Abstract
Many research studies have evaluated the effects of whole-body vibration exercise on muscular strength, standing balance, and bone density, but relatively few reports have evaluated safety issues for vibration exercises. Knee flexion reduces acceleration transmission to the head during static exercise. However, few studies have evaluated dynamic exercises. The purpose of this investigation was to evaluate the transmission of acceleration to the head during dynamic squats. Twelve participants performed dynamic squats (0°-40° of knee flexion) on a synchronous vertical whole-body vibration platform. Platform frequencies from 20 to 50 Hz were tested at a peak-to-peak nominal displacement setting of 1 mm. Transmissibilities from the platform to head varied depending on platform frequency and knee flexion angle. We observed amplification during 20 and 25 Hz platform vibration when knee flexion was <20°. Vibration from exercise platforms can be amplified as it is transmitted through the body to the head during dynamic squats. Similarly, this vibration energy contributes to observed injuries such as retinal detachment. It is recommended that knee flexion angles of at least 20° and vibration frequencies above 30 Hz are used when performing dynamic squat exercises with whole-body vibration.
Keywords
Introduction
Whole-body vibration exercise (WBVE) has become a popular modality and is found in homes, public gyms, and in the offices of various health-care professionals. WBVE can lead to improvements in strength, 1 improved bone mineral density in animal models, 2 articular cartilage in human subjects, 3 and decreased risk of falls in the elderly. 4,5 While these studies report benefits of WBVE, others have reported mixed results depending on the performance indicator. 6 –8
Several studies have investigated the safety of WBVE and the response of the body to mechanical vibration. 9 –12 Occupational research has identified that prolonged exposure to whole-body vibration has deleterious effects on the musculoskeletal system. 13,14 In particular, resonance, where the vibration is amplified, may increase the risk of injury from mechanical vibration. The head resonates at vibration frequencies below 30 Hz. 9,15 Excessive mechanical energy transferred to the head can cause retinal detachment, visual disruptions, and cognitive impairment. 16,17 Knee flexion angles (KFAs) greater than 20° can effectively dampen mechanical vibration reaching the hip 12 and head during static squat postures. 9 Similar attenuation of vibration reaching the hip has been reported for slow squats 12 but has not been evaluated for the transmission to the head.
WBVE platforms are often used for dynamic exercise. 1,5,7,18 –23 However, some evidence indicates that WBVE using dynamic movements appear to lead to different biodynamic responses than static exercises, 12 and accordingly dynamic exercises warrant additional research. The goal of this research was to evaluate transmissibility to the head during dynamic squats at 7 discrete input frequencies between 20 and 50 Hz from a WBVE platform. In addition, the concentric and eccentric phases of the squat are evaluated to determine whether the musculature is limited in its capacity to attenuate vibration during these different types of contraction. This research may provide insight for safer prescription of WBVE.
Materials and Methods
Participants and Study Design
Twelve healthy male volunteers 26.3 years of age (SD 2.1), 178.0 cm height (SD 6.0), and 79.5 kg weight (SD 11.5) were recruited to participate in this study. This sample size was calculated using commercially available software 24 (G*power version 3.1.9.3), based on 80% power to detect a large effect size (0.8), with alpha = 0.05. Due to exclusion criteria, none of these participants had a history of head trauma, cardiovascular diseases, joint implants, or low back pain. The study was approved by the research ethics board of the University of Western Ontario and each participant provided informed consent by signing the approved consent form. Participants completed a preliminary session on the day prior to testing to familiarize them with the postures, the vibrating exercise platform, and the attachment protocol of the instrumentation. Participants were asked to report any extreme discomfort or unusual symptoms; if these occurred then the experiment would be stopped.
Participants were instructed not to partake in any physical activity in the hours leading up to the experiment as muscular fatigue could alter vibration transmissibility. 25
All trials were performed on a commercial vibrating exercise platform (WAVE® Manufacturing Inc, Windsor, ON, Canada) that generated vertical vibration. Participants were exposed to vibration at selected frequencies, 20, 25, 30, 35, 40, 45, and 50 Hz, at a nominal 1 mm displacement amplitude. Pilot testing validated the frequency output of the platform to the nominal frequency setting by calculating the frequency from time domain data. Each trial lasted 30 s and a 2-minute rest period was provided between each experimental trial to minimize muscular fatigue. The sequence of the different vibration frequency trials was randomized using a random number generator with a pick without replacement scheme to ensure that confounding factors of learning effect and fatigue did not affect the experimental outcomes.
