1. Introduction
Voluntary movement is not a simple consequence of muscle activation but the result of a carefully orchestrated process of planning, timing, and execution that involves multiple cortical and subcortical structures. A hallmark of this preparatory process is the readiness potential (RP), a slow, negative shift in the electroencephalogram that emerges up to two seconds before the onset of voluntary action [
1]. The RP was first characterized through experiments showing that this potential could be observed even in self-paced movements without external cues, thus reflecting an internally generated intention to act. Later, Libet, Gleason [
2] extended these findings by demonstrating that the RP precedes the subjective awareness of the intention to move by several hundred milliseconds, a result that has since been pivotal in debates about free will and the temporal hierarchy of motor intention.
Over time, the RP has become a fundamental tool for probing motor preparation, particularly because its amplitude and temporal profile provide insight into the recruitment and organization of motor-related cortical areas. Functional and intracerebral studies have shown that RP generation involves the primary sensorimotor cortex, supplementary motor area (SMA), pre-SMA, and anterior cingulate cortex [
3]. These areas coordinate the transition from a preparatory state to the initiation of movement, with the RP reflecting the gradual buildup of neuronal activity required to surpass the threshold for motor execution. Importantly, RP dynamics are shaped by the characteristics of the intended action its complexity, duration, and energetic requirements [
4,
5].
Task complexity has long been known to influence motor preparation. Early work by Wohlert [
4] demonstrated that oral movements of greater complexity elicited larger RP amplitudes at central sites, indicating that the RP encodes not just the decision to move but also the computational demands of motor programming. Studies in hand and limb movements have similarly reported that sequences requiring precise coordination or multiple effectors lead to increased RP amplitudes and earlier onset latencies [
6]. This relationship between complexity and RP amplitude aligns with the notion that more elaborate motor plans necessitate greater recruitment of premotor and supplementary cortical resources.
Another critical factor influencing RP dynamics is movement duration. Research has shown that prolonged movements are associated with longer reaction times, extended premotor periods, and altered RP profiles[
7,
8]. Xu, Sommer [
9] and Bortoletto and Cunnington [
10] have provided evidence that timing and sequencing contribute differently to RP components, with timing affecting the early buildup phase and sequencing influencing later components. These findings underscore the temporal sensitivity of the RP and suggest that it serves as a dynamic index of how the nervous system allocates preparatory resources over time.
Despite these advances, the interaction between temporal constraints and mechanical effort in shaping the RP remains poorly understood. Mechanical load, an intrinsic parameter of motor tasks, is known to influence both performance and neural activity. Deschamps, Murian [
11] observed that increased mechanical constraints can degrade pointing accuracy but do not necessarily reduce mental effort, implying that cortical preparatory activity may scale with mechanical demand even when behavioral outcomes deteriorate. Similarly, Kennefick, Burma [
12] demonstrated that motoneuronal excitability increases with rising task complexity during preparation phases, further supporting the notion that motor effort is encoded upstream of execution.
An additional layer of complexity emerges from findings on neural variability during motor preparation. Churchland, Yu [
13] showed that trial-to-trial variability in premotor cortex decreases as movement onset approaches, a phenomenon interpreted as the stabilization of motor plans. This reduction in variability correlates with shorter reaction times and improved movement precision, suggesting that preparatory neural states are optimized when temporal and mechanical demands are clearly defined. However, how RP amplitude evolves under the simultaneous influence of mechanical load and movement duration has not been systematically explored.
Beyond basic motor neuroscience, the RP has gained relevance in translational cotexts, especially in the development of brain-computer interfaces (BCIs) aimed at motor rehabilitation. Because RP features (such as amplitude, onset latency, and lateralization) can predict motor intention before movement onset, they have been successfully implemented in exoskeleton control, adaptive neuroprostheses, and functional electrical stimulation systems [
14,
15]. Notably, asynchronous BCIs that do not rely on external cues but instead detect spontaneous RP fluctuations have been shown to enhance ecological validity and adaptability [
16]. Understanding how RP properties vary with both temporal constraints and mechanical effort could therefore inform the development of BCIs that are more precise and responsive to the natural variability of human motor behavior.
In our previous work, we demonstrated that RP amplitude scales linearly with movement duration, providing evidence that preparatory activity is finely tuned to temporal demands [
17]. This finding suggests that the RP can serve as a sensitive index of how cortical networks allocate resources when actions require precise timing. Building on this foundation, the present study investigates whether progressive mechanical load further modulates RP amplitude and spectral characteristics. Specifically, we examine whether incremental weights, applied in three levels, produce a load-dependent amplification of the RP and how this effect interacts with the duration of the executed movement.
By combining electroencephalography (EEG), electromyography (EMG), and kinematic measures, we aim to provide a comprehensive characterization of motor preparation under conditions that simultaneously manipulate temporal precision and mechanical effort. This approach not only extends our understanding of the neurophysiological bases of voluntary movement but also offers a methodological framework for future research in neurorehabilitation and BCI technologies. Ultimately, exploring how RP dynamics encode both timing and effort could lead to more adaptive and ecologically valid paradigms for detecting motor intentions in both healthy and clinical populations.
2. Materials and Methods
2.1. Ethical Approval
All procedures complied with the ethical principles outlined in the Declaration of Helsinki. The study was reviewed and approved by the Ethics Committee of the Centro Universitario de Ciencias de la Salud, Universidad de Guadalajara (approval number: CI-01325, accepted February 6, 2025). Prior to participation, all volunteers received a full explanation of the procedures and signed written informed consent. Participants were informed that they could withdraw from the study at any time without penalty. The ethical framework, selection criteria, informed consent procedures and signal recordings were consistent with previous work in our laboratory [
17].
2.2. Participants
Thirty-one healthy volunteers (15 males and 16 females; mean age: 21.5 ± 2.9 years) were recruited from the university community. Hand dominance was assessed using the Edinburgh Handedness Inventory, and only right-handed participants were included to minimize hemispheric variability in motor cortical activity. All participants had normal or corrected-to-normal vision, no history of neurological, orthopedic, or musculoskeletal disorders, and were free of medications that could influence neuromuscular function or cortical excitability. Data from three participants were excluded: two due to excessive EEG artifacts that precluded reliable analysis and one due to incomplete task performance. The final analysis therefore included 28 participants (13 males, 8 females).
