Development of the Rope-Climbing Ergometer for Physical Training and Testing.

The purpose of this study was to develop and characterize a rope-climbing ergometer. A custom-made loading device that has an eddy current brake with an electrical current control circuit was developed to impose resistive load on the rope. A calibration test was first performed using a three-phase induction motor to associate the scale of the load-level setting (100 levels) with the resultant traction force. The calibration test yielded criteria values of loads (123 N at Level 0 and 1064 N at Level 100). The human test was carried out by 14 male subjects. The participants performed eight sets of 10-second maximal-effort exercises at different levels. Presumable trajectories of force, velocity, and power were obtained. The mean force increased by 161% (from 147.5 N at Level 0 to 383.7 N at Level 18), whereas the mean velocity decreased by 64.7% (from 1.87 m/s at Level 0 to 0.66 m/s at Level 18). The mean power reached its peak at Level 9 (320 W). The new rope ergometer for physical training and testing was successfully developed and characterized in this study. However, it remains to be seen whether its concurrent validity and reliability are qualifiable.

Introduction

Training, measurement, and evaluation of physical fitness, including strength, power, endurance, and flexibility are fundamental for athletes seeking to improve their performance. To assess aerobic and anaerobic capabilities, many practitioners and researchers have used cycle ergometry 2 11 16 29 . Ergometer measurements are typically performed in a laboratory instead of in field tests, allowing for precise quantification of the mechanical output with discretional choice of measuring protocols. Owing to these advantages, many studies have used ergometers to evaluate physiological characteristics and indices, such as the force-velocity relationship of muscle 12 28 , maximum anaerobic power 4 10 30 , anaerobic capacity 17 , and maximum oxygen consumption 3 . Treadmills are also preferred by many technicians and researchers, because running recruits a larger active muscle mass with greater maximum oxygen consumption 3 . Nonetheless, the treadmill running tests need specialized biomechanical analyses to accurately quantify the mechanical work done by subject’s lower limbs 18 . In this respect, ergometer tests allow for direct measurements of the load and offer significant advantages for calculating the true work in a way that the treadmill cannot 11 . For decades, many athletes and researchers have benefited from ergometry to evaluate physical fitness in athletes.

The ergometer methodology can be subdivided into various modes. The traditional cycle ergometer is most commonly used. It recruits a relatively large amount of muscle around the lower limbs and can elicit a large magnitude of power output 11 30 . Validity and reproducibility of cycle ergometers have also been confirmed in previous studies 4 6 23 24 29 . Other methods have also been developed to duplicate specific conditions of each sport and approximate muscles that are involved 8 22 25 26 27 , including an arm-cranking ergometer 7 and a rowing ergometer 5 13 17 19 30 . The ergometer test for physical fitness includes a variety of movements. To our knowledge, no gold standard has been established for upper limb exercise similar to the cycle ergometer for lower limbs. Further ingenious developments of laboratory ergometer methodologies for the upper body will increase options for physical measurement and evaluation of near-competitive conditions for a specific sport.

In this study, we developed a rope-climbing ergometer (rope ergometer) to assess and train subjects to pull using their upper limbs. Although a commercially available rope-climbing device already exists (VLT Rope Trainer, Marpo Kinetics, Livermore, CA, USA), it does not have a computerized measuring system equivalent to the ergometer. The movement pattern when an athlete is exercising with this device is similar to the cyclic (repetitive) action of running and cycling, suggesting its potential as an ergometer for tests of explosive, high-intensity, and endurance-intensity efforts. The purpose of this study was to develop and characterize a rope-climbing ergometer that ensures the logical validity of measurements.

Methods

The rope-climbing ergometer

The overview and specifications of the rope ergometer developed in this study are represented in Fig. 1 2 and Table 1 , respectively. Our ergometer resembles the commercially available rope-training device (VLT Rope Trainer, Marpo Kinetics, Livermore, CA, USA) in terms of appearance and subject’s motion. The difference is that the device has a comprehensive system for measurement that is characteristic of ergometers.

Fig. 1

Snapshot of the rope ergometer with a subject.

Fig. 2

Schematic overview of the custom-made loading system (Apowatec, Apowatec Corporation). This loading system involves an eddy current brake (ECB), which is regulated by an electrical current control circuit (ECCC). The intensity of the impressed current is controlled by a microcomputer (H-8, Renesas Electronics) and an operating computer. To configure the detailed programs for measurements and to display the summary of results, custom-made application software was developed and installed on the operating computer.

