Abstract
We combined the theory of neural control of movement with referent coordinates and the uncontrolled manifold hypothesis to investigate multifinger coordination. We tested hypotheses related to stabilization of performance by covarying control variables, translated into apparent stiffness and referent coordinate, at different levels of an assumed hierarchy of control. Subjects produced an accurate combination of total force and total moment of force with the four fingers under visual feedback on both variables and after feedback was partly or completely removed. The “inverse piano” device was used to estimate control variables. We observed strong synergies in the space of hypothetical control variables that stabilized total force and moment of force, as well as weaker synergies stabilizing individual finger forces; whereas the former were attenuated by alteration of visual feedback, the latter were much less affected. In addition, we investigated the organization of “ascending synergies” stabilizing task-level control variables by covaried adjustments of finger-level control variables. We observed intertrial covariation of individual fingers’ referent coordinates that stabilized hand-level referent coordinate, but we observed no such covariation for apparent stiffness. The observations suggest the existence of both descending and ascending synergies in a hierarchical control system. They confirm a trade-off between synergies at different levels of control and corroborate the hypothesis on specialization of different fingers for the control of force and moment. The results provide strong evidence for the importance of central back-coupling loops in ensuring stability of action.
NEW & NOTEWORTHY We expand analysis of action in the space of hypothetical control variables to hierarchically organized multieffector systems. We also introduce the novel concept of ascending synergies, which reflect covariation of control variables to individual effectors (fingers) that stabilize task-specific control variables at a hierarchically higher, task-specific level (hand).
Keywords: force, multifinger coordination, referent coordinate, synergy, uncontrolled manifold hypothesis
INTRODUCTION
Two views have dominated the literature on the problem of motor redundancy, which arises due to the excess of variables at the level of effectors as compared to the number of constraints in typical tasks. According to the classical formulation (Bernstein 1967), motor redundancy is a major problem for the controller, which may be solved, for example, using methods of optimization (reviewed in Prilutsky and Zatsiorsky 2002). The alternative view (Gelfand and Latash 1998; Latash 2012) is that the problem of redundancy is merely apparent and that abundant sets of variables at the effector level allow the neural controller to ensure stability of different performance variables in a task-specific way (Latash 2012; Schöner 1995). This view has been developed within the physical approach to motor control (Latash 2016, 2017) that combines the ideas of the neural control of movement with spatial referent coordinates (RCs; Feldman 2015) and the uncontrolled manifold (UCM) hypothesis (Scholz and Schöner 1999).
According to the notion of action control with specification of time-varying RCs, the control of an effector can be described with time profiles of two basic commands, the reciprocal command (R-command) and the coactivation command (C-command). The C-command reflects overlapping spatial zones of activation of action-relevant agonist and antagonist musculature (Feldman 1980, 2015). Depending on external conditions, changes in the R- and C-commands lead to different measurable changes in performance. In particular, in isometric conditions during force production along a coordinate X, assuming that there is a non-zero degree of agonist-antagonist cocontraction (cf. Ghez and Gordon 1987; Gottlieb et al. 1989), the R-command is a neural entity related to changes in spatial referent coordinate (XR), whereas the C-command is the neural counterpart of the effector’s apparent stiffness (kX). In a linear approximation, the effector is expected to produce force according to Hooke’s law: FX = –kX × (XA − XR), where XA is the current coordinate of the effector. In experiments with smooth changes in XA, XR and kX values can be computed and used to infer the R- and C-commands, assuming that the subject does not change these commands during the change in XA (Ambike et al. 2016a).
In the present study, we explored four-finger pressing tasks that required the production of a magnitude of total force (FTOT). According to the theory of control with RCs, a set {RH; CH} is specified at the hierarchically highest (task) level to match the desired hand total force magnitude (Fig. 1). Note that we use {R; C} to address neural commands and {XR; k} for the related pair of variables computed in experiments. Neural mappings from the task level, given the extrinsic and intrinsic conditions, result in the emergence of each individual finger’s {Rf; Cf} values, which lead to individual finger forces (Ff) that sum up to produce total force, FTOT. For simplicity, the scheme in Fig. 1 skips other levels, such as, for example, propagation of XR to individual muscles; at the muscle level, XR is equivalent to threshold of the stretch reflex (λ) as in the classical equilibrium-point hypothesis (Feldman 1966, 1986). Although the scheme in Fig. 1 is essentially feedforward, it implies the existence of feedback loops, which are inherent in the theory of control with referent coordinates, in particular, those that adjust {Rf; Cf} at the finger level to ensure stable performance with respect to the salient task variable, i.e., FTOT (Latash et al. 2005; Martin et al. 2009).
A number of earlier studies have explored the mapping from the four finger forces to a single variable, FTOT (reviewed in Latash 2008). Several recent studies have estimated {XR; k} pairs measured in individual trials and explored their mapping on FTOT (2-to-1 mapping; Ambike et al. 2016a, 2016b, 2018; Reschechtko and Latash 2017). In both of these examples, numerous solutions at the hierarchically higher level were theoretically available to match the desired mechanical outcome. In the following, we address hypothetical neural mechanisms ensuring stability of the salient performance variable by covaried adjustments within abundant sets of elemental variables, such as finger forces and {XR; k} pairs, as “descending synergies.”
In the present study, for the first time, we address the role of an intermediate step, the specification of {Rf; Cf} at the finger level, in ensuring stability of performance. One aspect of this exploration is another example of a descending synergy, from the eight-dimensional {Rf; Cf} set (pairs of variables for each finger) to FTOT and total moment of force (MTOT) prescribed by the task. This mapping implies two steps: a mapping from {Rf; Cf} to each finger’s force (2-to-1 mapping) and a mapping from the digit forces to FTOT and MTOT (4-to-2 mapping). On the basis of earlier reports of a trade-off between synergies in hierarchical systems (Gorniak et al. 2007, 2009), we hypothesized that there would be strong synergies stabilizing FTOT and MTOT in the eight-dimensional {Rf; Cf} space (hypothesis 1A), but not necessarily those stabilizing individual finger forces in the two-dimensional {Rf; Cf} space, where f stands for the individual fingers, index, middle, ring, and little (hypothesis 1B). In the present paper, we use the term “descending synergy” to signify all few-to-many mappings in which hierarchically higher sets of elemental variables (kinematic, kinetic, or control) covary to stabilize hierarchically lower outputs. This nomenclature is a generalization of previous work on multielement synergies (reviewed in Latash et al. 2007).
We also explored the role of certain fingers in stabilization of total force and total moment by randomizing the {XRf; kf} pairs (cf. Müller and Sternad 2003) for one finger at a time and quantifying the effects of such randomization on FTOT and MTOT variability. Earlier studies in which subjects held and manipulated objects have provided evidence pointing at different functional roles of the “lateral fingers” (index and little) and “medial fingers” (middle and ring): the former were responsible for accurate moment production, whereas the latter ensured accurate production of the grip force (Zatsiorsky et al. 2002, 2003). On the basis of those studies, we hypothesized that FTOT stabilization would be highly sensitive to randomization of the {XRf; kf} pairs for the middle and ring fingers, whereas MTOT stabilization would be more sensitive to randomization of the {XRf; kf} pairs for the index and little fingers (hypothesis 2).
In our studies, synergies were estimated at two states, under continuous visual feedback on FTOT and MTOT and following a drift in performance caused by turning the feedback off (cf. Ambike et al. 2015; Vaillancourt and Russell 2002). On the basis of earlier studies (Parsa et al. 2016; Reschechtko and Latash 2017), we expected all the mentioned synergies to be strong under visual feedback and to weaken or disappear completely without feedback on one or both salient variables (hypothesis 3).
