045-g0008.tif"/>
</fig>
<p>The Big Heavy hammer was the most preferred hammer followed by the Big Light, Small Heavy, and Small Light hammers in that order based on subject ratings (Table <xref ref-type="table" rid="T3">3</xref>).</p>
<table-wrap position="float" id="T3">
<label>Table 3</label>
<caption><p>Results of subjects&#x00027; ranking of the hammers, e.g., S-H, Small Heavy; S-L, Small Light; B-H, Big Heavy; and B-L, Big Light.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Ranking vs. Hammer</bold></th>
<th valign="top" align="center"><bold>S-H</bold></th>
<th valign="top" align="center"><bold>S-L</bold></th>
<th valign="top" align="center"><bold>B-H</bold></th>
<th valign="top" align="center"><bold>B-L</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Best (10)</td>
<td valign="top" align="center">0</td>
<td valign="top" align="center">0</td>
<td valign="top" align="center">9</td>
<td valign="top" align="center">1</td>
</tr>
<tr>
<td valign="top" align="left">7</td>
<td valign="top" align="center">3</td>
<td valign="top" align="center">1</td>
<td valign="top" align="center">1</td>
<td valign="top" align="center">5</td>
</tr>
<tr>
<td valign="top" align="left">3</td>
<td valign="top" align="center">3</td>
<td valign="top" align="center">4</td>
<td valign="top" align="center">0</td>
<td valign="top" align="center">3</td>
</tr>
<tr>
<td valign="top" align="left">Worst (1)</td>
<td valign="top" align="center">4</td>
<td valign="top" align="center">5</td>
<td valign="top" align="center">0</td>
<td valign="top" align="center">1</td>
</tr>
<tr style="border-top: thin solid #000000;">
<td valign="top" align="left">Score</td>
<td valign="top" align="center">3.4</td>
<td valign="top" align="center">2.4</td>
<td valign="top" align="center">9.7</td>
<td valign="top" align="center">5.5</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</sec>
<sec sec-type="discussion" id="s4">
<title>Discussion</title>
<p>The goal of this study was to examine the mechanics of a human upper extremity impact task and determine whether existing models of upper limb movement can explain the data. We found that subjects plan optimal trajectories that are a tradeoff between maximum impact velocity and minimal effort reminiscent of Fitts&#x00027; Law and that are robust to different hammer conditions. However, we found that an altered version of Fitts&#x00027; Law was able to better match the data than the typical formulation. We also found that end-effector speeds follow a &#x0201C;bell curve and a half&#x0201D; trajectory in hammering in which the hammer head moves upwards with a bell-shaped speed profile and then downwards with a bell-shaped profile before being truncated before the zenith of the curve (Figure <xref ref-type="fig" rid="F3">3</xref>).</p>
<p>Our analyses showed that Fitts&#x00027; Law can be applied to human hammering (<italic>R</italic><sup>2</sup> &#x02265; 0.88). However, the large <italic>R</italic><sup>2</sup> values belie an apparent discrepancy between the curves generated using Fitts&#x00027; Law and the experimental results (Figure <xref ref-type="fig" rid="F7">7</xref>, gray lines). Therefore, we identified a relationship between movement time and target distance that better reproduces the experimental data (Equation 4, <italic>R</italic><sup>2</sup> &#x02265; 0.99). In most Fitts&#x00027; Law experiments, subjects are prescribed a reaching distance and are asked to move as fast as possible (Fitts, <xref ref-type="bibr" rid="B16">1954</xref>). However, in our experiments, we constrain permitted movement time using the metronome and subjects were allowed to select the distance to reach. This difference may account for the relative effectiveness of our inverted formulation of Fitts&#x00027; Law. However, other previous studies have reported violations of Fitts&#x00027; Law (Adam et al., <xref ref-type="bibr" rid="B1">2006</xref>; Glazebrook et al., <xref ref-type="bibr" rid="B20">2015</xref>). Glazebrook et al. (<xref ref-type="bibr" rid="B20">2015</xref>) determined that these Fitts&#x00027; Law violations are the result of pre-planning of movements. This explanation is also certainly plausible in the context of a cyclical task such as hammering. Finally, several studies have noted that Fitts&#x00027; Law does not hold for movements in which subjects were not asked to move as quickly and as accurately as possible (Young et al., <xref ref-type="bibr" rid="B53">2009</xref>). We do not explicitly instruct our subjects to move as quickly and accurately as possible. Instead, we instructed them to accomplish a task that is directly dependent on the speed of the movement and allow them to balance that movement speed with their motor capability, which we believe to be an approximation of the instructions to move as quickly and as accurately as possible. In hammering frequencies above 1 Hz, the computed values of &#x003B1; indicate that subjects weight movement speed very highly (Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F3">3</xref>), and thus likely approach a fast-as-possible movement for which Fitts&#x00027; Law is presumed to be valid.</p>