Table 1 Schematic specifications of the rope ergometer developed in this study.

Items	Specifications
Size	Length: 2 000 mm, width: 1 000 mm, height: 2 300 mm
	Mass: Roughly 100 kg
Structure	Main body: Rectangular steel tube (STKR400)
	Flooring: Slip-resistant rubber
	Cushions: PVC leather with cushioning materials on ply board
	Rope: Polyester synthetic fiber (‘Tetoron’, Toray), φ 30 mm
Loading System	Braking device: Eddy current brake
	Control unit: Constant current control circuit
	Regulation: Pulse-width modulation by a microcomputer (H-8 Renesas Electronics) and an inverter
Measuring System	Tension: Tension gauge (LC-1205-K500, A & D)
	Velocity: Circular encoder (E6A2-CW3C 360P/R 0.5M, OMRON)
Settings of Exercise Protocols	Load level: 100 stages (optional)
	Duration of each set: Optional
	Interval duration between each set: Optional
	Number of sets: Optional
Display Items on PC Application	Lapsed time (up to 999 min and 59.9 s with 0.1 s of resolution)
	Instant distance (up to 999.9 m with 0.1 m of resolution)
	Instant traction Force (up to 200.0 kgf with 0.1 kgf of resolution)
	Instant traction velocity (up to 4.00 m/s with 0.01 m/s of resolution)
	Instant power (up to 9999 W with 1 W of resolution)
	Instant work (up to 9999 J with 1 J of resolution)
Output of Data	As a csv file in the operating computer

* The rope material may warrant reconsideration. In this study, polyester was used because of its cost and durability advantages. On the other hand, the features of hemp or polyamide are expected to allow climbing without the hands sliding, which is not the case for polyester. This issue is to be reconsidered in later studies.

A custom-made loading system (Apowatec, Apowatec Corporation, Yashio, Japan; Fig. 2 ) was developed to a attain rigorously controlled resistive load on the rope. This loading system involves an eddy current brake (ECB), which is regulated by an electrical current control circuit (ECCC). In this system, the resistive torque can be generated in parallel with the magnitude of the impressed current in the ECCC. This torque is augmented by gears (gear ratio, 0.352) and transmitted to the pulley as resistive tension via the rope. The intensity of the impressed current is controlled by a microcomputer (H-8, Renesas Electronics, Tokyo, Japan) and an operating computer ( Fig. 2 ). To configure the detailed programs for measurements and to display the summary of results, custom-made application software was developed and installed on the operating computer. Any operation and data output were handled with this application.

The load-level settings consisted of 100 stages, and the axis was converted from an inverse logarithmic scale of the impressed current in the circuit, as follows:

Current·C=log Level (Level=exp(Current·C))

Current represents the impressed current in the ECCC, Level represents the stage of the load-level setting, and C is a constant representing the relationship between Current and Level . Both the number of stages (100) and C (0.141) can be discretionarily configured by users by modifying the application software on the computer. The relationships between the traction force loaded on the rope and both Current and Level are described below.

The instant traction force and velocity of the rope were measured using a tension gauge (LC-1205-K500, A and D) and circular encoder (E6A2-CW3C 360P/R 0.5M, OMRON). The tension gauge is located on the overhead pulley and directly detects the sum tension on the rope. Half of the tension measured by the gauge was defined as the instant traction force ( F ins ) [N]:

F ins =F gauge /2

where F gauge [N] represents the instant tensile force directly measured by the tension gauge. The instant velocity ( V ins ) [m/s] was then calculated based on each elapsed time ( T elapsed ) [s], which is recorded by the circular encoder:

V ins =D / T elapsed

D=0.547 [m]

where D is the distance between the landmarks that the rotary encoder detects. The data taken by the tension gauge and the circular encoder were transmitted to the microcomputer (sampling frequency is 100 Hz) and then read into the operating computer with the application. The application has a simultaneous display function that represents the mechanical variables regarding the exercising information ( Fig. 2 ). The data were exported from the computer in a .csv format and forwarded for further analysis.

Calibration test with a three-phase induction motor

Before the tests, we performed a calibration test to associate the scale of both Level and Current with the resultant traction force loaded on the rope. In the calibration test, a three-phase induction motor (maximum output power: 1.5 kW, G3LM-32-15-150, NISSEI) was used to pull the rope at constant speeds. The motor, which is virtually equivalent to a real human user, was fixed where the rope was on a pulley attached to the motor. Four sets of tests were examined at different pulling velocities (0.25 m/s, 0.50 m/s, 0.75 m/s, and 1.00 m/s). It should be noted that the instant traction force fluctuates unintentionally from the acceleration of the rope even at the same load levels. In other words, the traction force stays fixed only when the rope is pulled at a constant speed, which is why this calibration test was conducted at the constant velocities using the induction motor.