Finally, we explored a qualitatively different kind of synergies, from the eight-dimensional {XRf; kƒ} space to the two-dimensional {XRH; kH} space at a higher hierarchical level (see Fig. 1). Such “ascending synergies” are natural parts of the idea of hierarchical control with RCs; to our knowledge, they have never been explored quantitatively. We tentatively hypothesized that there would be synergies stabilizing {XRH; kH} by covarying across trials adjustments of {XRf; kƒ} and that those synergies would also be weakened under the removal of visual feedback (hypotheses 4A and 4B).
Our study uses two methods of synergy analysis. One of them is a more traditional method (reviewed in Latash et al. 2002) based on quantifying intertrial variance in two spaces, one of which is compatible with accurate performance of a salient variable (within its UCM, VUCM) and the other of which leads to changes in that variable (orthogonal to the UCM, VORT). This method is used when a linear mapping between elemental variables and the performance variable can be assumed. The other method (cf. Müller and Sternad 2003) uses a permutation technique to create surrogate data sets; the permutation is expected to remove covariation among elemental variables. After permutation, indices of performance variability are compared between the actual and surrogate sets. This method is used when mapping between elemental variables and the performance variable is known but expected to be strongly nonlinear.
METHODS
This is the second paper presenting results of a study with four-finger accurate FTOT and MTOT production. Details of the apparatus and procedures are available in the first paper (Reschechtko and Latash 2017). Below we briefly present the main steps of the experimental procedures.
Subjects
Ten adult subjects (5 women; ages 20–35 yr) participated in this study; due to exclusion criteria imposed during analysis (see Analysis), however, data from only nine subjects are analyzed in this article. Subjects were right handed, as assessed via self-reported use for activities of daily living, and reported no injuries or neurological disorders that would interfere with their ability to perform the study procedures. Subjects provided written informed consent according to procedures approved by The Pennsylvania State University Office for Research Protections.
Apparatus
This study used the “inverse piano” apparatus (Martin et al. 2011). This apparatus records finger forces while the fingers can be raised or lowered along the vertical axis. Four unidirectional force transducers (208C01; PCB Piezotronics, Depew, NY) measured force by individual fingers; each transducer was mounted on a linear actuator (PS01-23 × 80; Linmot, Spreitenbach, Switzerland) that allowed the sensor to be raised and lowered. Each force transducer was excited and amplified using an individual signal conditioner (PCB 484B11); analog data from these conditioners were sampled at a rate of 1 kHz at 16-bit resolution using a PCI-6052 analog-to-digital board (National Instruments, Austin, TX). Each linear actuator could be controlled independently using a four-channel servo drive (Linmot E400-AT), which was controlled via serial output from the personal computer used for data collection and feedback presentation.
Each subject sat with her or his right forearm approximately parallel to the ground with the shoulder abducted to ~45° with respect to horizontal and the elbow flexed to ~90°. Subjects placed each finger of the right hand on a corresponding force transducer (17-mm diameter); the transducers were mounted such that the centers of adjacent transducers were 3 cm from each other. Transducer position was adjusted in the anterior-posterior direction such that each finger was slightly curved while the finger pad rested in the middle of the transducer face.
A 19-in. monitor, positioned ~0.8 m from each subject’s face, provided visual feedback on total force produced by the four fingers (FTOT) and the computed moment of force (MTOT; see Procedures for computation). A purpose-built application designed in the LabVIEW programming environment (National Instruments) was used to log data for offline analysis, provide real-time visual feedback, and control the inverse piano. An illustration of the experimental setup is available in our earlier article (Reschechtko and Latash 2017).
Procedure
Data collection for this study consisted of three main components. First, subjects produced a four-finger maximal voluntary contraction (MVC). The MVC value recorded in this part of the procedure was used to set force values for subsequent experimental procedures. During this procedure, subjects received visual feedback on FTOT and were instructed to smoothly increase force to produce maximum force any time during a 6-s time window. Subjects were given one practice trial, followed by a 30-s imposed rest, and were then asked to produce the test MVC trial.
After the MVC trial, subject produced single-finger force ramps. Subjects were required to keep all of their fingers on the force sensors but to press with only one (instructed) finger to follow a 12-s force profile. This profile started with 3 s at 5% of the instructed finger’s contribution to the four-finger MVC (addressed further as this finger’s MVC), followed by a 6-s smooth ramp to 50% of its MVC and then 3 s at 50% MVC. Subjects performed one ramp trial for each finger. Data from the ramp trials were used to quantify finger enslaving (Zatsiorsky et al. 2000), but these data are not presented in the current article.
During the main experimental trials, subjects were instructed to produce a combination of FTOT and MTOT according to visual feedback. Subjects controlled a cursor that could move vertically and horizontally on the screen; vertical movement corresponded to changes in FTOT, whereas horizontal movement tracked changes in MTOT. MTOT was calculated about a horizontal axis in the anterior-posterior direction between the middle and ring fingers according to the nominal moment arms of the fingers: 4.5, 1.5, −1.5, and −4.5 cm for the index, middle, ring, and little fingers, respectively. The effects of tangential forces and changes in points of force application were neglected; as such, MTOT reflected a computed variable rather than the actual total moment of force.
A visual target was shown at the center of the screen; the initial cursor position was computed such that maintaining the cursor position in the target corresponded to specific values of FTOT and MTOT. The FTOT target was set at 20% of the four-finger MVC, whereas the MTOT value was equal to 7% of the index finger’s contribution to the four-finger MVC multiplied by the moment arm of the index finger (4.5 cm) with respect to an axis of rotation passing through the center of the hand in the proximal-distal direction, yielding a value of 31.5% MVCI·cm (where MVCI is the index finger’s contribution to the four-finger MVC). These values were selected on the basis of previous studies (Park et al. 2010; Parsa et al. 2016) such that they would not induce fatigue over multiple trials but had a good chance of inducing drifts in both FTOT and MTOT.
Each trial lasted for 21 s. When the trial began, subjects moved the cursor to the target position and maintained its position within the target. After 5 s, the inverse piano raised all four fingers simultaneously by 1.0 cm at a rate of 2.0 cm/s and then returned the fingers to their initial position at the same speed. Subjects were instructed not to react to this perturbation. Furthermore, they made any necessary corrections to bring the cursor into the target. Two seconds later (8 s after trial onset), visual feedback was manipulated in one of three possible ways: in the no-feedback condition, the cursor disappeared completely (while the target stayed on the screen); in the force-feedback condition, the cursor’s movement was frozen along the horizontal axis such that subjects received information only about FTOT production; and in the moment-feedback condition, the cursor’s movement was frozen along the vertical axis such that subjects received information only about MTOT production. An earlier study by Ambike et al. (2016a) randomized the timing of the application of the perturbation so that subjects could not predict its timing on the basis of the preceding removal of visual feedback. The present study, however, did not use such a randomization protocol because our subjects received full visual feedback when the perturbation was applied, so they could not use feedback removal as a cue for the perturbation onset. Furthermore, we trained the subjects to ignore the effects of perturbations on finger forces, in particular, the effects clearly seen on the feedback monitor. Subjects were also explicitly asked not to try to predict the timing of the perturbations.
Across conditions, subjects were instructed to continue to press as they had previously been pressing and to maintain cursor position in the target according to any visual feedback available. Eleven seconds after feedback had been changed, all four fingers were again raised by 1.0 cm at 2.0 cm/s and returned to their initial position, at which point the trial ended. Subjects performed three to four practice trials until they reported that they were comfortable with the instructions; they performed 24 trials under each feedback condition, for a total of 72 trials. The feedback manipulations were presented in a fully randomized order. Subjects were allowed to take any rest intervals they desired after each trial.
Data Analysis
Data were processed offline using Python 3 (Python Software Foundation) and packages from the SciPy library (Jones et al. 2001). Before analysis, data were low-pass filtered using a forward-and-reverse 4th-order Butterworth filter with a cutoff frequency of 10 Hz. Data were visually inspected for subjects’ failure to adhere to instructions; across subjects and conditions, the largest number of removed trials was three.