<p>Our feedforward optimal hammering simulation was able to reproduce many of the features of human hammering (Figures <xref ref-type="fig" rid="F2">2</xref>, <xref ref-type="fig" rid="F3">3</xref>). Our simulations also allow us to show that humans prefer to emphasize energy transfer to the nail (larger values of &#x003B1;) when task constraints are high (high hammering frequencies) and minimal efforts (smaller values of &#x003B1;) when task constraints are low (low hammering frequencies; Figure <xref ref-type="fig" rid="F8">8</xref>). Our cost function was formulated to minimize the sum squared actuator effort, which serves to keep commanded joint torques small. These small actuation signals prevent excessive energy expenditure during the task (Crowninshield and Brand, <xref ref-type="bibr" rid="B12">1981</xref>; Missenard and Fernandez, <xref ref-type="bibr" rid="B30">2011</xref>), but this quadratic formulation might also serve to keep disturbances from motor noise whose effects are multiplicative with actuator effort small (Harris and Wolpert, <xref ref-type="bibr" rid="B22">1998</xref>; Todorov and Li, <xref ref-type="bibr" rid="B47">2005</xref>; Franklin and Wolpert, <xref ref-type="bibr" rid="B18">2011</xref>). In this context, the adaptive prioritization that we observed (changing values of &#x003B1;) might be due to fewer task constraints permitting higher peak heights to be attained at slow hammering frequencies, thus increasing the potential for errors to accrue and increasing the relative importance of accuracy. While the exact cost function used by the nervous system cannot be known exactly, the current formulation reproduces many of the features observed in the experimental results including maximum heights attained, the general trajectories followed, and the robustness to different hammers (similar values of &#x003B1; for different hammers at the same hammering frequencies). However, this model failed to capture the latency after impact before initiating the upward movement of the hammer. This discrepancy may be due to compliance in the musculoskeletal system (e.g., series-elastic muscle-tendon units, Hill, <xref ref-type="bibr" rid="B24">1938</xref>; Fung, <xref ref-type="bibr" rid="B19">2013</xref>) that was not captured by our model.</p>
<p>Despite different hammer dynamics (Table <xref ref-type="table" rid="T1">1</xref>), hammering kinematics were fairly uniform across many different cases with few statistical differences found between the different hammers in the time from maximal height to impact, maximal hammer height, and impact velocity. Previous studies have suggested that the redundancy of the human musculoskeletal system (Bernstein, <xref ref-type="bibr" rid="B6">1967</xref>) may contribute to considerable robustness to slight changes in dynamics (Martelli et al., <xref ref-type="bibr" rid="B29">2015</xref>; Simpson et al., <xref ref-type="bibr" rid="B42">2015</xref>) or to dysfunction (Arnold et al., <xref ref-type="bibr" rid="B4">2005</xref>; Hicks et al., <xref ref-type="bibr" rid="B23">2008</xref>; Correa et al., <xref ref-type="bibr" rid="B10">2012</xref>; Steele et al., <xref ref-type="bibr" rid="B43">2012</xref>). While these studies rely on highly redundant lower body musculoskeletal models, other studies examining less redundant body parts have shown limited ability to compensate for dysfunction (Valero-Cuevas and Hentz, <xref ref-type="bibr" rid="B49">2002</xref>; Kutch and Valero-Cuevas, <xref ref-type="bibr" rid="B28">2011</xref>). However, detailed models of the upper extremity indicate muscular redundancy on the same level as detailed models of the lower body (Table <xref ref-type="table" rid="T4">4</xref>) suggesting that similar robustness to perturbations might be expected. The human nervous system may also select control strategies that are purposefully robust (Mitrovic et al., <xref ref-type="bibr" rid="B31">2010</xref>; Franklin and Wolpert, <xref ref-type="bibr" rid="B18">2011</xref>), but our formulation does not include any such criteria, suggesting that consistent movement patterns across conditions might be due to embodied intelligence (e.g., redundant actuators and compliance).</p>
<table-wrap position="float" id="T4">
<label>Table 4</label>