Fig. 3a describes the relationship between the Current and the resultant resistive forces at given pulling velocities. As depicted, the resistive forces at the identical Current tended to gradually become larger nonlinearly with increasing velocity. Importantly, the increments in the resistive forces progressively diminished with the gradual increase in velocity. When comparing the resistive forces at the identical Current , they approximately reached a ceiling above the velocity of 0.50 m/s. Therefore, it can safely be said that the resistive force at a given Current reached equilibrium at approximately 0.75 m/s. The force- Current relation (when the velocity=0.75 m/s) was fitted to a quadratic function. As shown, the relationship was well described (r 2 =1.00) with the quadratic equation below:

Fig. 3

The results of the calibration test with a three-phase induction motor. a The relationship between the Current and the resultant resistive forces at given pulling velocities. As depicted, the resistive forces at the identical Current tended to gradually become larger nonlinearly with increasing velocity. b The relationship between the Level and the resultant resistive forces when the velocity=0.75 m/s. In this figure, the axis of Level was converted from an inverted logarithmic scale of Current.

F 0.75 =a 1 *Current 2 +a 2 *Current+a 3

where F 0.75 is the resistive force when the pulling velocity was set at 0.75 m/s, and a 1 , a 2 , a 3 represent constants, respectively (a 1 =0.0059, a 2 =−0.1392, a 3 =129.81).

Fig. 3b represents the plots of the F 0.75 as a function of the Level ; 123 N of resistive force was observed when the Level was set at the minimum (i. e., Level =0). With the increment of the Level , F 0.75 increased approximately linearly. The force- Level relation (velocity=0.75 m/s) was fitted to a linear function with a moderately fitted regression line (r 2 =0.99) as shown below:

F 0.75 =b 1 *Level+b 2

where b 1 and b 2 represent constants, respectively (b 1 =9.8603, b 2 =61.257). It should be also noted that each constant (a 1 , a 2 , a 3 , b 1 , and b 2 ) can be forced to change when C is discretionally modified by adjusting the software.

The tests by subjects

Fourteen healthy, injury-free males participated in the experiment. All participants were active individuals but not ongoing competitive athletes. Their mean (±SD) age, height, and body mass were 32.6±6.0 years, 1.738±0.049 m, and 74.9±12.7 kg, respectively. All participants refrained from intense activities on the previous day to prevent unintentional fatigue during the tests. Informed consent was obtained from all participants after explaining the purpose and design of the study. This experiment was approved by the Ethics Committee of the Japan Institute of Sports Sciences and meets the ethical standards of the journal 15 .

The participants performed eight sets of maximal-effort rope-climbing trials. Based on previously reported load-power relationships 1 10 20 , we varied the Level s (0, 3, 6, 9, 12, 15, 18, and 21, respectively). The exercise duration was configured for 10 s at Level ≤9, and 7 s at Level >12, to avoid an excess fatigue. Eight sets of trials were performed in a random order to offset the order effect, with at least a 10-minute rest period between each successive trial.

Each participant performed light aerobic exercises with the rope ergometer and stretches of muscles relevant to the pulling exercise to warm up before the tests. The trials were carried out in a sitting posture on the seat of the ergometer. The participant’s thighs were tightly secured against a pad to keep their body stationary during exercise. The subjects raised their hands above the head and firmly gripped the rope before the beginning of the tests. It was optional how the subjects configured their posture in particular. All operations concerning the machinery and verbal cues including countdown were given by the assessors.

We analyzed the data exported to the computer. The time of the force and velocity were smoothed with a nine-sample simple moving average process, and then the instant power was calculated. In the pilot experiment, the time-course data of force and power contained cyclically spiked waveforms, probably because of the changeovers of the right and left hands (e. g., Fig. 4 ), which the moving average process failed to remove. Consequently, data from each time course were used to evaluate a peak value 4 and averaged for three seconds (from two seconds after the initial moment) for each trial. This time period was based on the qualitative observations of the data from each time course throughout the Level s in the pilot experiment.