Computation of referent coordinates and apparent stiffness.
Hypothetical control variables Rf and Cf (for each finger f) were reflected in pairs {XR; k} computed twice for each experimental trial according to methods used by Ambike et al. (2016a). These {XR; k} pairs, referred to subsequently as initial (ini) and final (fin) values, were computed over 0.5 s between 5 and 5.5 s after trial onset (under visual feedback) and again between 19 and 19.5 s with respect to trial onset. We first verified that the force change occurring while fingers were raised was a linear function of the time-varying finger position. We did this by requiring that the best-fit linear regression of the data explained at least 50% of the observed finger force variance (i.e., R > 0.71). Compared with previous studies (Ambike et al. 2016a, 2016b; Reschechtko and Latash 2017), this threshold is relatively low; this was due to the fact that some fingers produced relatively low force, effectively decreasing the signal-to-noise ratio, as well as the requirement that both episodes of finger raising and lowering within a trial be acceptably linear. Across subjects, this criterion yielded an average of 17.8 usable trials per condition per subject (range: 11–24), and we were forced to remove one subject from analysis due to a low number of usable trials in one condition. Finally, because we used some measures susceptible to outliers, we removed any trials in which any finger’s values of XR or k were more than 3 SD from the mean values. This reduced the number of trials analyzed by an average of 1.2 trials (range: 0–3) per subject per condition. Note that the number of trials analyzed in the present study is equal to or greater than the number used in previous studies using these methods (Ambike et al. 2016a; Reschechtko and Latash 2017).
On ensuring a relatively linear response of Ff to change in finger position, we computed the average value of Ff during the 50 ms before the fingers were raised, as well as the average value of Ff during the final 10 ms of upward sensor motion. We then subtracted the final value from the initial value to obtain ΔFf and divided ΔFf by the change in finger position (1.0 cm), yielding k (apparent stiffness) in units of %MVC/cm. XRf (in cm) was subsequently computed as XRf = −Ff/k. Our choice of coordinate frame (after Ambike et al. 2016a), in which the initial position of the fingers is defined as 0, yields values of XR < 0.
We computed average values of XR and k both before (XRini; kini) and after (XRfin; kfin) feedback manipulation, as well as the ranges of XR and k for each subject in each condition. We also computed the changes in XR and k observed within each accepted trial: ΔXR = XRfin − XRini and Δk = kfin − kini.
Permutation analysis in the {XR; k} space.
FTOT is related to finger forces (Fi) according to the following equation:
(1) |
Furthermore, by setting XA = 0, Ff can be approximated as
(2) |
Combining these two equations, we obtain
(3) |
Because the solution space for this equation is nonlinear, we used the permutation analysis (cf. Müller and Sternad 2003) to generate surrogate data. This analysis estimates the variability of FTOT expected if XR and k vary randomly across trials while being sampled from distributions with the same means and standard deviations as the original values. We generated {XRf; kf} pairs by combining values of XR and k observed in different trials and subsequently computing FSUR and MSUR. We then computed the standard deviations of FSUR and MSUR (SDSUR,F and SDSUR,M, respectively) over 10,000 permutations. Finally, we compared SDSUR,F and SDSUR,M with those for the actual data (SDACT,F and SDACT,M) to obtain a ratio: RSD = SDSUR/SDACT, which was used as a synergy index. Theoretically, RSD > 1 means that the original data set included covariation of {XRf; kf}, which made SDACT lower than expected in a data set without covariation. However, see discussion for further evaluation of an appropriate null hypothesis; given the nature of computation of XR values from k values, RSD > 2 is a more likely criterion, although uncontroversial specification of this criterion is impossible at this time. In the present study, we applied the permutation analysis to various subsets of fingers and individual fingers, as well as to XRf or kf separately.
UCM-based analysis in the finger force space.
Analysis of intertrial variance in the finger force space was performed within the framework of the UCM hypothesis (Scholz and Schöner 1999). To match our methods for permutation analysis, we analyzed FTOT and MTOT data using the UCM method during the 0.5 s immediately preceding the onset of perturbations used for computation of XR and k (initial: 4.5–5 s; final: 18.5–19 s with respect to trial onset). Using this method, we partitioned intertrial variance produced by sets of fingers in two subspaces: the UCM and the subspace orthogonal to it (ORT). As such, variance within the UCM (VUCM) does not affect the performance (e.g., FTOT and/or MTOT) production, whereas variance orthogonal to it (VORT) does affect this performance. The UCM was estimated as the null space of the Jacobian matrix for FTOT (J = [1, 1, 1, 1]) or MTOT (J = [4.5, 1.5, −1.5, −4.5]). For subsets of fingers, the Jacobian included only those entries corresponding to the digits in question. For more detail regarding the computation of VUCM and VORT, see Scholz et al. (2002) and Latash et al. (2001). We quantified the relative amounts of VORT and VUCM by computing the index of synergy, ΔV = (VUCM/VORT)/VTOT, where VUCM, VORT, and VTOT are normalized by their respective dimensionalities depending on the subset of fingers analyzed. Before further statistical analysis, ΔV was z-transformed to produce an index, ΔVZ.
UCM-based analysis in the finger-level {XRƒ; kƒ} space.
We also used the UCM framework to investigate whether control variables at the levels of the individual fingers, {XRf; kf}, covaried to stabilize the hand-level control variables {XRH; kH}. This question can be split into two components: 1) whether the individual fingers’ ki covaried to stabilize hand-level kH, and 2) whether the individual fingers’ XRƒ covaried to stabilize hand-level XRH. Because in a system of parallel springs, the apparent stiffness magnitudes sum up to produce the apparent stiffness of the system, Jk = [1, 1, 1, 1] for the mapping from ki to kH. In contrast, there is no a priori mapping from finger-level XRƒ to hand XRH. As such, we used multiple linear regression to define entries in the JXR matrix:
(4) |
using values of XRH and XRƒ obtained individually for each subject separately for each feedback condition (no feedback, force feedback, and moment feedback) and analysis epoch (initial and final), where subscript I is index finger, M is middle finger, R is ring finger, and L is little finger. The regression equations we obtained accounted for 62% to 99% of variance in XRH (mean: 90%) across subjects, conditions, and epochs of analysis. The regression coefficients af were then combined into the Jacobian, JXR = [aI, aM, aR, aL]. Note that our use of such computational methods to reveal approximate mappings among variables at different levels of analysis does not imply the central nervous system (CNS) uses any computations for the purposes of control.
Statistics
To test the effect of visual feedback on the organization of synergies in eight-dimensional space of finger-level {XRf; kf}, we used one-way repeated-measures ANOVAs with the factor Feedback (3 levels: no feedback, force feedback, moment feedback) on the outcome variable ΔRSD, the change in RSD under altered feedback with respect to its magnitude under full visual feedback. This ANOVA was run on ΔRSD computed for MTOT- and FTOT-stabilizing synergies in {XRf; kf} space separately.
To test whether different fingers were used to stabilize FTOT and MTOT, we compared IL and MR fingers’ RSD with respect to FTOT and MTOT separately, using data pooled across feedback conditions during the full feedback phase (when all trials were identical), using a one-way repeated-measures ANOVA with factor the Fingers Permuted (2 levels: IL, MR).
To test hypothesis 4, regarding so-called ascending synergies, we used the two-way repeated-measures ANOVA with factors Feedback × Phase (2 levels: full feedback, altered feedback) for ΔVZ with respect to XRH-stabilizing XRf and kH-stabilizing kf separately. In addition to the aforementioned tests related to our specific hypotheses, we used a three-way ANOVA with factors Feedback and Phase (as previously described) as well as Finger (4 levels: I, M, R, L) on different outcome variables (force, XR, and k) to explore differences between individual fingers in their reactions to modified feedback.