2.3. Experimental Design
The experimental paradigm was designed to evaluate how incremental mechanical load influences cortical preparatory activity reflected in the RP (
Figure 1). Participants were seated comfortably in an adjustable chair with their right forearm resting on a padded support and the elbow fixed at ~90° flexion. The task consisted of voluntary arm flexion movements performed while gripping a custom-designed handle. This handle was mechanically coupled to a support that allowed incremental load application while simultaneously triggering a TTL signal at the precise moment of load release.
Three load conditions were tested: (i) 0 kg, consisting of the unloaded handle (baseline); (ii) 1 kg, corresponding to a light mechanical load; and (iii) 2 kg, corresponding to a moderate load. At the same time, each load condition was tested using three different time constraints: (i) 2 s movements, (ii) 4 s movements and (iii) 6 s movements. Each condition consisted of 40 self-paced trials, resulting in a total of 360 movements per participant. To minimize potential order effects and fatigue, the task was separated into two different days, and the sequence of blocks was randomized across subjects. There was a resting period of 10 minutes in between each set of movements performed on the same day.
Participants sat in front of a screen that indicated the start and end of each task. At the beginning of each block, both the weight load and the intended movement duration were communicated to them. Participants were given instructions to perform smooth and controlled arm flexion movements, avoiding abrupt accelerations, while maintaining a constant wrist angle, restricting the movement exclusively to the elbow joint. Importantly, participants were told to start the movement at their own pace. No external cues, auditory signals, or metronomes were provided, ensuring that movement preparation remained internally generated. A countdown was displayed on the screen after movement onset to help participants guide the timing of their movement. After each movement, participants returned to the initial position, and a randomized resting period of 3 to 8 seconds was displayed on a screen to prevent temporal habituation and anticipation. To avoid using this as a new starting cue, participants were instructed to wait a while after the resting period ended, and to start the next movement at their own pace. A minimum waiting period of 3 seconds was required between the end of the resting period and the initiation of the next movement, but participants weren’t informed about this. If the waiting period was too short, they were simply reminded not to use the end of the resting period as a marker to start the next movement.
A TTL pulse was generated mechanically by the disconnection of the weighted pin from its metallic base at the onset of flexion. This signal provided a millisecond-precise marker of movement initiation. To verify movement onset and ensure temporal alignment, the TTL pulse was cross validated against accelerometer deviations recorded on the wrist.
A training session was held before the experiment to help participants become familiar with the task and perform the movements correctly.
2.4. EEG Recordings
Scalp EEG was recorded using a Grass AS40 Comet system (Natus Medical Inc., USA) with a sampling frequency of 400 Hz. Electrodes were positioned according to the international 10–20 system at Fz, F3, F4, Cz, C3, C4, Pz, P3, and P4, with Fpz as ground and Oz as reference. Impedances were kept below 20 kΩ, which has been validated as adequate for capturing event-related potential without significant distortion [
18,
19].
Analyses focused primarily on Cz and C3 electrodes, corresponding to the supplementary motor area and contralateral motor cortex, where RP amplitudes are most pronounced [
20].
2.5. EMG and Kinematic Recordings
Surface EMG activity was recorded from the right biceps brachii using bipolar Ag/AgCl electrodes (2 cm inter-electrode distance). A ground electrode was placed over the olecranon. Signals were amplified (gain: 10,000) and digitized at 1 kHz using an Axon Digidata 1550B interface (Molecular Devices).
A triaxial accelerometer (200 Hz) was mounted on the medial area of the wrist’s dorsal surface to capture movement kinematics, including onset, duration, and angular displacement of arm flexion. Synchronization between EEG, EMG, and accelerometer data was achieved through a shared hardware clock and validated offline by comparing TTL pulses with accelerometer signals.
2.6. Data Preprocessing and Synchronization
All signals were analyzed offline using MATLAB (MathWorks Inc., Natick, MA, USA). Continuous EEG data were filtered with a zero-phase Butterworth band-pass filter with high and low cut-off frequencies of 0.1 and 30 Hz, respectively. EMG data was band-pass filtered with a Butterworth band-pass filter with cut-off frequencies between 30 and 400 Hz with a notch filter at 60 Hz to remove line noise. The accelerometer signal was filtered using a 5 Hz low-pass IIR filter.
Movement onset was determined using the TTL pulse as a reference. Additional verification by accelerometer deviations was performed to detect cases where movement initiation was not translated into an instant TTL pulse (i.e., anticipatory wrist motion, or errors in TTL signaling) Specifically, if the accelerometer signal exceeded a dynamic threshold (defined as the mean plus two standard deviations of the rest period baseline for each movement) before the TTL pulse, the onset timestamp was adjusted to the earlier point of deviation. Finally, this movement onset adjustment was verified visually by comparing TTL, accelerometer and EMG activity simultaneously.
Epochs for all signals were extracted from –3000 ms to +1000 ms after expected movement duration. Movements that deviated more than 0.5 seconds from the expected time were removed from analysis. All epoch containing gross artifacts in the EEG recording were eliminated via visual inspection. Ocular and muscular artifacts in EEG signals were removed using EEGLAB, an open-source MATLAB toolbox, with the Infomax ICA algorithm [
21], followed by manual verification. Epochs with amplitudes exceeding ±100 µV after artifact removal were automatically discarded due to unsatisfactory removal. For each participant, tasks with fewer than 25 epochs were excluded from the final analysis to minimize RP waveform distortion due to low trial counts
2.7. Data Processing and Analysis
Data processing and analysis were conducted to extract the RP as well as EMG, and kinematic data.
2.7.1. EMG Normalization and Envelope Extraction
To evaluate the temporal dynamics of EMG activation, and to account for inter-subject variability in muscle activation levels, data were normalized using a z-score transformation. For each trial, the EMG signal was transformed as:
Where μbaseline and σbaseline represent the mean and standard deviation of the EMG signal during a pre-movement baseline window (–1200 to –700 ms). This normalization allowed direct comparison of EMG across different load conditions and between participants, effectively scaling all signals to a common unit of standard deviations relative to each participant’s resting activity. After normalization, the signal was rectified, and peak envelope detection was applied
2.7.2. RP Extraction and Quantification
EEG artifact-free trials epochs were averaged within each condition to produce participant-specific waveforms, which were subsequently grand-averaged across participants. A moving average of 30 samples was applied to the RP signal for noise reduction. RP amplitude was quantified from the smoothed RP for each participant using three indices: Early RP (–2000 to –500 ms), Late RP (–500 to 0 ms), and Peak RP (maximum negativity between –500 and +100 ms). Tasks without a clearly observable RP were excluded from analysis.
