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Learning Intermittent Strategy

        Continuous Type              One-sided Intermittent Type Two-sided Intermittent Type
         Subject 4 Trial 14
                                     Subject 2 Trial 27                                                      Subject 9 Trial 29
100
                               100 100

10−2                           10−2                                                                    10−2
PSD [rad2/Hz]
10−4                                        PSD [rad2/Hz]10−4                                          10−4
                                                                                        PSD [rad2/Hz]

10−6                           10−6                                                                    10−6

         SlopLow:−0.42838            SlopLow:−0.93                                                           SlopLow:−1.0604

         SlopHigh:−6.1971            SlopHigh:−6.1963                                                        SlopHigh:−5.8397

10−8                           10−8                    15                                              10−8
   0.01  0.1               15  0.01 0.1                                                                0.01 0.1                15

         Freq [Hz]                   Freq [Hz]                                                                  Freq [Hz]

Figure 9. Power spectral density (PSD) functions of sway dynamics (h) of the pendulum during successful trials. A: Trial 14 of Subject 4
(continuous type). B: Trial 27 of Subject 2 (one-sided intermittent type). C: Trial 29 of Subject 9 (two-sided intermittent type).
doi:10.1371/journal.pone.0062956.g009

saddle point exhibited by the inverted pendulum with no active                                         continuous type did not exhibit slow oscillations, but included high
control. See Table 3 for statistics.                                                                   frequency components.

3.5 Power spectral analysis and energy efficiency                                                         Notice that the average of total power for the continuous type
   Power spectral density (PSD) was estimated for every successful                                     was significantly smaller than that of those for the intermittent
                                                                                                       types, reflecting the fact that the amplitude of slow oscillation in
trial. Slopes (scaling factors) at the low and the high frequency                                      the continuous type was smaller than those in the intermittent
bands (LF and HF) of the log-log plotted PSD were calculated to                                        types.
characterize the double power-law behavior in sway of the virtual
pendulum. Figs. 9A, B and C show PSDs of the representative                                               We estimated mechanical energies (powers) consumed by the
subjects of three types.                                                                               active torques during F5 and the successful trials (Table 4). For F5
                                                                                                       trials, mean powers for the two-sided intermittent, one-sided
   Table 4 summarizes average slopes at LF and HF bands that                                           intermittent and continuous types were 1:3 W, 1:69 W and 2:81
were examined separately over the subjects of each type. The
average values of slope at LF band for the subjects of two-sided                                         Table 4. Slopes of PSD at LF and HF bands for successful
intermittent, one-sided intermittent and continuous types were                                           trials and power consumption [W] for F5 and successful trials
20.99, 21.31 and 20.41, respectively. The slopes for two and                                             for each subject and for average of each type.
one-sided intermittent types were significantly steeper than that for
the continuous type (pv0:05). The absolute values of slope at LF                                                LF HF Power (F5) Power (Succ)
band in the intermittent types were close to the corresponding
scaling exponent of b~1:5 (H~0:25) reported by Collins and De                                          S1       20.9660.45         25.8460.32 1.0860.12  0.3660.13*
Luca [52] in their two-point correlation functions and by Asai et al                                   S9                                                0.6160.21
[32] in their simulation of the intermittent control model.                                            two-int  21.0360.16         26.0560.33 1.5360.16  0.4760.13[c]
                                                                                                       S2                                                0.2760.11
   The average values of slope at HF band in the two-sided                                             S3       20.9960.19{c} 25.9260.19 1.3060.11       0.2760.37*
intermittent, one-sided intermittent and continuous types were                                         S5                                                0.2360.57
25.92, 25.99 and 25.63, respectively. There were no significant                                        S8       21.1160.70         26.1760.10 0.7760.08  0.1360.96
differences in the slope of the HF band between any two types.                                         one-int                                           0.2260.31[c]
The absolute values of slope at HF band in all of three types were                                     S4       21.2360.23         26.5160.64 2.2560.29  1.5460.22
about two times larger than the scaling exponent of b~2:6                                              S7                                                0.8460.55
(H~0:8) reported by Collins and De Luca [52]. However, the                                             S11      21.3560.27         25.5160.32 1.3160.51  1.1660.35*
value of about 6.0 was in agreement with the corresponding                                             cont                                              1.2860.20[t][o]
exponent reported by Asai et al [32] and Nomura et al [53] in                                                   21.5460.48         25.9460.45 2.4460.74
their simulation of the intermittent control model.
                                                                                                                21.3160.14{c} 25.9960.14 1.6960.25
   The steep slopes at LF band for the subjects of one and two-
sided intermittent types implied that the long-term-correlated                                                  20.2060.37         25.8060.39 2.6460.28
fluctuations were included in the sway motion of the pendulum
controlled by the subjects adopted the intermittent control. This                                               20.9060.52         25.3560.72 2.8560.49
was consistent with the fact that sway of h in the subjects of those
two types showed slow oscillations, whereas that in the subjects of                                             20.1660.99         25.6760.57 2.9660.27

                                                                                                                20.4160.13{t}{o} 25.6360.13 2.8160.20

                                                                                                       Symbols of à indicate significant difference between F5 and successful trials
                                                                                                       (pv0:01). Brackets [ ] and {} represent the significance levels of difference in the
                                                                                                       mean values of each index among three types of strategies for successful trials,
                                                                                                       respectively with pv0:01 and pv0:05. See caption of Table 3.
                                                                                                       doi:10.1371/journal.pone.0062956.t004

PLOS ONE | www.plosone.org                                             15 May 2013 | Volume 8 | Issue 5 | e62956
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