To test for the presence of synergies in the {XRf; kf} space, we compared RSD values with the critical value of 2 using one-sided, single-sample t-tests. To test for the presence of ascending synergies, we compared ΔVZ values with the critical value of 0.55 using one-sided, single-sample t-tests.
All statistics were run in SAS 9.4 (SAS Institute, Cary, NC). ANOVAs accommodated the repeated-measures nature of the experimental design using mixed models (PROC MIXED), in which subject is treated as a random factor (rather than a classical split-plot repeated-measures design). For this analysis, we assumed a variance components variance-covariance structure. In the case of significant interactions or significant main effects with more than two levels, we used post hoc tests with Bonferroni correction to evaluate which levels were different from one another. F-test degrees of freedom were computed using the Kenward-Roger method (Kenward and Roger 1997), as implemented by SAS 9.4. Unless otherwise stated, numerical data are presented as means ± SE.
RESULTS
General Performance
All 10 subjects were able to satisfactorily complete the full experimental procedure and were included in analysis in our previous paper (Reschechtko and Latash 2017). However, data from only 9 of these 10 analyzed subjects are included in the present paper, because not enough values of {XRf; kf} were recoverable for one of the subjects. With the inclusion of all trials by all subjects, median R2 for the linear regression under visual feedback was 0.94 for the whole hand, 0.94 for the index finger, 0.86 for the middle finger, 0.91 for the ring finger, and 0.98 for the little finger. Across all accepted subjects (n = 9; all trials and conditions), the hand-level FTOT response was within the linearity constraint of R ≥ 0.71 in all conditions during both the first and second perturbations for ~97% of the trials; the changes in force exhibited by the index, middle, and ring fingers were acceptable in ~92–94% of the trials, whereas the little finger showed no appreciable difference from the hand.
Performance Drifts
Although no subjects reported fatigue during the experiment, subjects’ performance did drift for the performance variables, FTOT and/or MTOT, when they did not receive visual feedback on that variable. When FTOT feedback was removed (no-feedback and moment-feedback conditions), the subjects showed a drop in FTOT; when MTOT was removed (no-feedback and force-feedback conditions), they drifted from the original supination value of MTOT to a pronation value. Across-subjects average time series plots of this behavior for FTOT and MTOT, as well as force produced by each finger, are provided in Fig. 2. Analysis of the force changes in individual fingers indicated that the changes in FTOT and MTOT occurred because the ring finger decreased force production in all conditions and the little finger decreased force production in the no-feedback and force-feedback conditions, whereas the index and middle fingers’ force decreased to a smaller extent or even increased. This behavior was especially pronounced in the force-feedback condition: the index and middle fingers increased force, whereas the ring and little fingers decreased force to maintain FTOT.
Figure 3 illustrates the difference in force (ΔF) from the initial to final phase for each finger in each condition. The two-way ANOVA Feedback × Finger on the magnitude of force drift ΔF showed significant main effects of Feedback (F2,88 = 10.76; P < 0.001) and Finger (F3,88 = 21.97; P < 0.0001), as well as a significant interaction (F6,88 = 5.58; P < 0.001). Post hoc tests on Feedback indicated that ΔF values for the force-feedback condition (−0.09 ± 0.21% MVC) and moment-feedback condition (−0.52 ± 0.17% MVC) were not significantly different from each other across fingers, but both were significantly larger than that observed in the no-feedback condition (−1.05 ± 0.22% MVC). Post hoc tests on Finger indicated that ΔF of the index finger was positive (0.37 ± 0.12% MVC), significantly larger than ΔF of the little finger (–0.85 ± 0.22% MVC) and the ring finger (–1.47 ± 0.24% MVC) across feedback conditions. Additionally, ΔF of the middle finger (–0.26 ± 0.22% MVC) was significantly larger than that of the ring finger. The interaction indicated that ΔF of the middle finger and little finger changed depending on the feedback condition: for the middle finger, ΔF in the force-feedback condition was significantly larger than in the no-feedback or moment-feedback condition; for the little finger, ΔF was significantly smaller in the moment-feedback condition than in the no-feedback condition. ΔF was equivalent across conditions for the index and ring fingers.
{XR; k} Synergies Stabilizing FTOT and MTOT
Our previous analysis of FTOT- and MTOT-stabilizing synergies organized at the {XRH; kH} level (Reschechtko and Latash 2017) indicated that when visual feedback on FTOT and MTOT was provided, {XRH; kH} covaried across trials such that both FTOT and MTOT were stabilized. A typical data set for the hand-level {XRH; kH} data is illustrated in Fig. 4, top Note the very high R2 value for the hyperbolic regression under full visual feedback and a drift of the data toward lower k values without visual feedback (no-feedback condition) accompanied by a drop in R2.
Similarly, we found synergies stabilizing FTOT and MTOT in the eight-dimensional space of individual finger {XRf; kf} values (we cannot illustrate the data distribution in the 8-dimensional space in a figure). These synergies are reflected in the large magnitudes of RSD, the ratio of SD of FTOT or MTOT derived from the permuted data set, SDSUR, vs. the SD of the values observed during the experiment, SDACT. Because trials in each feedback condition were identical before visual feedback was manipulated, data for the analysis of synergies in the eight-dimensional {XRƒ; kƒ} space were pooled across feedback conditions to evaluate the presence of FTOT- and MTOT-stabilizing synergies predicted by hypothesis 1A. Under full visual feedback, RSD with regard to FTOT was 12.03 ± 0.78, whereas RSD with regard to MTOT was 11.83 ± 1.03 (i.e., SDSUR was ~12 times larger than SDACT for each task-related variable).
To assess the effect of visual feedback on the organization of FTOT- and MTOT-stabilizing synergies in the eight-dimensional {XRf; kf} space, we used the one-way ANOVA with factor Feedback on the change in RSD (ΔRSD) over the trial duration for MTOT and FTOT separately. For ΔRSD computed for FTOT, the effect of Feedback was significant (F2,16 = 34.50; P < 0.0001), indicating that different feedback alterations affected RSD differently. Note that this result is expected because in the force-feedback condition, subjects continued to receive feedback regarding FTOT. Post hoc comparisons indicated that RSD for FTOT dropped in the no-feedback (ΔRSD = –9.77 ± 1.10) and moment-feedback conditions (ΔRSD = –10.14 ± 1.73), whereas it increased modestly in the force-feedback condition (ΔRSD = 1.46 ± 1.47).
Similarly, the one-way ANOVA on ΔRSD for MTOT showed a significant Feedback main effect (F2,16 = 24.09; P < 0.0001). Post hoc tests indicated that ΔRSD for MTOT in the no-feedback (ΔRSD = –7.67 ± 1.49) and force-feedback conditions (ΔRSD = –11.84 ± 2.03) corresponded to a large drop in RSD, whereas its drop in the moment-feedback condition was much smaller (ΔRSD = –1.54 ± 1.83). Again, values for ΔRSD for MTOT in the no-feedback and force-feedback conditions were not different from one another. Figure 4 illustrates magnitudes of RSD for FTOT (top) and MTOT (bottom) before and after feedback was altered.
{XR; k} Synergies Stabilizing Force of Individual Fingers
Hypothesis 1B predicted that synergies in the two-dimensional space of {XRf; kf} would stabilize individual finger forces Ff. That is, XR and k for individual fingers would covary across trials to stabilize an individual finger’s force production. In contrast to the aforementioned synergies stabilizing FTOT and MTOT, however, note that no explicit feedback on Ff for any finger was provided: subjects received feedback only on FTOT and MTOT.