2.7.3. Fatigue and Muscular Activity Analysis
To evaluate the EMG total energy, Root Mean Square (RMS) were extracted from preprocessed EMG data without z-score normalization. Avoiding normalization prevents converting amplitudes into relative units (i.e., percentage of maximum voluntary contraction, or standard deviation of the resting state) preserving RMS as a direct proxy of EMG amplitude/power, reflecting motor-unit recruitment and firing rate.
To monitor muscle fatigue across load conditions, we computed the EMG power spectrum using a Fast Fourier Transform (FFT) and defined the Median Frequency (MDF) as the frequency at which the one-sided cumulative power reached 50% of the total. For each task, both the initial and final MDF were computed as the mean MDF of the first and last 5 movements, respectively.
Progressive increases in RMS amplitude together with downward shifts in MDF across trials were interpreted as markers of peripheral fatigue [
22].
2.7.4. Kinematic Analysis
A single axis of the triaxial accelerometer data was used to quantify elbow angular displacement, angular velocity, and movement smoothness. The orientation of the sensor and the nature of the movement made gravitational acceleration the main influence on the accelerometer. As the forearm flexed upward, the sensor became progressively more aligned with the gravitational vector resulting in a reliable measure of angular position. The minimum value of the signal, recorded when the arm was resting perpendicular to gravity, was defined as 0 degrees. The maximum value, observed at the end of the flexion where the sensor was aligned with gravity, was defined as 90 degrees. This was then used to compute the mean, maximum and standard deviation of the angular velocity for each movement. Peak angular velocity and variability across repetitions were extracted to assess consistency of motor execution under increasing loads.
2.8. Statistical Analysis
Statistical analyses were performed to assess differences across using the software IBM SPSS Statistics (Version 26.0, Armonk, NY, USA). The study used 9 incomplete blocks each one corresponding to a combination of weight load and movement duration. On average, 14.44 ± 1.67 subjects contributed to each block (coverage 51.6% ± 6.0%; range 42.9–60.7%). Each subject contributed an average of 4.64 ± 2.53 blocks (median 4; range 1–9); 2 participants completed only one block. To test group differences, we used a linear mixed-effects model for a repeated-measures design with incomplete blocks, treating subjects as a random effect across experimental blocks. A Bonferroni correction was applied to control type I error.
Peak RP, Early RP, and Late RP were compared across conditions to assess waveform morphology. Two modeling strategies were used: the first (called model A), duration and load as categorical factors; second (called model B), duration and load as continuous predictors to test linear trends. Mean angular velocity and total RMS values were also used as continuous predictors to test lineal trends in a different model. A final multiple regression model was performed to compare the influence of RMS and weight load in RP when adjusting each other.
Differences in RMS across conditions were also measured using a linear mixed-effects model. In total 6 different analysis of RMS were made considering a combination of weight load and movement duration as categorical factors: 3 of those between weight load in the same movement duration category, the other 3 between movement duration in the same weight load category.
To analyze muscle fatigue, a paired-samples Student t-test compared the Initial MDF and the Final MDF within each experimental block.
Results were considered statistically significant at p < .05 after correction for multiple comparisons where applicable.
3. Results
3.1. Grand Average and Quantitative Modulation of Biceps EMG and Cortical Readiness Potential at Cz
The grand averages revealed systematic modulations of both EMG activity and readiness potential amplitude as a function of mechanical load and movement duration. The EMG envelope of the biceps brachii increased consistently with load magnitude, showing the strongest recruitment in the heaviest condition and the weakest in the unloaded condition. This effect was evident from the onset of contraction and persisted throughout the flexion period, reflecting progressive adjustments of motor unit activity to meet the increased demands (
Figure 2).
Quantitative analyses of RMS values confirmed significant differences between load conditions in the same movement duration (2 s: F(24.053) = 14.21, p < .001; 4 s: F(28.358) = 17.479, p < .001; 6 s: F(22.252) = 10.588, p < .001), while no significant effect of movement duration was observed within the same load condition (0 kg: F(21.153) = 2.251, p = .130; 1 kg: F(22.429) = 1.955, p = .165; 2 kg: F(22.120) = 0.158, p = .855). Pairwise comparisons of load conditions within the same movement duration showed significant differences after Bonferroni correction (all p < .05), except between 0 and 1 kg in the 2 s movement (p = .322) and between 4 and 6 kg in the 6 s movement (p = .764)
At the cortical level, the readiness potential displayed the characteristic slow-rising negativity preceding movement onset. RP amplitude at Cz scaled reliably with mechanical load, with the largest negativity obtained in the heavy-load condition, intermediate values in the light-load condition, and the smallest amplitudes in the unloaded condition. This modulation was consistent across all movement durations, indicating that mechanical load enhances motor preparatory activity independently of temporal constraints.
Movement duration also influenced the morphology of the RP, as previously demonstrated in our earlier work [
17]. In that study, we reported that longer movement durations are associated with a gradual reduction in RP amplitude, reflecting temporal downscaling of cortical preparation. The present results confirm this temporal effect, with shorter movements displaying steeper slopes and larger amplitudes, whereas longer movements produced more gradual build-ups with smaller amplitudes. Crucially, these temporal dynamics did not alter the load-related ordering of RP amplitudes, which was preserved across all durations.
Taken together, these findings demonstrate that incremental mechanical load enhances muscle activation at the periphery (EMG) and cortical preparatory activity (RP) in a consistent manner. At the same time, movement duration independently modulates the temporal profile of the RP, confirming our previous observations and highlighting the complementary influence of load and time on the dynamics of motor preparation.
3.2. Modulation of Peak RP by Mechanical Load and Movement Duration at Cz
Statistical analysis of the peak amplitude of the RP at CZ using weight load and movement duration as categorical factors revealed distinct and statistically independent influences of mechanical load and movement duration on cortical preparatory activity. As a first approximation a model considering all combinations of weight load and movement duration, as well as the interaction between them. As shown in
Figure 3, no statistical significance was observed in the interaction of conditions (
F(4,105.5)=0.312,
p = .869) meaning that the effect of weight load and movement duration in the Peak RP was independent of each other, making possible the comparison between them by adjusting for the effect of the other. This comparison revealed statistical differences between different movement durations (
F(2, 105.140) = 24.657,
p < .001) and weight loads
For the effect of mechanical load, the estimated marginal means showed a consistent increase in peak amplitude as the lifted weight increased. The largest negativities were obtained under the 2 kg condition (mean = -8.144 ± .393 µV), followed by the 1 kg condition (mean = -7.329 ± .394 µV), whereas the unloaded condition displayed the smallest amplitude (mean = 5.750 ± .397 µV). The main effect of load was significant ( F( 2, 108.872) = 108.872, p < .001), with post-hoc comparisons confirming differences between 0 kg and 2 kg (p < 0.001) and between 0 kg and 1 kg (p = 0.003).