Dynamic Squat Exercise
To investigate the effects of dynamic lower extremity movement on vibration transmissibility, participants performed dynamic squats through a knee angle range of 0°-40°. This range was selected to reflect commonly used KFAs reported in WBVE, 9,26 although some studies have assessed deeper squats. 21 The squat was timed to have a 4-second concentric and 4-second eccentric contraction phase of the knee extensors. This controlled the angular velocity of the flexion and extension phases of each squat. Participants were provided with sport socks to wear during testing and performed the experiment unshod as variations in footwear have different dampening properties. 27 Participants were instructed to position their feet shoulder width apart and maintain equal weight distribution between both feet. Each participant’s stance width was measured and marked off on the platform to ensure that they remained in the same position across all trials. There is some evidence that changes in stance width and feet position can affect transmissibility. 28 To ensure that their feet did not slip or move during testing, sand paper was secured to the surface of the platform using double-sided tape.
A video camera (HDR-XR550; Sony, Tokyo, Japan) was positioned 4-m away from the vibration platform to capture real-time sagittal plane images of the participant (Figure 1A), which were displayed on a monitor that was positioned in front of the vibration platform in the participant’s field of view (Figure 1B). Participants were instructed to maintain an upright and erect upper body posture and keep their gaze on the video monitor during each experimental trial. A piece of acetate was taped over the screen and their upper body posture was drawn on with marker.

A, Sagittal plane view of a participant standing on the synchronous vertical whole-body vibration platform. B, Illustration of the postural feedback presented to the participant during testing. Video monitor (i) presents whole-body posture to the participant, while the computer monitor (ii) provides knee angle feedback from the electro-goniometer.
Knee angle data were displayed on a second video monitor, also made visible to the participant, to provide updated feedback about their degree of knee flexion (Figure 1B). This feedback provided the participant with the necessary timing of their dynamic squat. Trials were repeated if the participant had to grasp the machine to maintain balance, lost their footing noticeably from their original position, or if the participant did not perform a trial in the prescribed manner.
Instrumentation
A tri-axial piezoelectric accelerometer (20 × 26 × 20 mm3, total mass = 20 g; Model# 356B08 PCB Piezotronics; Depew, New York) was magnetically attached to the center of the top surface of the platform to measure platform acceleration. Head accelerations were measured using a triaxial accelerometer (15 × 8 × 15 mm3; total mass = 4 g; + 2g peak acceleration; Model#7523A1; Dytran Instruments Inc., St. Chatsworth, California) attached to a head piece created from the liner of a safety helmet. The accelerometer was positioned atop the approximate center of the participant’s frontal bone (forehead). The headpiece used a ratcheting mechanism to tighten the headpiece around the head. The strap and accelerometer had a combined mass of 98 g. This method has lower intra-subject variability over the bite bar method. 29 An electrogoniometer (Model#SG150 Biometrics; Penny and Giles Inc, Santa Monica, California) was taped to the lateral aspect of the right knee of all participants to monitor knee angle. During pilot testing, the electrogoniometer was calibrated against a manual plastic full circle goniometer with 18 cm arms and 1° measurement increments; the largest error across various joint angles was 5°. This measurement setup was also used in a previous publication investigating transmissibility during static squat WBVE. 9
Data Acquisition and Processing
The two accelerometers and goniometer were assembled using a BNC connector (Model BNC-2111; National Instruments; Austin, Texas) and sampled at 2000 Hz using a 16-bit analog-to-digital converter (Model PCI-6221; National Instruments). The raw acceleration data were smoothed using a second-order low-pass Butterworth filter with a cutoff frequency of 120 Hz and the DC offset was removed. Raw knee angle data were smoothed using a second-order low-pass Butterworth filter with a cutoff frequency of 20 Hz. Resultant accelerations were calculated using the root sum square of the X, Y, and Z components. This method was picked to represent the sum of total energy generated at the platform and all measurement locations on the body. The running root-mean-square (rms) value of the signal was calculated using a 500-ms moving window. The amount of energy contained in the vibration is related to the average acceleration, thus rms is most commonly used for quantifying the severity of human vibration exposure. 30 Running rms values at the input (platform surface) and output (head) were used to calculate “instantaneous” transmissibility ratios (Equation 1). 31
One dynamic squat maneuver was extracted for each trial and was subsequently separated into the concentric and eccentric components. The transmissibility data for each of these components were binned into 4 knee joint flexion angle categories: 0° to 10°, 10° to 20°, 20° to 30° and 30° to 40°. The average transmissibility in each of these knee flexion categories was calculated for each participant. All data acquisition and signal processing were performed using a custom written program in LabVIEW (LabVIEW 2012; National Instruments; Austin, Texas).