Figure 5, bottom, illustrates {XR; k} values for the individual fingers of one subject under the no-feedback condition. Note that under full visual feedback, R2 values for individual fingers were lower than for the hand, although still corresponding to statistically significant effects. Across fingers, {XR; k} values displayed better hyperbolic fits (larger R2) under full visual feedback than after feedback manipulation. There was also a shift in the average values of XR and k across trials from the values observed under feedback to those observed at the end of the trial. Typically, this shift involved a consistent drop in k and variable adjustments in XR. Figure 6 shows across-subjects average changes in XRf and kf for individual fingers elicited by the alteration of visual feedback. In the force-feedback condition, the drop in kf was accompanied by a consistent drop in XRf to keep FTOT on the target. In the other two conditions, XR adjustments were highly variable across subjects.
Because trials in each feedback condition were identical before visual feedback was altered, we tested whether synergies in the {XRf; kf} space stabilized individual finger forces by analyzing data pooled across all feedback conditions. We found that XRf and kf for the index and middle fingers stabilized the production of Ff, as indicated by values of RSD > 2, as assessed by individual, single-sided t-tests for each finger. RSD was 3.82 ± 0.41 for the index finger (t26 = 4.48; P < 0.0001), 3.04 ± 0.26 for the middle finger (t26 = 4.05; P = 0.0004), 2.27 ± 0.15 for the ring finger (t26 = 1.75; P = 0.09), and 2.09 ± 0.19 for the little finger (t26 = 0.44; P = 0.66). These values, however, were much smaller than those at the hand level: RSD with respect to FTOT was 12.03 ± 0.78. A one-way ANOVA with factor Finger on RSD showed a significant effect of Finger (F3,96 = 9.30; P < 0.0001). Pairwise contrasts with Bonferroni correction indicated that RSD of the index finger was significantly larger than that of the ring and little fingers; no other pairs of RSD values were significantly different from one another.
Figure 7 shows RSD both before and after visual feedback was altered. We investigated whether removing visual feedback on FTOT or MTOT affected RSD for Ff organized by covariation of {XRf; kf} for individual fingers. For this analysis, we used the three-way ANOVA Finger × Feedback × Phase on RSD. This ANOVA showed main effects for Finger (F3,184 = 17.83; P < 0.0001) and Phase (F1,184 = 20.65; P < 0.0001) without other significant main effects or interactions. The main effect of Feedback shows that, across all fingers and feedback conditions, when feedback was altered (by removing information on FTOT, MTOT, or both), RSD decreased significantly from 2.80 ± 0.14 to 2.09 ± 0.10. Post hoc mean comparisons on the levels of Finger indicated that, across feedback conditions and alterations, RSD for the index finger (3.16 ± 0.24) and middle finger (2.85 ± 0.19) was greater than for the little and ring fingers (1.84 ± 0.11 and 1.93 ± 0.10, respectively). However, the index and middle fingers were not significantly different from one another, and the ring and little fingers were not significantly different from each other either.
Role of Lateral and Medial Fingers in Stabilization of FTOT and MTOT
As indicated by the aforementioned exploratory analysis of RSD for individual fingers, not all fingers displayed equivalent covariation of XRf and kf. A related question is whether different fingers affected FTOT and/or MTOT differently, the subject of hypothesis 2, predicting that FTOT is primarily stabilized by the medial fingers (middle and ring), whereas MTOT is primarily stabilized by the lateral fingers (index and little). To test this hypothesis, we again pooled data across feedback conditions and compared RSD for FTOT and MTOT obtained by permuting the {XR; k} data for the medial and lateral fingers separately under full visual feedback. We then used two separate one-way repeated-measures ANOVA (factor Fingers Permuted) to evaluate whether the lateral and medial fingers stabilized FTOT and/or MTOT differentially.
The ANOVA on MTOT showed that the lateral fingers (RSD = 11.1 ± 1.0) stabilized MTOT significantly more strongly than the medial fingers (RSD = 4.69 ± 0.37; F1,44 = 49.08; P < 0.0001). In contrast, the ANOVA on FTOT showed equivocal results that did not reach the significance criterion (F1,44 = 3.68; P = 0.062), although RSD was, on average, higher for medial fingers (9.79 ± 0.55) than for lateral fingers (8.51 ± 0.55).
Ascending Synergies
The final goal of this analysis was to investigate so-called ascending synergies. This analysis was split into two parts: analysis of covariation of kƒ with respect to kH, and analysis of covariation of XRƒ with respect to XRH. The latter analysis involved a step of identifying the Jacobian matrix using linear regression. R2 values obtained for each multiple linear regression ranged from 0.996 to 0.752 across all 54 computed mappings (9 subjects × 3 feedback conditions × 2 phases); seven values were <0.9, but we observed no obvious relation between R2 values and experimental conditions.
After determining XRf-to-XRH mappings, we used the UCM-based methods to evaluate the presence of kH-stabilizing and XRH-stabilizing synergies separately. To assess whether feedback manipulations affected these ascending synergies, we used a two-way repeated-measures ANOVA, Feedback × Phase, on ΔVZ computed for kH- and XRH-stabilizing synergies separately (Figs. 8 and 9). These analyses showed a significant main effect of Phase (XR stabilizing: F1,40 = 9.17; P = 0.004; k stabilizing: F1,40 = 4.26; P = 0.046) without other significant effects or interactions. This effect indicates that indices of XRH-stabilizing synergies increased significantly from ΔVZ = 0.82 ± 0.09 to ΔVZ = 1.12 ± 0.09 (Fig. 8, top), and kH-stabilizing synergies also increased significantly from ΔVZ = 0.14 ± 0.05 to ΔVZ = 0.26 ± 0.06 (Fig. 9, top). Given the critical value of ΔVZ ≈ 0.55, single-sided t-tests indicated that kH-stabilizing synergies were absent, whereas XRH-stabilizing synergies were present both with (t26 = 3.02; P = 0.003) and without (t26 = 6.37; P < 0.0001) relevant visual feedback.
Changes in ΔVZ can come about because VORT changes without VUCM changing, VUCM changes while VORT does not change, or both change simultaneously. We explored which of these might have occurred by using the two-way ANOVA on VORT or VUCM separately, for indices of variance with respect to both kH and XRH. Values of VORT and VUCM were log-transformed for normality before analysis. For XR-related analysis, VORT was not significantly affected by removal of feedback (F1,40 = 2.66; P = 0.11; Fig. 8, bottom, whereas VUCM significantly increased from 1.51 ± 0.34 to 3.04 ± 0.52 cm2 (F1,40 = 21.12; P < 0.0001; Fig. 8, middle). For kH-related analysis, VORT significantly decreased from 0.34 ± 0.05 (%MVC/cm)2 under visual feedback to 0.14 ± 0.02 (%MVC/cm)2 under altered feedback (F1,40 = 36.03; P < 0.0001; Fig. 9, bottom), whereas VUCM significantly decreased from 0.15 ± 0.03 to 0.08 ± 0.01 (%MVC/cm)2 (F1,40 = 31.54; P < 0.0001; Fig. 9, middle). As such, we conclude that the observed increase in ΔVZ for XRH resulted from an increase in VUCM, whereas the decrease in ΔVZ for kH resulted from simultaneous but disproportional drops in both VORT and VUCM.
DISCUSSION
Our experiment was designed to address a set of hypotheses related to a relatively new theoretical development (Latash 2010, 2017) that combines the main ideas of the uncontrolled manifold (UCM) hypothesis (Scholz and Schöner 1999) and the theory of control with spatial referent coordinates (RCs; Feldman 2015). We tested the hypotheses by quantifying stability of hand action within spaces of control variables, R and C, related to the computed pair of variables {XR; k} of either the hand or individual fingers (cf. Ambike et al. 2016a; Reschechtko and Latash 2017). Our first hypothesis was related to synergies stabilizing the hand force and the individual finger forces in the space of finger-specific {XRƒ; kƒ} pairs. Our earlier study (Reschechtko and Latash 2017) documented strong synergies stabilizing total hand force (FTOT) and moment (MTOT) in the four-dimensional space of finger forces as well as synergies stabilizing FTOT in the two-dimensional space of hand-level {XRH; kH}. The current study documented strong synergies stabilizing hand FTOT and MTOT in the eight-dimensional {XRƒ; kƒ} space in support of hypothesis 1A. Additionally, there were relatively weak synergies in the space of finger-specific {XRf; kf} pairs stabilizing individual fingers’ forces, as predicted by hypothesis 1B.