Fig. 4

Typical examples of time series trajectories of force, velocity ( a and c ), and power ( b and d ), when Level was set relatively low (Level 3, a and b ) and high (Level 15, c and d ), respectively. These data are chosen from a single subject.

Comparisons of force, velocity, and power between the Level s were performed through one-way repeated-measures ANOVAs with Bonferroni-adjusted pairwise post-hoc analyses. The significance level was set at P <0.05. All statistical analyses were performed using R Statistical Software (version 3.3.3; R Foundation for Statistical Computing, Vienna, Austria).

Results

Typical examples of time series trajectories of the force, the velocity, and the power are shown in Fig. 4 . These data are chosen from a single subject. We observed cyclically spiked waveforms of force and power for every trial and subject ( Fig. 4 ), presumably due to transitions between the right and left hands. The frequency of these spikes was relatively higher in the trials with low load levels ( Fig. 4a,b ), and decreased with increasing load levels ( Fig. 4c,d ). The length of time spent to achieve peak velocity ranged from two to four seconds after onset regardless of the Level ( Fig. 4a,c ). The peak values for the trajectory of force were found immediately after onsets ( Fig. 4a,c ), and its relative size compared with the subsequent force tended to be larger when the Level was low ( Fig. 4a ). We were unable to discern the exact time required for the peak force and power because of the influence of the spike noises.

The time series for the force, velocity, and power were averaged between two and five seconds after onsets for all the load levels, and plotted on Fig. 5a,b . The one-way ANOVA indicated that there were significant differences between the Level s in all of these three variables ( p <0.01 in force and velocity and p <0.05 in power). Regarding the comparisons between adjacent Level s, the post-hoc analyses indicated that significant differences were observed between Level 12 vs. 15 ( p <0.01) and 15 vs. 18 ( p <0.01) in force, between 9 vs. 12 ( p <0.01), 12 vs. 15 ( p <0.01), and 15 vs. 18 ( p <0.01) in velocity, and 15 vs. 18 ( p <0.01) in power ( Fig. 5a,b ). As a function of Level , the mean force increased by 161% on average (from 148±41 N at Level 0, to 384±26 N at Level 18), whereas the mean velocity decreased by 64.7% (from 1.87±0.23 m/s at Level 0, to 0.66±0.20 m/s at Level 18). Magnitudes of the increments of force and the decrements of velocity with increasing Level tended to be smaller at lower Levels , and became larger at higher Level s ( Fig. 5a ). The mean power reached its peak at Level 9 (320±123 W: Level 9), although the post-hoc comparison indicated that there were no significant differences of powers between adjacent Level s (p>0.05 between Level 8 vs. Level 9 and between Level 9 vs. Level 10).

Fig. 5

Averaged forces ( a ), velocities ( a ), and powers ( b ) as functions of Level for 14 subjects. These plots are the mean values between two and five seconds after onset of exercises. In a , the results of force in the calibration test (0.75 m/s) were also plotted for comparison between the calibration and the human tests.

Discussion

In this study, we developed the new rope climbing ergometer and provided a mechanical characterization of its device. To our knowledge, our rope ergometer is the first that combines the rope-climbing exercise with the function of an ergometer. This device has a potential for use in physical training and evaluation of the upper limbs, particularly focusing on muscles relevant to the pulling movement.

The most elaborate component of our ergometer is the loading system (Apowatec, Apowatec Corporation, Yashio, Japan). Existing ergometers include various loading devices 6 , such as the ECB (PowerMax V3 Series, Combi Wellness Corporation, Tokyo, Japan), and friction-based loading (Monark Series, Monark Exercise AB, Vansbro, Sweden). In our study, the ECB was adopted because it has an advantage in strictness and easiness of load adjustment. The rope ergometer has provided for the arbitrary control of the Level by handling the computer, offering a user-friendly equivalent to the existing commercial ergometers such as the PowerMax V3 series. This indicates that the present ergometer is suitable to assess peak power, considering the load-power (as well as the force-velocity) relations of muscle 1 9 28 . In addition, our device allows for the detailed organization of measuring protocols including Level s, durations, sets, intervals, and combinations. These functional capabilities suggest the potential applicability of the present rope ergometer to both practical situations of training and testing and to laboratory tests.