When analyzed as a function of movement duration, the peak amplitude exhibited an opposite trend, decreasing progressively as movement time increased. The highest negativities were found in the 2-s condition (mean = -8.740 ± .397 µV), followed by the 4-s (mean = -7.055 ± .381 µV) and 6-s conditions (mean = -5.428 ± .400 µV), which showed progressively smaller amplitudes. The global effect of duration was statistically significant (p < 0.001), with pairwise differences between 2 s and 4 s (p = 0.001), 2s and 6 s (p <.0.001) and between 4 s and 6 s (p = 0.002).
This result indicates that mechanical load and temporal duration contribute independently to the modulation of RP amplitude. Together, these findings demonstrate that while increasing load enhances cortical preparation, longer movements attenuate it, confirming that both factors act as complementary yet non-interacting determinants of preparatory cortical dynamics.
3.3. Comparative Distribution of Peak Readiness Potential Amplitude Across Load and Duration Conditions
A complementary analysis was performed to reinforce the results by comparing specific combinations of weight load and movement duration as categorical factors: 3 comparisons between weight load in the same movement duration category and another 3 between movement duration in the same weight load category. The distribution of peak readiness potential amplitude at Cz exhibited systematic variations across movement durations and load conditions.
Figure 4 presents the grouped boxplots showing the spread, median, and interquartile range of the amplitude values obtained for each weight load (0, 1, and 2 kg) at the three movement durations (2, 4, and 6 s). All models showed significant effects (all p < .05) except for the effect of weight load in the 2 s movement condition (F(2, 29.142) = 2.38, p = .111).
Regarding the comparisons of movement duration within the same weight load, for the unloaded condition (0 kg), the marginal mean RP amplitudes were −8.045 ± 0.572 µV at 2 s, −5.881 ± 0.519 µV at 4 s, and −4.221 ± 0.593 µV at 6 s. Significant differences were found between 2 s and 4 s (p < .05) and between 2 s and 6 s (p < .001). Under the 1 kg condition, amplitudes were −8.830 ± 0.593 µV at 2 s, −7.579 ± 0.552 µV at 4 s, and −5.947 ± 0.535 µV at 6 s, with a significant difference between 2 s and 6 s (p < .01). For the 2 kg condition, amplitudes were −9.805 ± 0.680 µV at 2 s, −8.105 ± 0.700 µV at 4 s, and −6.266 ± 0.748 µV at 6 s, with a significant difference again between 2 s and 6 s (p < .01).
In the comparisons of weight load within the same movement duration, for the 2 s movement, the marginal mean amplitudes were −8.005 ± 0.710 µV (no load), −8.701 ± 0.736 µV (1 kg), and −9.933 ± 0.666 µV (2 kg), with no significant differences. For the 4 s movement, amplitudes were −5.733 ± 0.555 µV (no load), −7.581 ± 0.590 µV (1 kg), and −8.161 ± 0.589 µV (2 kg), with a significant difference between 2 kg and no load (p < .01). For the 6 s movement, amplitudes were −4.059 ± 0.584 µV (no load), −5.952 ± 0.510 µV (1 kg), and −6.217 ± 0.564 µV (2 kg), with significant differences between 2 kg and no load (p < .05) and between 1 kg and no load (p < .05).
The data distributions displayed in
Figure 4 show well-defined separations among medians and interquartile ranges within each load condition, as well as consistent shifts across durations. The observed pattern highlights the quantitative relationships among time, load, and amplitude magnitude, as reflected in the spread and central tendency of the boxplot distributions.
3.4. Modulation of Late and Early RP Amplitude by Mechanical Load and Movement Duration at Cz
The analysis of Late RP at Cz using weight load and movement duration as categorical factors revealed distinct and statistically independent influences of mechanical load and movement duration on cortical preparatory activity. No statistical significance was observed in the interaction of these conditions (F (4,110.808) = 0.132, p = .970), while differences were revealed between different movement durations (F(2, 108.988) = 10.628, p < .001) and weight loads (F(2, 112.813) = 6.822 p = .002)
Following the same modulation of the Peak RP, the estimated marginal means for Late RP showed a consistent increase in amplitude as the lifted weight increased ( 0 kg mean = -3.317 ± .349 µV; 1 kg mean = -3.979 ± .348 µV; 2 kg mean = -4.945 ± .346 µV), and a consistent decrease as the movement duration increased (2 s mean = -4.899 ± .4.409 µV; 1 4 s mean = -4.409 ± .334 µV; 2 kg mean = -2.932 ± .353 µV). Post-hoc comparisons confirmed differences between 0 kg and 2 kg (p < 0.01), between 2 s and 6 s (p < 0.001) and between 4 s and 6 s (p < 0.01) (
Figure 5).
In contrast, the analysis of Early RP at Cz only showed a statistical difference in the effect of weight load (F(2, 114.308) = 3.379 p = 0.038) with no differences in the effect of movement duration (F(2, 110.544) = 1.051 p = 0.353). Post-hoc comparisons of weight load didn’t show statistical differences (all p > 0.05).
3.6. Linear Trend Modeling of Peak RP Amplitude Based on Experimental and Physiological Predictors at Cz Channel
As previously shown in
Figure 3 and
Figure 4, a linear trend between the experimental conditions and Peak RP amplitude was apparent. To formally test this relationship, a linear mixed-effects model was implemented using movement duration and load as continuous predictors. Additionally, a second approach was evaluated based on physiological and mechanical outcomes of the movement. Model A included movement duration and weight lifted as predictors, whereas Model B included biceps RMS and mean angular velocity.
Figure 6 summarizes the fitted regressions and the correspondence between observed and predicted values for both models.
In Model A, the regression analysis revealed that readiness potential amplitude decreased significantly with increasing movement duration (β = 0.817, p < 0.001, 95% CI [0.588, 1.046 ]) and increased with increasing weight load (β = −1.208, p < 0.001, 95% CI [-1.668, -0.749]). The tridimensional representation showed a continuous modulation of amplitude across both predictors. The predicted-versus-observed comparison demonstrated a significant linear correspondence (R2 = 0.335, p < 0.001), which increased when accounting for the random intercept of each subject (R2 = 0.527 p < 0.001).