We also explored finger-level specialization in the {XRf; kf} space to stabilize FTOT and MTOT. We found that the lateral fingers (index and little) contributed much more strongly to the stabilization of MTOT than the medial fingers (middle and ring). The data related to stabilization of FTOT were less conclusive: the medial fingers showed higher contribution to stabilization of FTOT, but their difference from the contribution of the lateral fingers was just below the significance level. Overall, we view these findings as supporting hypothesis 2 and being in agreement with earlier conclusions on the digit specialization with respect to force and moment production (Zatsiorsky et al. 2002, 2003).
Turning off visual feedback on one or both task-specific variables, FTOT and MTOT, led to a rather dramatic drop in the index of stabilization of the variable deprived of the feedback. These findings support hypothesis 3 and earlier reports on changes in the synergic control of variables without visual feedback (Parsa et al. 2016, 2017).
We view as potentially most exciting the results of our analysis of ascending synergies (see Fig. 1), i.e., analysis of stabilization of the hand-level control variables, {XRH; kH}, reflected in intertrial covariation of {XRƒ; kƒ} for the four fingers. Under full visual feedback, we observed strong synergies in the four-dimensional space of XRƒ stabilizing XRH (in support of hypothesis 4A), whereas no synergies in the four-dimensional kƒ space stabilized kH (against hypothesis 4A). When visual feedback was removed, the index of both XRH-stabilizing and kH-stabilizing synergies increased; the latter index, however, remained below the critical level, which indicates that kH is not stabilized (these data speak against hypothesis 4B).
Furthermore, we interpret the results within the general control scheme described in the introduction (Fig. 1). We address a number of issues related to synergic control in hierarchical systems, stability of performance, the role of visual feedback, and possible further directions of exploring the advantages of synergic control at different levels of analysis.
Methodological Aspects of the Reconstruction of XR and k
One potential concern regarding the methods used in this study is that XR and k are reconstructed using a single computational procedure applied to a single data set: k is computed as the ratio of force change to coordinate change: ΔF/ΔX, whereas XR is computed as the ratio of the initial force level to k: –F/k. Because, for the hand force, F should be close to the task force level, there is an intuition that XR and k must automatically (and trivially) covary according to the equation F = –XR · k, leading to a hyperbolic UCM.
An important consideration regarding the covariation of XR and k, particularly in the present study, is the extent to which F is prescribed. Subjects are never able to perfectly produce the task level of hand force, FTASK (or moment); as such, F varies across trials, and the values of XR and k from different trials belong to different hyperbolic UCMs. This variability is relatively small (but never 0) in the presence of visual feedback on the force magnitude, and it becomes substantially larger without visual feedback. Earlier studies used hyperbolic regression to fit {XR; k} data with a best-fit UCM (Ambike et al. 2016a, 2016b). The aforementioned intertrial variability in F is expected to lead to deviations of the data points from this UCM; however, variability of XR and k along (rather than orthogonal to) the best-fit UCM is not constrained by the task. In particular, it could be lower than variability orthogonal to the UCM or even zero. In such a case, the points would deviate from the hyperbolic best-fit UCM primarily in the orthogonal direction with little or no deviations along the UCM. The randomization method would lead in such a situation to RSD < 1, which never happened in our experiment. Therefore, our results show that the data varied along the UCM more than orthogonally to the UCM, which is a consequence of subjects’ behavior, not a trivial outcome of the computation.
In the present study, we also present analysis with respect to variables that received no visual feedback at all, such as the individual finger forces. For these variables, intertrial variability of force values was substantial, leading to relatively large deviations from the best-fit UCM. Despite the higher variability of Ff than FTOT, however, we still observed values of RSD indicating XR and k for individual fingers covaried in a way that left individual finger forces relatively unchanged. Note also that we observed different behaviors of XR and k across feedback conditions (consistent changes in k that were not matched by consistent changes in XR; see Fig. 6), which may not be expected if our results were trivial outcomes of the computational procedure.
There is another important issue regarding the present methodology, related to the fact that some of the variables used in the analysis were measured relatively independently (such as force F and its change due to sensor motion, resulting in apparent stiffness k), whereas the second variable at the assumed control level (XR) was computed from the first two. This procedure, by itself, could lead to covariation among pairs of variables, in particular between XR and k, as a result of algebra of random variables. This problem is inherent to many studies that analyze covariation in spaces of elemental variables that are not measured independently but computed on the basis of other, directly measured, variables. For example, analysis of covariation in joint configuration spaces typically uses individual joint rotations as elemental variables (e.g., Scholz and Schöner 1999; Scholz et al. 2000). These rotations, however, are not measured but computed from the measured values of marker coordinates. Similar problems emerge with analysis within spaces of activation of muscle groups (M-modes; Krishnamoorthy et al. 2003).
Estimating potential effects of such computations on expected magnitudes of covariation is nontrivial because of a number of factors. First, the precise expectations arising from such operations are dependent on the actual distributions of the measured variables, which are difficult to evaluate in our studies given the relatively small number of trials collected. The situation is also complicated by the fact that the two variables, force and apparent stiffness, which can be viewed as measured more or less independently, are expressed in incommensurate units and are not normally distributed (in particular, they are both nonnegative). The latter issue may be seen as relatively minor because the actual values are far from zero, and so the distributions of F and k may be viewed as approaching normality. To deal with the former issue, we analyzed expected covariation patterns after expressing the two variables in normalized units such that the mean of each equals unity.
Figure 10 illustrates this issue in more detail via simulations in sets of 1,000 samples of F and k that were drawn from independent normal distributions and used to compute XR values for three different distributions of k, assuming a normal distribution of F with the mean μF ≈ 1.0 and standard deviations σF ≈ 0.1 (chosen to approximate experimental data under visual feedback). The mean for k was always assumed μk ≈ 1.0, whereas its standard deviation varied among the illustrated simulations. In Fig. 10A, σF = σk; intuitively, this corresponds to the null hypothesis, assuming that variation of elemental variables was comparable to that of the performance variables. Note that the RSD value computed from these data is ≈1.8, rather than 1.0, as it has been assumed in previous studies. In Fig. 10B, σF > σk; in this case, RSD indeed approaches 1.0. Finally, in Fig. 10C, σF < σk, which we interpret as a synergy in the {XR; k} space stabilizing the performance variable F. In this case, RSD is ~22 (>>1.0) as expected.
The applicability of this particular simulation with its large number of samples and known distributions to the experimental data is still admittedly tenuous. One of the main results of these simulations is revision of the idea that our null hypothesis corresponds to RSD = 1.0, and subsequent reinterpretation of certain previous results. In particular, in an earlier study, we observed RSD values ~2.0 after force drifts in the absence of visual feedback (Reschechtko and Latash 2017). We interpreted those results as reflecting a weak synergy stabilizing F, whereas in fact, the synergy could be absent. In future work, we intend to develop a metric directly comparing the relatively independently recorded measures F and k, rather than invoking the computed measure XR and associated methodological problems.
It must be admitted that, given the aforementioned issues (including incommensurate units and unknown data distributions), there is no way to prove that a given criterion value of RSD is the applicable threshold in a given experiment. Such problems are, however, by no means unique to the present methodology or application: all studies comparing the variances of computed elemental variables (including joint angles in radians recovered from best-fit kinematic marker paths and muscle modes in mV recovered from processed and dimension-reduced electromyographic recordings) with variances of performance variables expressed in different units (e.g., end-point coordinate in m and center of pressure coordinate in m, respectively) suffer from the same shortcomings, and we attempt to be as transparent as possible about these shortcomings.