The present rope ergometer quantifies the mechanical outputs (i. e., force and velocity) based on the actual observations using the tension gauge (located on the overhead pulley) and the circular encoder (placed inside the main unit), respectively ( Fig. 2 ). It is reasonable to suppose that there is no room for substantial error in these mechanical variables, because no interfering factors exist in these measurements and calculations. With regard to the other factors that might cause possible error, the hardware side of the rope ergometer should be taken into consideration. In particular, mechanical friction originating from the rope, pulleys, and gears is assumed to influence the results of the traction force measurement. Yet the estimated values of force and velocity are assumed to be acceptably accurate, because in the present ergometer the tension gauge and the circular encoder directly evaluate the measured values exerted by a subject, and hence the measuring processes are independent of the ergometer hardware. Nevertheless, it should be noted that this study lacks the examination of concurrent validity and reliability. Therefore in the future, it remains to be seen whether the ergometer’s validity, reliability, and sensitivity are qualifiable as a tool for measuring the power of the upper limbs 24 .

In this study, the calibration test was conducted with a three-phase induction motor to associate the scales of Level and Current with the resultant traction force. In this regard, we should mention that there was a considerable difference in the observed traction forces between the subject test and the calibration test ( Fig. 5a ), even when the Level was identical. In particular, the traction forces observed in the subject test resulted in larger values than those observed in the calibration test when the Level was set relatively higher (e. g., the former was 313±36 N vs. the latter was 218 N at Level 15, and 384±26 N vs. 238 N at Level 18). Supposedly, the magnitudes of the traction force observed in the two tests ought to unambiguously correspond to each other regardless of the Level setting, provided the velocity of the rope is constant (the filled plots in Fig. 5a were supposed to overlap Fig. 3b ). The factor that caused the gap between the two tests (i. e., the subject test and the calibration test) would be the effect of acceleration of the rope, because the acceleration instantly boosts the Current and thus the load on subjects. In the case of the subject test, inevitable acceleration and deceleration of the rope occur during use, largely because of the cyclic replacement of right and left hands. These fluctuations in the velocity of the rope would result in the increase in traction force in the case of the subject test, whereas the rope velocity was mechanically kept constant in the calibration test, which used the motor. In addition, it should also be noted that the gap in the traction forces became greater with the increment in the load levels. This is probably because the load level was so intense at Levels 15 and 18 that the subjects changed the manner of pulling, such as suspending their upper body from the rope, thus resulting in the conspicuous fluctuation in velocity. In light of these results, when using this ergometer at higher Level settings, it should be noted that actual traction force applied to the subject becomes larger nonlinearly.

In the subject test, the peak power resulted in 320±123 W ( Level =9, Fig. 5b ) on average. This magnitude is smaller than those of the preceding studies that used the cycle 20 and the rowing 17 ergometers. Regarding cycle ergometry, an interpolating calculation with regression formulae has been generally used to estimate the peak power over various loads. With the use of this calculation, the peak power with the cycle ergometer was recorded around 930 W for adult male non-athletic subjects 20 and up to 1 600 W for male elite cyclists 10 . As for the rowing ergometer, Klasnja et al. (2010) reported that 522 W of peak power was observed for male rowers 17 . A presumable rationale for the smaller peak power with the present ergometer is the total volume of muscles involved in the pulling exercise. Namely, with the rope ergometer, muscles of the upper limbs and some trunk muscles are assumed to be mainly recruited, whereas muscles of the lower limbs, which are comparatively large in volume, are involved in exercises with the cycle and the rowing ergometers. Nonetheless we ought not to get into further discussion on this issue, because none of the biomechanical and electromyographic measurements were included in this study. These measurements remain to be investigated in future studies.

Meanwhile, the present results should also be compared with those of the arm cranking ergometer, which like the present rope ergometer, mainly engages muscles of upper limbs and some part of trunk. Indeed, Flueck et al. (2015) applied an arm cranking ergometer to non-athletic individuals in a sitting posture, and observed that the peak power was from 312 W to 334 W 14 , indicating a value close to that of the present study. On the other hand, Neville et al. (2010) observed the peak power (up to 1347 W) to be four times greater than in the present study 21 . It should be noted that there are two fundamental differences between Neville et al. (2010) and the present study; in the preceding study, the participants were professional yacht racers and the tests were carried out with participants in a standing position 21 . Concerning the rope ergometer, it is highly likely that the magnitudes of peak power would change with variations in the testing conditions (e. g., profiles of subjects and testing posture). This issue will become apparent with practical use.

Conclusions

We developed and characterized the new rope-climbing ergometer in this study. This new device has a potential for use in the physical training and testing of upper limbs. However, future study is warranted to verify whether its concurrent validity, reliability, and sensitivity are qualifiable as a tool for measuring power.