In Model B, modeled as a function of (°/s) and biceps RMS (µV), both predictors showed negative linear coefficients: angular velocity (β = −0.100, p < 0.001, 95% CI [-0.135, -.066 ]) and RMS (β = −0.0129, p < 0.05, 95% CI [-.0237, -.002]). The tridimensional surface displayed the combined contribution of these variables, with a gradual increase in amplitude along both axes. The predicted-versus-observed plots confirmed a stable linear fit (R2 = 0.205, p < .001 ), which increased after incorporating subject-level random effects (R2 = 0.386 p < .001).
Across both models, the predicted and observed values showed low dispersion, indicating a consistent linear relationship between readiness potential amplitude and the predictors included in each model. Model A captured variance primarily associated with task parameters (movement duration and load), whereas Model B accounted for the biomechanical and muscular components (RMS and angular velocity). This evidence shows that both predictor sets can be used to explain the effects in Peak RP amplitudes.
3.7. Linear Trend Modeling of Late and Early RP at Cz Channel
The same models used to test for linear trends in Peak RP were applied to test for Late and Early RP effects.
Late RP showed the same modulation as Peak RP with increased amplitude as a function of weight load, RMS, and angular velocity, and decreased amplitude as a function of movement duration (Model A: movement duration β = 0.486, p < 0.001, 95% CI [0.270, 0.703], weight load β = −0.797, p < 0.001, 95% CI [-1.228, -0.365]; Model B: angular velocity β = −0.059, p < 0.001, 95% CI [-0.088, -0.028 ], RMS β = −0.012, p < 0.05, 95% CI [-.0211, -.003]).
In contrast, Early RP only showed a modulation as a function of weight load for model A and no significant modulation for Model B respectively (Model A: movement duration β = -0.076, p = 0.432, 95% CI [-0.267, 0.114], weight load β = −0.461, p < 0.05, 95% CI [-0.841, -0.081]; Model B: angular velocity β = −0.059, p < 0.001, 95% CI [-0.088, -0.028 ], RMS β = −0.012, p < 0.05, 95% CI [-.0211, -.003]).
3.8. Corrected Fixed-Effects Modeling of Readiness Potential Amplitude at Cz as a Function of Mechanical Load and Biceps RMS
As both linear trend models showed a significant effect as a function of task demands and physiological responses, a final analysis was performed to determine if the physiological responses were more important than the task demands. To assess potential multicollinearity, we first examined the correlations between RMS and weight lifted, and between angular velocity and movement duration. The analysis showed a moderate correlation for the RMS and the weight lifted (r = 0.382 p< 0.001). and a strong negative correlation between angular velocity and movement duration (r = -0.803 p < 0.001). Given the strong correlation between angular velocity and movement duration, only RMS and weight lifted were retained as independent predictors in subsequent analyses.
Additionally, because RMS represents the overall muscular response during the entire movement rather than the preparatory phase, an Iinital RMS (iRMS) measure was computed from −200 to +200 ms around movement onset. This value was used as an index of early neuromuscular activation, potentially reflected in the neural activity preceding movement execution.
Two separate linear regression analysis were performed to evaluate the relationship between RP amplitude and the combined effects of weight lifted and biceps RMS or iRMS respectively, using corrected fixed effects derived from the mixed-effects models.
Figure 7 illustrates the resulting multidimensional regressions for both the peak and late components of the potential.
The results showed that the main predictor for the peak component was the weight load, as the effect of biceps RMS loses all its statistical effect when adjusted for the first. Panel A shows the interaction between weight lifted on the x-axis, RMS on the y-axis, and amplitude in microvolts on the z-axis, revealing a consistent negative slope across both predictors (β_weight =−1.320, p <0 .001; β_RMS = −0.001, p = .851). When iRMS values were considered instead of total RMS (Panel B), the overall pattern remained similar (β_weight = -1.022 p = 0.001 ; β_iRMS = -0.023, p = 0.071).
For the late component, a similar relationship was observed. The tridimensional representation (Panel C) shows amplitude as a function of weight lifted and total RMS (weight β = -0.711, p < 0.05 ; RMS β = -0.005, p = 0.425). When iRMS was used (Panel D) both predictors showed significant effects on Late RP (β_weight = -0.559, p < 0.05; β_iRMS = -0.025, p < 0.05), suggesting an independent contribution of early neuromuscular activation to the late RP beyond the influence of weight load.
3.9. Spatial Distribution of RP Across EEG Regions
Statistical analysis of the Peak and Late RP across all EEG channels revealed consistent and statistically independent effects of mechanical load and movement duration on cortical preparatory activity (all
p < .01), with no significant interaction between them (all
p > 0.05). In contrast, Early RP only showed statistical effects in Cz, C3 and F4 electrodes (all
p < 0.05).
Table 1 summarizes the fixed effects for each electrode.
The estimated marginal means of Peak and Late RP follow the same trend across channels, with higher amplitudes in the 2 s and 2 kg conditions and lower amplitudes in the 0 kg and 6 s conditions. Peak RP amplitude increased most clearly at central electrodes (Cz, C3, C4) as movement duration decreased, and at Cz, C3, and F4 as weight load increased. The electrodes most influenced by load corresponded to the contralateral motor and ipsilateral frontal regions relative to the moving arm (
Figure 8) Regarding Early RP, only weight load showed observable effects especially in central and frontal regions.
The analysis of linear trends across EEG channels, using movement duration and weight lifted as predictors, is summarized in
Figure 9. Late and Peak RP components showed the same modulation pattern, with amplitude increasing as a function of weight load and decreasing with longer movement duration across all channels (all p < 0.05). In contrast, the Early RP showed a significant modulation only as a function of weight load, mainly over the frontal region (F3, F4, Fz; p < 0.05), the contralateral central region (Cz, C3; p < 0.05), and the P4 electrode (p < 0.05).
Regarding the weight load predictor, the higher slopes were found in F4 (Peak RP β = −1.531 p < .001; Late RP β = −1.116, p < .001; Early RP β = −0.492, p = .026) and C3 (Peak RP β = −1.543 p < .001; Late RP β = −0.806, p < .001; Early RP β = −0.491, p = .006) channels. The movement duration predictor was only significant for Peak and Late RP with higher slopes in the central and frontal regions.