Statistical Analyses
Statistical analyses were performed using commercial software (SPSS 25; IBM Corp., Armonk, New York). A repeated measures (RM) 3-way ANOVA was used to investigate the interaction of squat exercise phase, vibration frequency, and KFA on platform-to-head transmissibility. Mauchly’s sphericity test was performed, and Greenhouse-Geisser corrections were performed if the assumption of sphericity was violated. Significant interactions were followed up with 2-way and 1-way RM ANOVAs, and post hoc tests with Bonferroni adjustments for multiple comparisons, as appropriate. P < .05 was considered significant for all tests.
Results
The platform-to-head transmissibility changed continuously with KFA as the participants performed the dynamic squat exercise (Figure 2). The vibration was amplified (transmissibility > 1.0) with vibration frequencies of 20 and 25 Hz, for shallow KFAs (<20° at 20 Hz, and <10° at 25 Hz; Figure 3). Intersubject variability was larger at low vibration frequencies and small KFAs (Figure 3).

Platform to head transmissibility during dynamic squats at 30 Hz. The different lines represent the concentric and eccentric squat phases for the individual participants.

Mean (SD) platform-to-head transmissibility as a function of specific ranges of knee flexion angle (KFA): 0° to 10°, 10° to 20°, 20° to 30° and 30° to 40°—at each vibration frequency tested during eccentric (A) and concentric (B) squat phase. A transmissibility value of 1.0 indicates that the amplitude of the vibration is equal at the head and the platform surface.
The assumption of sphericity was not met for the vibration frequency, KFA, and squat phase × KFA interaction (P < .0005, P = .001, P = .008, respectively). Results of the 3-way ANOVA indicated that the 3-way interaction (squat phase × vibration frequency × KFA interaction) was not statistically significant (P = .177). The KFA × vibration frequency 2-way interaction was statistically significant (P < .0005). The other 2-way interactions were not statistically significant (P = .897 and P = .262, for the squat phase × KFA and squat phase × vibration frequency interactions, respectively). The main effect of squat phase was significant (P = .025) with the transmissibility being larger during the concentric phase (average transmissibility = 0.484) than the eccentric phase (average transmissibility = 0.469).
One-way RMs ANOVAs were performed to evaluate transmissibility differences between the 7 vibration frequencies, for each of the KFA ranges, and for the different squat phases. These tests revealed consistent patterns for all of the KFA ranges and squat phases: the transmissibilities were not significantly different between 20 and 25 Hz vibration frequencies, and the transmissibilities were not significantly different between the higher vibration frequencies (e.g., 30-50 Hz for KFA 0°-10° for the concentric phase, and KFA 30°-40° for both the concentric and eccentric phases, and 40-50 Hz for KFA 0°-10° for the eccentric phase).
Discussion
This study measured the transmissibility from a commercially available WBVE platform to the head during controlled dynamic squats across a range of vibration frequencies. We observed that the vibration to the head was amplified (transmissibility > 1.0) for shallow KFAs at vibration frequencies of 20 and 25 Hz and that the vibration amplitudes were attenuated for larger knee angles (>30°). We observed that the head vibrations were attenuated for vibration frequencies between 30 and 50 Hz for all KFAs. Abercromby et al 10 measured head acceleration across varying degrees of knee flexion at 1 vibration condition (30 Hz and 4 mm p-p). They found a linear decrease in rms head acceleration with increasing KFAs from 10° to 30°. Above 30° of knee flexion, they found that the ability of the legs to reduce head acceleration decreased. Our results found a similar reduction in head transmissibility as knee angle increased; however, the reduction was nonlinear for lower frequency vibrations, and we did not see an increase in transmissibility above 30° of knee flexion. Some participants did show peaks in transmissibility as they went through a certain range of knee flexion; however, this was not consistent across all participants. The difference in transmissibility between the eccentric and concentric phases was statistically significant, but small (3.28%) and not considered important relative to the influence of KFA and vibration frequency. Accordingly, the results of the study illustrate that both the eccentric and concentric phases have similar transmissibility across knee angle ranges between 0° and 40°. There is no reason to advocate an individual to use more of the concentric phase versus an eccentric squat during WBVE.