Is Redundancy a Problem?
Our approach to the problem of motor redundancy (Bernstein 1967) is based on the principle of abundance (Gelfand and Latash 1998; Latash 2012). According to this principle, the excess of elemental variables (those produced by elements at a selected level of analysis) is not a computational problem for the CNS (e.g., solved using optimization approaches; Prilutsky and Zatsiorsky 2002; Seif-Naraghi and Winters 1990), but a high-dimensional space where lower dimensional subspaces can be stabilized corresponding to the production of stable magnitudes of salient performance variables. This can be done, for example, by using feedback loops from peripheral receptors or central back-coupling loops, as suggested in earlier studies (Latash et al. 2005; Martin et al. 2009). Stabilization of such subspaces allows the controller to ensure natural stability of action based on laws of nature (Latash 2016), as well as offering the ability to perform secondary tasks without interference with the primary one (e.g., Zhang et al. 2008) and to adjust stability of a performance variable in a task-specific way (e.g., in preparation to a quick change in that variable; Olafsdottir et al. 2005).
Until recently, studies of action stability within the UCM hypothesis framework have been limited to analysis of higher dimensional space of performance variables produced by elements, e.g., finger forces, joint rotations, and muscle activations (reviewed in Latash 2008). Merging this framework with the idea of control with spatial referent coordinates (reviewed in Feldman 2015) offers an exciting opportunity to explore the synergic control of performance at the level of hypothetical control variables (Ambike et al. 2016a). This method has so far been applied to studies of single-effector actions, either an individual finger (Ambike et al. 2016a, 2016b) or the hand as a whole (Reschechtko and Latash 2017), controlled with two basic commands, R and C, that translate into changes in the effector XR and k. Our present study is the first to apply this method to a multieffector task where each of the effectors is controlled with the corresponding {R; C} pair. Our results show that, within the eight-dimensional {XRf; kf} space, two one-dimensional subspaces, corresponding to the desired magnitudes of the performance variables FTOT and MTOT, were strongly stabilized. Although subjects could have involved more proximal muscles during the task performance, the isometric conditions and intermediate posture of the fingers used in the present study did not allow passive transmission of forces not mediated by activation of finger muscles. That is why we only analyze the behaviors presented in this article at the finger and hand level.
We do not propose that a given {XR; k} pair is precomputed at some level of the CNS, but rather that it emerges as a result of selecting values of the R- and C-commands to match the task requirements. The R- and C-commands may be viewed as tools available to humans to perform various tasks; specific patterns of these tools are used, based on experience and available sensory feedback. A given {XRf; kf} pair at the finger level may lead to different combinations of joint-level r- and c-commands in different trials, realized via various combinations of stretch reflex thresholds (λ) of involved muscles. As such, individual joint and muscle actions are not unique even if they originate from the same combination of the R- and C-commands, another facet of the notion of “repetition without repetition” introduced by Bernstein (1967). Joint- and muscle-level control variables emerge and show patterns of covariation, which ensure that the individual effector actions are combined to be compatible with the performance dictated by the {R; C} pair. Neurophysiological mechanisms involved in these transformations are unknown, and in this article we try to develop concepts, such as central back-coupling and ascending synergies, which, at this time, seem promising to address issues of the neural control of performance stability.
We view the relatively large variability of the elemental variables within subspaces corresponding to stable magnitudes of salient performance variables as a consequence of selective stability in different directions of the original multidimensional space. The unavoidable variability of the intrinsic states of the body, and of its interaction with the environment, serves as a source of perturbations for the elemental variables that respond naturally by larger deviations in directions of low stability. The indices of stability such as, for example, indices of the structure of intertrial variance (Scholz et al. 2002), motor equivalence (Mattos et al. 2011), and the RSD index used in the current study do not reflect computations by the controller (e.g., as in optimal feedback control schemes; Diedrichsen et al. 2010; Todorov and Jordan 2002) but natural processes within the system characterized by different stability in different directions.
Stability of Processes in a Hierarchical System
Stability of variables within a hierarchical system is a nontrivial issue. Stabilization of total force produced by the four fingers implies the existence of a three-dimensional subspace within the original four-dimensional finger force space where processes are less stable and show relatively large variance. The large variance in that subspace means that variance in the behavior of individual effectors is also large. Can the outputs of individual effectors be stabilized at a different level of the hierarchy, e.g., within their {XRf; kf} spaces, given their large variance? An earlier series of studies (Gorniak et al. 2007, 2009) showed that in pressing and prehensile tasks, some mechanical variables were stabilized only at the task-specific level of analysis, whereas other variables were stabilized at both task-specific level and a lower level combining a subset of digits (so-called “virtual finger”; Arbib et al. 1985). These findings led to the conclusion that stabilization at more than one level of a hierarchy may indicate the controller’s prioritization of different performance variables.
In our study, we observed relatively high indices of synergies quantified at the {XRf; kf} level with respect to task-specific performance variables FTOT and MTOT (RSD > 10). These indices for the forces produced by individual fingers (Ff) were much lower (1.5 < RSD < 4.0). However, all these indices were significantly higher than unity, which may correspond to synergies stabilizing resultant force and moment as well as individual fingers' forces—however, it is unclear whether this criterion is appropriate (see discussion for indication that 2 may be more appropriate). These results are notable as another sign of a trade-off between synergies at different levels of a control hierarchy. They also indicate that the controller cared not only about performing the explicit task accurately but also about stabilizing values of individual finger forces, possibly to keep them within a range perceived as natural or in some sense optimal.
Earlier studies of prehension tasks have suggested that fingers play different roles with respect to resultant mechanical variables applied to the grasped object. In particular, the middle and ring finger forces were highly sensitive to manipulations of the external load (while the external torque was kept constant), whereas the index and little finger forces showed high sensitivity to manipulations of the external torque rather than external load (Gao et al. 2006; Zatsiorsky et al. 2002). We explored this hypothesis at the level of pairs of control variables to individual fingers. This was done by removing possible stabilizing effects of finger subsets with the help of permutation of their {XRf; kf} pairs. Permutation of {XRf; kf} to the lateral fingers (index and little) led to strong effects on accuracy of MTOT performance, much stronger than permutation of the {XRf; kf} to the medial fingers (middle and ring). The effect on FTOT was opposite: stronger effect was observed as a result of permutation of the {XRf; kf} to the medial fingers, but the difference between the finger pairs was under the level of statistical significance. Overall, our observations corroborate the original hypothesis by Zatsiorsky and colleagues on specialization of finger pairs in prehensile tasks.
Natural Processes Leading to Performance Drifts
Unintentional drifts in human performance have been reported in multiple contexts, including slow force drifts during force-production tasks (typically to lower magnitudes; Slifkin et al. 2000; Vaillancourt and Russell 2002), faster force drifts in trials with external perturbations (Wilhelm et al. 2013; Zhou et al. 2014), and drifts in other performance variables that may occur over a long series of trials (Heijnen et al. 2012, 2014). In our study, we explored drifts in force and moment after removal of salient visual feedback. These phenomena have commonly been explained in terms of shortcomings in working memory (Vaillancourt and Russell 2002), supported by clinical studies (Prodoehl et al. 2007) and brain imaging studies (Coombes et al. 2011; Poon et al. 2012). There is also evidence, however, that such drifts do not come about because subjects “forget” the required level of force production. For example, when a subject is asked to interrupt a force production trial, relax, and then return to the required force, no force drop is observed (Jo et al. 2016; Solnik et al. 2017). Additionally, when force production by one hand drifts, subjects tend to match the original force level if asked to match the force production with their contralateral hand (Reschechtko et al. 2018).