5. Conclusions
The present study provides convergent electrophysiological evidence that the amplitude of the RP scales systematically with both mechanical load and movement duration, reflecting the integrative function of cortical preparatory networks in voluntary motor control. Incremental increases in load produced a proportional enhancement of RP negativity, supporting the interpretation that this potential encodes the intensity of central motor command and the energetic cost of action. Conversely, prolonged movement durations led to attenuated RP amplitudes, suggesting that temporal uncertainty and extended control windows redistribute preparatory resources, thereby reducing cortical readiness.
Taken together, these findings indicate that the RP embodies a dual coding mechanism: one dimension related to the magnitude of mechanical effort, and another to the predictability and timing of action initiation. This dual modulation highlights the hierarchical organization of preparatory activity, with the SMA coordinating temporal anticipation and the M1 specifying quantitative motor parameters.
By combining controlled manipulations of load and duration, the present work bridges previously separate lines of research on effort- and time-dependent modulation of the RP. The results contribute to a refined theoretical framework in which cortical readiness operates as an adaptive optimization process, integrating energetic, temporal, and predictive dimensions to ensure efficient and accurate voluntary movement.
Beyond its theoretical implications, the present evidence also strengthens the translational relevance of the RP for neuroengineering and rehabilitation. Since RP features such as amplitude, onset latency, and spatial distribution can predict motor intention before overt movement, understanding how these parameters vary with mechanical and temporal constraints may guide the development of asynchronous BCIs and adaptive neuroprosthetic systems. In particular, the graded RP modulation identified here could inform algorithms capable of decoding not only the occurrence of movement intention but also the intensity and timing demands of the planned action, thereby enhancing the ecological precision and responsiveness of next-generation brain–computer interfaces.
Author Contributions
Conceptualization, Oscar Alexis Becerra-Casillas and Braniff de la Torre-Valdovinos; methodology, Oscar Alexis Becerra-Casillas, Karen Alejandra Díaz-Lozano and Braniff de la Torre-Valdovinos; validation, Oscar Alexis Becerra-Casillas, Karen Alejandra Díaz-Lozano, Mario Treviño, Paulina Osuna-Carrasco, and Braniff de la Torre-Valdovinos; formal analysis, Oscar Alexis Becerra-Casillas, Karen Alejandra Díaz-Lozano and Braniff de la Torre-Valdovinos; investigation, Oscar Alexis Becerra-Casillas, Karen Alejandra Díaz-Lozano; resources, Mario Treviño and Braniff de la Torre-Valdovinos; data curation, Oscar Alexis Becerra-Casillas, Karen Alejandra Díaz-Lozano, Mario Treviño, and Paulina Osuna-Carrasco; writing—original draft, Oscar Alexis Becerra-Casillas, Karen Alejandra Díaz-Lozano, Mario Treviño, Paulina Osuna-Carrasco, and Braniff de la Torre-Valdovinos; writing—review and editing, Oscar Alexis Becerra-Casillas, Karen Alejandra Díaz-Lozano, Mario Treviño, Paulina Osuna-Carrasco, and Braniff de la Torre-Valdovinos; supervision, Braniff de la Torre-Valdovinos; project administration, Braniff de la Torre-Valdovinos; funding acquisition, Braniff de la Torre-Valdovinos..
Figure 1.
Experimental setup and muscle fatigue analysis. (A) Signal acquisition scheme. EEG was recorded from scalp electrodes positioned according to the international 10–20 system at Fz, F3, F4, Cz, C3, C4, Pz, P3, and P4, with Fpz as ground and Oz as reference. EMG was recorded from the biceps brachii, and acceleration from a wrist-mounted accelerometer. Participants performed nine sets of forty arm flexions, each set corresponding to a specific movement duration (2, 4, or 6 s) and load condition (0, 1, or 2 kg). A TTL pulse synchronized EEG, EMG, and accelerometer recordings. (B) Comparison of the median frequency (MDF) of the EMG signal at the beginning (Initial MDF) and end (Final MDF) of each set of movements. Initial and Final MDF values were computed as the average MDF of the first and last five movements, respectively. No significant differences were found between initial and final MDF across conditions (all p>0.05).
Figure 1.
Experimental setup and muscle fatigue analysis. (A) Signal acquisition scheme. EEG was recorded from scalp electrodes positioned according to the international 10–20 system at Fz, F3, F4, Cz, C3, C4, Pz, P3, and P4, with Fpz as ground and Oz as reference. EMG was recorded from the biceps brachii, and acceleration from a wrist-mounted accelerometer. Participants performed nine sets of forty arm flexions, each set corresponding to a specific movement duration (2, 4, or 6 s) and load condition (0, 1, or 2 kg). A TTL pulse synchronized EEG, EMG, and accelerometer recordings. (B) Comparison of the median frequency (MDF) of the EMG signal at the beginning (Initial MDF) and end (Final MDF) of each set of movements. Initial and Final MDF values were computed as the average MDF of the first and last five movements, respectively. No significant differences were found between initial and final MDF across conditions (all p>0.05).
Figure 2.
Grand averages of readiness potentials and EMG envelopes across load conditions and movement durations. Grand averages of the readiness potential at Cz (upper traces) and the biceps brachii EMG envelope (lower traces) recorded during voluntary wrist flexion under three load conditions: 2 kg (brown), 1 kg (green), and 0 kg (yellow). Traces are time-locked to movement onset (0 ms). The RP traces show the premotor activity aligned to movement initiation, while the EMG envelopes illustrate the corresponding muscle activation. (A) Recordings obtained during movements executed in 2 s; (B) recordings obtained during movements executed in 4 s; (C) recordings obtained during movements executed in 6 s.
Figure 2.
Grand averages of readiness potentials and EMG envelopes across load conditions and movement durations. Grand averages of the readiness potential at Cz (upper traces) and the biceps brachii EMG envelope (lower traces) recorded during voluntary wrist flexion under three load conditions: 2 kg (brown), 1 kg (green), and 0 kg (yellow). Traces are time-locked to movement onset (0 ms). The RP traces show the premotor activity aligned to movement initiation, while the EMG envelopes illustrate the corresponding muscle activation. (A) Recordings obtained during movements executed in 2 s; (B) recordings obtained during movements executed in 4 s; (C) recordings obtained during movements executed in 6 s.
Figure 3.
Estimated marginal means ± 95% CI of the peak amplitude at the Cz electrode. (A) Effect of mechanical load, showing amplitude as a function of lifted weight (2 kg = brown; 1 kg = green; 0 kg = yellow). (B) Effect of movement duration, showing amplitude as a function of movement time (2 s = red; 4 s = blue; 6 s = green). (C) Combined representation of load and duration illustrating their independent contributions to cortical modulation. N=132 from 28 subjects.