At lower input frequencies (20-30 Hz), smaller KFAs resulted in amplification of mechanical energy at the head. Our findings with dynamic squat exercise are similar to those for static KFAs. 9,32 We found resonance of the head at these knee angles during 20 and 25 Hz platform vibration. Approximately 20° of knee flexion appears to reduce the stiffness of the body and cause a reduction in vibration transmission through the body to the head. Vertical head transmissibility displays multiple peaks between 0.25 and 25 Hz. 15,28 Previous literature has reported that the eyeball resonates around 20 Hz, and disruptions to visual perception have been reported between 20 and 25 Hz. 17 A case report found that individuals with intraocular prostheses can have had spontaneous dislocation after WBVE. 16 This indicates that energy reaching the head during WBVE can be injurious and have detrimental impacts to vision. Platform users should be advised to maintain at least 20° of knee flexion during static and dynamic squats.
Platform to head transmissibility depends strongly on the KFA. Accordingly, it is important that research using WBVE should control KFA during static and dynamic squats and should report the ranges of knee flexion. While some investigations report KFAs, 5,18 –20 unfortunately many do not report these details. 1,4,7,21,22,33 –36 Our findings show that the platform vibrations can be attenuated or amplified as they are transmitted through the skeleton, and the KFA is an important parameter that should be controlled and reported.
At frequencies of 40 Hz and higher, acceleration values at the head remained below 50% that of the platform across all KFAs. Frequencies above 30 Hz may be the safest for WBVE as at these frequencies the vibration is localized primarily to the lower extremity. 11 These frequencies, used in previous training studies, lead to documented changes in muscle activation 20 and muscular strength 5,6,21 but may not be anabolic to the skeletal system. 8,37
We observed greater intersubject variability at low frequencies (20-25 Hz) and smaller knee angles (<20°). These findings are likely related to differences in the segment resonant frequencies between individuals, 28 differences in shock-absorbing capacity between individuals, 38 as well as the large influence of differences in posture. 15
This investigation was limited to evaluating dynamic squats during WBVE. This work complements our previous reports of static squat exercises; 9 we have previously reported measures of vibration transmissibility to the head during static squat exercises at KFAs of 0°, 20°, and 40°, using 7 platform vibration frequencies between 20 and 50 Hz, and at two peak-to-peak displacement settings (1 and 2 mm nominal). While other studies have measured vibration transmission to other parts of the skeleton, such as the hip and spine, 39 and the ankle, knee, hip, and spine, 11 we have focused on transmission to the head. We observed that mechanical vibration can be amplified as it is transmitted through the skeleton and that knee flexion is an important factor for limiting the amount of vibration energy reaching the head. We have not evaluated exercises involving vibration passed to the body while sitting on the platform (eg, abdominal crunches or sit-ups), 6 sitting off the platform with feet on the platform, 40,41 placing hands on the vibration platform (eg, planks or push-ups), 5,6,42 –44 or performing bicep curls and tricep extensions holding nylon straps attached to the vibration platform. 45 We advocate caution as these postures may result in excessive vibration energy reaching the head as the vibration is transmitted to the upper body, bypassing the knees and the vibration attenuation that knee flexion provides.
Conclusions
This study found that the response to dynamic exercise is similar to static postures: transmission of vibration to the head is reduced with KFAs greater than 20°. This finding is consistent with previous research that larger knee angles should be advocated when using WBVE platforms, 11 especially at frequencies below 30 Hz where resonance of the head is likely. There do not appear to be large difference in transmissibility between the eccentric and concentric phases of the squat. Our results add further evidence that the head has a natural frequency between 20 and 30 Hz, and this frequency value may vary between individuals and the posture adopted. Since excessive vibration energy may have a detrimental effect on the visual, 16,17 auditory, 46 and vestibular systems, 47 these frequencies should be avoided.
Footnotes
Acknowledgments
The authors acknowledge the commitment of the research participants, and WAVE Manufacturing Inc. for loaning the vibration platform used in this study.
Declaration of Conflicting Interests
The author(s) declared no potential conflicts of interest with respect to the research, authorship, and/or publication of this article.
Funding
The author(s) disclosed receipt of the following financial support for the research, authorship, and/or publication of this article: This research was funded by a discovery grant from the Natural Sciences and Engineering Research Council of Canada [RGPIN-2016-05187], and scientific instrumentation was funded by an infrastructure grant from the Canadian Foundation for Innovation [CFI number 23521]. Robert Caryn was supported by a scholarship at Western University.