Within the context of neural control of movement with RCs, explanations of force drift have been proposed suggesting that this phenomenon results from a natural drift of XR toward the actual effector coordinate. This natural process reflects the tendency of all physical systems to move toward minimum of potential energy but remains compatible with the aforementioned explanations because it takes place at a different level of explanation and has received support in a number of recent studies. In particular, earlier studies have documented drifts in both XR and k during the unintentional force drift (Ambike et al. 2016b; Reschechtko and Latash 2017). Similarly, we observed such drifts in the {XR; k} pairs at the level of the hand and individual fingers (see Fig. 5). However, it is notable in the present experiment (and in Reschechtko and Latash 2017) that we saw a consistent drift in k across conditions with and without visual feedback. When visual feedback on FTOT was present, XR adjustments allowed keeping the FTOT at the required level; without visual feedback on FTOT, this variable showed a drift. The consistent decreases in k may reflect both the high energetic requirements of the C-command (increased agonist-antagonist muscle coactivation), as well as the ecological rarity of tasks that require sustained coactivation: modulation of the C-command is more often observed transiently during fast movements, and it subsides during steady states (as exemplified in the classic triphasic electromyographic patterns observed during single-joint movements; reviewed in Gottlieb et al. 1989).
Role of Different Feedback Modalities in Modulation of Stability
In an isometric force production task, the feedback modalities that can stabilize variables including FTOT and MTOT are relatively limited. It is unsurprising, therefore, that visual feedback is particularly important for allowing the CNS to stabilize force or moment of force in isometric conditions. A less trivial finding in our previous study was that {XRH; kH} synergies at the hand level were strongly attenuated by the removal of visual feedback but that they did not completely disappear: RSD was never observed to drop below the critical value of 1. This indicated that even during the force drift without visual feedback, intertrial variability in XRH and kH was still structured to stabilize FTOT, which could result from aforementioned central back-coupling processes (Latash et al. 2005) or other feedback modalities, including somatosensation in the fingertips and proprioceptors in the involved muscles. The fact that the subjects were unaware of the force and moment drifts despite their large magnitudes, however, casts doubt on the latter hypothesis.
In our present study, we again observed the strong attenuation of synergies in the {XRƒ; kƒ} space stabilizing FTOT and MTOT during unintentional drifts in these variables. These results confirm previous findings (Ambike et al. 2016b; Parsa et al. 2016; Reschechtko and Latash 2017), but our present findings also extend to processes involving multiple effectors. In particular, we found relatively weak synergies in the {XRf; kf} space stabilizing individual finger forces, which again were attenuated but not extinguished by feedback alteration. This finding is somewhat surprising given that feedback on individual finger forces was never provided, so any organization of {XRf; kf} synergies took place without visual feedback, and it is not clear why feedback alteration should further affect these synergies. Nevertheless, existence of such synergies at the individual finger level suggests that processes governing the {XRH; kH}-to-{XRf; kf} transformation are somewhat stable, possibly to stabilize certain solutions in the {XRf; kf} space, which may serve various functions, including the stabilization of digit posture or maintenance of some baseline level of cocontraction.
The observed drifts in performance were associated with consistent drifts of k toward lower magnitudes, whereas XR adjustments depended on available feedback. This observation suggests lower stability of processes associated with specifying k compared with those associated with specifying XR, a finding that may be partially resultant from the study of isometric action rather than free motion, and one that we address further below.
Ascending Synergies
A primary goal of this paper is to introduce the notion of ascending synergies and make an (admittedly naive) effort to quantify them. We use the term “ascending” to highlight the idea that a high-dimensional space at certain intermediate levels of a hierarchy may be organized to stabilize its input rather than its output, an assumed aspect of control with RCs. This statement may appear to violate the causal relations within the system illustrated in Fig. 1, but this is only a seeming violation. The XRH and kH inputs into the lower level may be seen as structuring the eight-dimensional space of finger level {XRƒ; kƒ} pairs in a way compatible with stabilization of both XRH and kH, naturally leading to the stabilization of total hand force FTOT, which is a direct function of XRH and kH.
We split the problem of {XRH; kH} stabilization into two problems because the problem of kH stabilization in the four-dimensional {kƒ} subspace is linear and independent of variations in XRƒ. We emphasize, however, that our choice in splitting the problem is done for computational purposes and is in no way an endorsement of the idea that the CNS actually splits the problem or performs such computations. Although we do not know how such synergies are organized, some kind of central back-coupling could be used for this purpose (Latash et al. 2005).
To our surprise, we did not find kH-stabilizing synergies even when full visual feedback was available. Moreover, the synergy index ΔVZ was consistently much lower than the critical value, suggesting that individual finger kƒ values covaried positively across trials. This could be due to the organization of extrinsic finger flexors, which are multitendon muscles serving all four fingers. As a result, natural intertrial variations in muscle activation could lead to parallel changes in the apparent stiffness of the individual fingers, resulting in the very low ΔVZ values.
Analysis of the XRH-stabilizing synergies led to a very different outcome. Despite the fact that our linear model was merely based on multiple regression, strong synergies were observed in the {XRƒ} space stabilizing XRH. This result supports a hypothesis suggested earlier by Feldman (2015) that the R-command (which is linked to XR in our study) plays a primary role in the control of actions, whereas the C-command (which is linked to k) is subordinate to the R-command.
Without visual feedback, the index of the synergy stabilizing XRH increased, in contrast to other synergies described in the study. This was primarily due to a less stereotypical set of solutions in the {XRƒ} space, as reflected by the significant increase in the VUCM component of variance, without a major change in the other component, VORT. Although a similar trend was seen in the index of synergy stabilizing kH, this resulted from disproportionate decreases in both VUCM and VORT, indicating that kf changes became more stereotypical. Furthermore, the increase in ΔVZ was insufficient to constitute a synergy stabilizing kH. These results show the particular sensitivity of mechanisms related to XR production to feedback manipulations, whereas mechanisms related to k production remain relatively immune. Because the present study investigates only performance variables, and not configuration of the hand, limbs, and/or body (as may be expected in studies with free motion), the values of and changes in XR and k may also differ from those that would be observed during tasks requiring such movement.
Concluding Comments
In the present study, we have made an attempt to quantify ascending synergies, which result from the mapping of a low-dimensional task control variables on a high-dimensional space of redundant control variables to individual effectors. We also admit to shortcomings in our current methodology. For example, the range of feedback alterations and tasks performed was quite limited, albeit due to the amount of time subjects could focus on the task without fatigue. The lack of physiological measurement (e.g., surface electromyography) also limits our ability to interpret our results in terms of muscle activations; this is undoubtedly an important level of analysis, and one that we hope to use in future studies. Furthermore, the method we used to link finger- and hand-level XR values is admittedly crude, and we are open to the possibility that it may prove to be a suboptimal practice as the exploration of ascending synergies commences. Finally, the index used in this and previous studies to compare variability of the performance and control variables, RSD, suffers from computational problems related to algebra of random variables. Although similar computational assumptions are commonplace in the literature, we plan to avoid such methodological problems in future work by comparing variables that are measured independently when such measurements are possible, and we believe that the methodologies employed in this study display no unique shortcomings.
GRANTS
This work was supported by National Institute of Neurological Disorder and Stroke Grant R21-NS95873 (to M. L. Latash).
DISCLOSURES
No conflicts of interest, financial or otherwise, are declared by the authors.
AUTHOR CONTRIBUTIONS
S.R. and M.L.L. conceived and designed research; S.R. performed experiments; S.R. and M.L.L. analyzed data; S.R. and M.L.L. interpreted results of experiments; S.R. and M.L.L. prepared figures; S.R. and M.L.L. drafted manuscript; S.R. and M.L.L. edited and revised manuscript; S.R. and M.L.L. approved final version of manuscript.
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