<caption><p>Musculoskeletal models used in examinations of robustness.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Body part</bold></th>
<th valign="top" align="center"><bold>Degrees of freedom</bold></th>
<th valign="top" align="center"><bold>Number of muscles</bold></th>
<th valign="top" align="left"><bold>References</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Upper extremity</td>
<td valign="top" align="center">15</td>
<td valign="top" align="center">50</td>
<td valign="top" align="left">Holzbaur et al., <xref ref-type="bibr" rid="B26">2005</xref></td>
</tr>
<tr>
<td valign="top" align="left">Lower body</td>
<td valign="top" align="center">23</td>
<td valign="top" align="center">54&#x0002B;</td>
<td valign="top" align="left">Delp et al., <xref ref-type="bibr" rid="B14">1990</xref>, <xref ref-type="bibr" rid="B13">2007</xref></td>
</tr>
<tr>
<td valign="top" align="left">Index finger</td>
<td valign="top" align="center">4</td>
<td valign="top" align="center">7</td>
<td valign="top" align="left">Kutch and Valero-Cuevas, <xref ref-type="bibr" rid="B28">2011</xref></td>
</tr>
<tr>
<td valign="top" align="left">Simple leg</td>
<td valign="top" align="center">3</td>
<td valign="top" align="center">14</td>
<td valign="top" align="left">Kutch and Valero-Cuevas, <xref ref-type="bibr" rid="B28">2011</xref></td>
</tr>
</tbody>
</table>
</table-wrap>
<p>Stiffness, or impedance, is a crucial parameter modulated by humans to stably interact with their environment (Burdet et al., <xref ref-type="bibr" rid="B9">2001</xref>; Franklin and Wolpert, <xref ref-type="bibr" rid="B18">2011</xref>). Impedance is difficult to record experimentally, but previous studies have attempted to estimate joint stiffnesses based on muscle properties (Hu et al., <xref ref-type="bibr" rid="B27">2011</xref>), through simulation (Thelen et al., <xref ref-type="bibr" rid="B45">2003</xref>), or by experimentally recording endpoint stiffnesses (Burdet et al., <xref ref-type="bibr" rid="B8">2000</xref>, <xref ref-type="bibr" rid="B9">2001</xref>). Because of practical limitations, measurements of muscle activity or impedance were not included in this study, but likely play an important role in impact tasks and should be considered in future works.</p>
<p>Despite the difficulty of controlling a highly nonlinear plant using noisy control signals and noisy sensors with variable delays in an uncertain environment, biological movement appears to be highly robust. However, robustness has not been well addressed in robot learning (Schaal and Atkeson, <xref ref-type="bibr" rid="B39">2010</xref>; Nguyen-Tuong and Peters, <xref ref-type="bibr" rid="B34">2011</xref>) primarily because it is difficult to design controllers that are robust to the model structure or parameter errors. One possible solution is to use control policies with optimization criteria based on biological models. For example, the tradeoff between maximizing task performance and accuracy could potentially serve as an optimization criteria for robot hammering.</p>
<p>In this paper, we have extracted the mechanics involved in a targeted upper extremity impact task and demonstrated that the human motor control strategies involved are robust to many different conditions including hammer mass, hammer face area, and timing constraints. We have shown that while many traditional models of human reaching hold for this novel task (bell-shaped speed profiles and Fitts&#x00027; Law), an altered version of Fitts&#x00027; Law can better match experimental results. We have also demonstrated that optimality principles previously demonstrated for reaching movements can be generalized to targeted impact tasks and thus lay a framework that can be used for the planning of targeted impact tasks in robots.</p>
</sec>
<sec id="s5">
<title>Author contributions</title>
<p>TP, CS, AU, and AI contributed to the design, execution and drafting of this work, and approved the final manuscript. Experimental data was collected and analyzed by TP and CS.</p>
<sec>
<title>Conflict of interest statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</sec>
</body>
<back>
<ack>
<p>The authors thank the members of the Biorobotics laboratory at EPFL for their assistance with data collection and participant recruitment.</p>
</ack>
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<app-group>
<app id="A1">
<title>Appendix</title>
<sec>
<title>Model parameters</title>