Figure 3.
Estimated marginal means ± 95% CI of the peak amplitude at the Cz electrode. (A) Effect of mechanical load, showing amplitude as a function of lifted weight (2 kg = brown; 1 kg = green; 0 kg = yellow). (B) Effect of movement duration, showing amplitude as a function of movement time (2 s = red; 4 s = blue; 6 s = green). (C) Combined representation of load and duration illustrating their independent contributions to cortical modulation. N=132 from 28 subjects.
Figure 4.
Distribution of peak readiness potential amplitude at Cz across the nine experimental conditions (3 movement durations x 3 load conditions). Each group of three boxplots represents 2-kg (brown), 1-kg (green), and no-weight (yellow) movements within a single duration condition (2 s, 4 s, 6 s). Boxes indicate interquartile ranges with median lines; whiskers represent the 10th–90th percentiles. Pairwise comparisons derived from six independent linear mixed-effects models (three testing the effect of load within each duration, and three testing the effect of duration within each load) are indicated above the relevant groups. N values correspond to the number of observations included in each linear mixed-effects model: for analyses of weight load within each movement duration, 2 s condition (N = 43, from 23 subjects), 4 s (N = 47, from 24 subjects), and 6 s (N = 42, from 26 subjects); and for analyses of movement duration within each load, 0 kg (N = 44, from 21 subjects), 1 kg (N = 44, from 23 subjects), and 2 kg (N = 44, from 23 subjects).
Figure 4.
Distribution of peak readiness potential amplitude at Cz across the nine experimental conditions (3 movement durations x 3 load conditions). Each group of three boxplots represents 2-kg (brown), 1-kg (green), and no-weight (yellow) movements within a single duration condition (2 s, 4 s, 6 s). Boxes indicate interquartile ranges with median lines; whiskers represent the 10th–90th percentiles. Pairwise comparisons derived from six independent linear mixed-effects models (three testing the effect of load within each duration, and three testing the effect of duration within each load) are indicated above the relevant groups. N values correspond to the number of observations included in each linear mixed-effects model: for analyses of weight load within each movement duration, 2 s condition (N = 43, from 23 subjects), 4 s (N = 47, from 24 subjects), and 6 s (N = 42, from 26 subjects); and for analyses of movement duration within each load, 0 kg (N = 44, from 21 subjects), 1 kg (N = 44, from 23 subjects), and 2 kg (N = 44, from 23 subjects).

Figure 5.
Estimated marginal means (±95% CI) of RP amplitude at the Cz channel. (A) Late RP amplitude showed significant main effects of both weight load and movement duration, with increasing load and shorter durations associated with higher (more negative) amplitudes. (B) Early RP amplitude showed a weaker modulation, reaching significance only for weight load (p = 0.038). Global effects and pairwise comparisons are indicated in each panel.
Figure 5.
Estimated marginal means (±95% CI) of RP amplitude at the Cz channel. (A) Late RP amplitude showed significant main effects of both weight load and movement duration, with increasing load and shorter durations associated with higher (more negative) amplitudes. (B) Early RP amplitude showed a weaker modulation, reaching significance only for weight load (p = 0.038). Global effects and pairwise comparisons are indicated in each panel.
Figure 6.
Linear regression models relating readiness potential amplitude to experimental and physiological predictors. (A) Model A: tridimensional surface showing amplitude as a function of movement duration (x-axis), weight lifted (y-axis), and mean potential in µV (z-axis). (B) Predicted versus observed amplitudes for Model A. (C) Predicted versus observed amplitudes including subject intercepts for Model A. (D) Model B: tridimensional surface showing amplitude as a function of angular velocity (x-axis), biceps RMS in µV (y-axis), and mean potential in µV (z-axis). (E) Predicted versus observed amplitudes for Model B. (F) Predicted versus observed amplitudes including subject intercepts for Model B. The red dashed line represents the identity line, indicating the values predicted according to the linear regression model, whereas the black solid line corresponds to the regression computed directly from the observed data.
Figure 6.
Linear regression models relating readiness potential amplitude to experimental and physiological predictors. (A) Model A: tridimensional surface showing amplitude as a function of movement duration (x-axis), weight lifted (y-axis), and mean potential in µV (z-axis). (B) Predicted versus observed amplitudes for Model A. (C) Predicted versus observed amplitudes including subject intercepts for Model A. (D) Model B: tridimensional surface showing amplitude as a function of angular velocity (x-axis), biceps RMS in µV (y-axis), and mean potential in µV (z-axis). (E) Predicted versus observed amplitudes for Model B. (F) Predicted versus observed amplitudes including subject intercepts for Model B. The red dashed line represents the identity line, indicating the values predicted according to the linear regression model, whereas the black solid line corresponds to the regression computed directly from the observed data.
Figure 7.
Linear regression of corrected fixed effects on readiness potential amplitude at Cz. (A) Peak component as a function of weight lifted (x-axis), biceps RMS (y-axis), and mean amplitude in µV (z-axis). (B) Peak component as a function of weight lifted and initial RMS. (C) Late component as a function of weight lifted and total RMS. (D) Late component as a function of weight lifted and initial RMS. All regressions correspond to corrected fixed effects from the mixed-effects models.
Figure 7.
Linear regression of corrected fixed effects on readiness potential amplitude at Cz. (A) Peak component as a function of weight lifted (x-axis), biceps RMS (y-axis), and mean amplitude in µV (z-axis). (B) Peak component as a function of weight lifted and initial RMS. (C) Late component as a function of weight lifted and total RMS. (D) Late component as a function of weight lifted and initial RMS. All regressions correspond to corrected fixed effects from the mixed-effects models.
Figure 8.
Topographic distribution of the estimated marginal means of RP components. (A) Peak RP, (B) Late RP, and (C) Early RP amplitudes are shown as a function of movement duration (rows: 6, 4, and 2 s) and weight load (columns: 0, 1, and 2 kg). Each map represents the marginal means of RP amplitude across participants obtained from the linear mix effects model analysis, illustrating stronger central negativity with shorter movement durations and higher weights. Color scales represent amplitude in microvolts (µV).
Figure 8.