<p>In this paper, we have modeled the human arm holding a hammer as a torque driven 3 degree of freedom (DOF) robot operating in the sagittal plane. Each DOF is driven by an independently controlled torque generator capable of producing both positive and negative torques. The robot parameters (link lengths, center of mass locations, etc.) were computed based on data from Winter (<xref ref-type="bibr" rid="B51">2009</xref>) using the mean height (176.9 cm) and weight (77 kg) of subjects that participated in this study. The hammers were simulated by adding the relevant mass to the end effector. Parameters of the hammers are in Table <xref ref-type="table" rid="T1">1</xref>. The robot parameters are given in Table <xref ref-type="table" rid="T5">A1</xref>.</p>
<table-wrap position="float" id="T5">
<label>Table A1</label>
<caption><p>Parametes of the dynamical model.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Part</bold></th>
<th valign="top" align="center"><bold>Upper Arm</bold></th>
<th valign="top" align="center"><bold>Lower Arm</bold></th>
<th valign="top" align="center"><bold>Hand &#x0002B; Hammer</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Link No.</td>
<td valign="top" align="center">1</td>
<td valign="top" align="center">2</td>
<td valign="top" align="center">3</td>
</tr>
<tr style="border-top: thin solid #000000;">
<td valign="top" align="left">Length</td>
<td valign="top" align="center">0.2794</td>
<td valign="top" align="center">0.2667</td>
<td valign="top" align="center">0.0855</td>
</tr>
<tr>
<td valign="top" align="left">Mass</td>
<td valign="top" align="center">2.0751</td>
<td valign="top" align="center">1.2225</td>
<td valign="top" align="center">0.4810</td>
</tr>
<tr>
<td valign="top" align="left">Center of mass location</td>
<td valign="top" align="center">0.1613</td>
<td valign="top" align="center">0.1220</td>
<td valign="top" align="center">0.0676</td>
</tr>
<tr>
<td valign="top" align="left">Inertia</td>
<td valign="top" align="center">0.0131</td>
<td valign="top" align="center">0.0067</td>
<td valign="top" align="center">0.0010</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<p><italic>Note that all units are SI (m, kg). Note also that the center of mass location is relative to the proximal end of the relevant link</italic>.</p>
</table-wrap-foot>
</table-wrap>
</sec>
<sec>
<title>Hammer hits</title>
<p>The table reports how many cycles were necessary to totally drive in the nail with respect to the hammer and frequency.</p>
<table-wrap position="float" id="T6">
<label>Table A2</label>
<caption><p>Number of impacts required to drive nail by hammer and frequency (mean &#x000B1; standard error).</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th/>
<th/>
<th valign="top" align="center" colspan="4" style="border-bottom: thin solid #000000;"><bold>Hammer</bold></th>
</tr>
<tr>
<th/>
<th/>
<th valign="top" align="center"><bold>S-H</bold></th>
<th valign="top" align="center"><bold>S-L</bold></th>
<th valign="top" align="center"><bold>B-H</bold></th>
<th valign="top" align="center"><bold>B-L</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Frequency</td>
<td valign="top" align="center">1</td>
<td valign="top" align="center">12 &#x000B1; 5.114</td>
<td valign="top" align="center">9.9 &#x000B1; 1.215</td>
<td valign="top" align="center">7.1 &#x000B1; 1.663</td>
<td valign="top" align="center">8.5 &#x000B1; 1.258</td>
</tr>
<tr>
<td valign="top" align="left">[Hz]</td>
<td valign="top" align="center">2</td>
<td valign="top" align="center">16 &#x000B1; 3.303</td>
<td valign="top" align="center">12.2 &#x000B1; 1.679</td>
<td valign="top" align="center">9.7 &#x000B1; 2.285</td>
<td valign="top" align="center">13.4 &#x000B1; 2.817</td>
</tr>
<tr>
<td/>
<td valign="top" align="center">3</td>
<td valign="top" align="center">19.7 &#x000B1; 4.6</td>
<td valign="top" align="center">14.4 &#x000B1; 2.579</td>
<td valign="top" align="center">10.6 &#x000B1; 1.655</td>
<td valign="top" align="center">14.4 &#x000B1; 1.968</td>
</tr>
<tr>
<td/>
<td valign="top" align="center">4</td>
<td valign="top" align="center">22 &#x000B1; 3.48</td>
<td valign="top" align="center">19.5 &#x000B1; 2.693</td>
<td valign="top" align="center">12.9 &#x000B1; 2.089</td>
<td valign="top" align="center">14.1 &#x000B1; 2.677</td>
</tr>
<tr>
<td/>
<td valign="top" align="center">5</td>
<td valign="top" align="center">29.2 &#x000B1; 6.2</td>
<td valign="top" align="center">23.8 &#x000B1; 3.62</td>
<td valign="top" align="center">14.2 &#x000B1; 2.732</td>
<td valign="top" align="center">20.2 &#x000B1; 3.511</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
</app>
</app-group>
<fn-group>
<fn fn-type="financial-disclosure">
<p><bold>Funding.</bold> This material is based upon work supported by Sciex-NMSCH project 14.069 to TP and a Fulbright Scholarship, Swiss Government Excellence Scholarship, and National Science Foundation Graduate Research Fellowship to CSS. The research leading to these results has received funding from the Slovenian Research Agency under grant agreement no. J2-7360.</p>
</fn>
</fn-group>
</back>
</article>