Topographic distribution of the estimated marginal means of RP components. (A) Peak RP, (B) Late RP, and (C) Early RP amplitudes are shown as a function of movement duration (rows: 6, 4, and 2 s) and weight load (columns: 0, 1, and 2 kg). Each map represents the marginal means of RP amplitude across participants obtained from the linear mix effects model analysis, illustrating stronger central negativity with shorter movement durations and higher weights. Color scales represent amplitude in microvolts (µV).
Figure 9.
Topographic distribution of linear regression slopes for weight load and movement duration effects on Readiness Potential (RP) amplitude. (A) Scalp maps show the regression slopes (β) for the effect of weight load across Peak, Late, and Early RP components. Increasing weight load was associated with stronger (more negative) RP amplitudes, especially over central and frontal regions. (B) Regression slopes for movement duration revealed an opposite trend, with longer durations producing smaller (less negative) RP amplitudes, mainly over central electrodes. Color scales represent β values from linear models (β, in µV per unit change of the predictor variable).
Figure 9.
Topographic distribution of linear regression slopes for weight load and movement duration effects on Readiness Potential (RP) amplitude. (A) Scalp maps show the regression slopes (β) for the effect of weight load across Peak, Late, and Early RP components. Increasing weight load was associated with stronger (more negative) RP amplitudes, especially over central and frontal regions. (B) Regression slopes for movement duration revealed an opposite trend, with longer durations producing smaller (less negative) RP amplitudes, mainly over central electrodes. Color scales represent β values from linear models (β, in µV per unit change of the predictor variable).
Table 1.
Type III Tests of Fixed Effects for RP Amplitude Across Electrodes.
Table 1.
Type III Tests of Fixed Effects for RP Amplitude Across Electrodes.
| |
Effect |
Peak RP |
Late RP |
Early RP |
| |
|
n_df |
d_df |
F |
p |
d_df |
F |
p |
d_df |
F |
p |
| CZ |
Movement Duration |
2 |
105.14 |
24.66 |
< 0.001*** |
108.99 |
10.63 |
< 0.001*** |
110.54 |
1.05 |
0..53 |
| Weight Load |
2 |
108.87 |
13.22 |
< 0.001*** |
112.81 |
6.82 |
0.002** |
114.31 |
3.38 |
0.038* |
| Interaction |
4 |
105.50 |
0.31 |
0.869 |
109.29 |
0.29 |
0.884 |
110.81 |
0.13 |
0.97 |
| C3 |
Movement Duration |
2 |
106.22 |
32.25 |
< 0.001*** |
109.84 |
10.51 |
< 0.001*** |
110.95 |
0.20 |
0.821 |
| Weight Load |
2 |
109.91 |
31.80 |
< 0.001*** |
113.24 |
14.64 |
< 0.001*** |
114.85 |
3.60 |
0.030* |
| Interaction |
4 |
106.56 |
0.97 |
0.869 |
110.12 |
0.55 |
0.699 |
111.20 |
0.16 |
0.96 |
| C4 |
Movement Duration |
2 |
109.07 |
21.08 |
< 0.001*** |
109.75 |
10.48 |
< 0.001*** |
108.99 |
0.73 |
0.487 |
| Weight Load |
2 |
113.88 |
8.53 |
< 0.001*** |
113.80 |
5.83 |
0.004** |
113.77 |
0.70 |
0.501 |
| Interaction |
4 |
109.34 |
0.85 |
0.499 |
110.03 |
0.37 |
0.829 |
109.26 |
1.32 |
0.269 |
| FZ |
Movement Duration |
2 |
111.47 |
16.94 |
< 0.001*** |
114.25 |
6.22 |
0.003** |
108.70 |
0.20 |
0.82 |
| Weight Load |
2 |
115.79 |
9.16 |
< 0.001*** |
117.76 |
4.88 |
0.009** |
114.48 |
3.06 |
0.051 |
| Interaction |
4 |
111.68 |
0.57 |
0.683 |
114.39 |
0.81 |
0.521 |
108.89 |
0.69 |
0.6 |
| F3 |
Movement Duration |
2 |
109.52 |
14.17 |
< 0.001*** |
109.20 |
8.93 |
< 0.001*** |
108.56 |
0.08 |
0.92 |
| Weight Load |
2 |
113.23 |
6.25 |
< 0.001*** |
113.22 |
5.40 |
.006** |
113.40 |
3.06 |
0.051 |
| Interaction |
4 |
109.81 |
1.33 |
0.262 |
109.49 |
0.82 |
0.513 |
108.84 |
1.22 |
0.309 |
| F4 |
Movement Duration |
2 |
108.22 |
13.99 |
< 0.001*** |
109.29 |
5.52 |
0.005** |
108.22 |
0.02 |
0.985 |
| Weight Load |
2 |
113.46 |
13.99 |
< 0.001*** |
113.12 |
10.90 |
< 0.001*** |
112.49 |
4.58 |
0.012* |
| Interaction |
4 |
108.49 |
0.73 |
0.574 |
109.58 |
0.39 |
0.817 |
108.53 |
0.79 |
0.536 |
| PZ |
Movement Duration |
2 |
100.20 |
26.56 |
< 0.001*** |
107.10 |
11.17 |
< 0.001*** |
114.45 |
1.56 |
0.216 |
| Weight Load |
2 |
105.94 |
17.87 |
< 0.001*** |
110.96 |
9.00 |
< 0.001*** |
118.31 |
2.24 |
0.111 |
| Interaction |
4 |
100.65 |
1.86 |
0.123 |
107.44 |
0.85 |
0.5 |
114.52 |
2.02 |
0.096 |
| P3 |
Movement Duration |
2 |
108.99 |
14.01 |
< 0.001*** |
115.20 |
4.51 |
0.013* |
113.66 |
0.06 |
0.94 |
| Weight Load |
2 |
114.23 |
12.48 |
< 0.001*** |
118.71 |
5.81 |
.004** |
117.96 |
0.78 |
0.462 |
| Interaction |
4 |
109.22 |
1.19 |
0.318 |
115.26 |
0.81 |
0.521 |
113.70 |
2.00 |
0.1 |
| P4 |
Movement Duration |
2 |
108.76 |
9.16 |
< 0.001*** |
111.04 |
3.66 |
0.029* |
111.42 |
0.14 |
0.867 |
| Weight Load |
2 |
113.05 |
7.62 |
< 0.001*** |
115.24 |
3.49 |
0.034* |
116.00 |
0.88 |
0.417 |
| Interaction |
4 |
109.05 |
0.13 |
0.97 |
111.27 |
0.16 |
0.958 |
111.60 |
0.90 |
0.465 |