1. Introduction
The practice of road cycling is often associated with low levels of comfort for the cyclist and can be a physically painful experience on bad roads. It can also be linked to increased health risks such as handlebar palsy caused by the compression of the ulnar nerve [
1], and the potential onset of erectile dysfunction caused by compression of the pudendal nerve [
2]. In that regard, reducing road induced vibration transmitted to the cyclist is an important consideration, and has been an increasingly active research field since the early 2000’s. Many studies have been undertaken to assess and understand road bicycle dynamic comfort, which relates to the capacity of a road bicycle to filter the vibration generated by the road surface, and this must be distinguished from static comfort, which relates to the bicycle’s size with respect to the size and shape of the cyclist. A range of test protocols and test rigs have been developed that mimic the excitation of a road surface [
3,
4,
5,
6], and transducers have commonly been used around the bicycle, e.g., in the seatpost, handlebar, stem, and brake hoods in order to measure the acceleration, force, power, and energy transmitted to the cyclist [
7,
8,
9,
10]. An assessment of the ability of bicycles, bicycle components, and cycling apparel to filter vibration has also been conducted [
3,
5,
10,
11,
12], while cyclists’ vibration perceptual thresholds have been determined using psychophysical approaches [
13,
14].
Apart from cushioning in the saddle, applying handlebar tape, or reducing tyre pressure, a road bicycle offers in itself few options for comfort improvement, as it is primarily designed for performance, with emphasis on low mass and high stiffness, and typically is not equipped with suspension components, as is the case for other types of bicycles (e.g., full suspension mountain bike). However, a range of components exist (e.g., suspension stems and seatposts) that can be fitted to a road bicycle, which can potentially improve comfort with only a limited increase in mass.
In this context, the aim of this study was to assess the effectiveness of suspension stems in reducing the vibration transmitted to a cyclist’s hands in the case of impact load excitation at the front wheel. We chose to use impact loads as it was thought that these would provide a more measurable difference between test conditions than random-type excitation (i.e., excitation related to road surface roughness). The vibrational energy transmitted at a cyclist’s hands was used for this assessment, as in previous studies for impact load excitation [
12,
14].
2. Materials and Methods
Three 90 mm road bicycle stems were tested in this study (
Figure 1), namely: (1) a Kalloy Uno 7 stem (Model ASA105, Kalloy Industrial, Taiwan), (2) a TranzX ANTISHOCK suspension stem (model JD-ST146A.2, JD Components Co., Ltd., Taiwan), and (3) a Redshift ShockStop suspension stem (model RS-40-01, RedShift Sports, Philadelphia, PA, USA). The technical data for the three stems are given in
Table 1. The suspensions stems were selected for testing in this study because they were deemed the two most suitable suspension stems for road bike application. The Kalloy Uno 7 stem is a regular stem (i.e., not a suspension stem), and this was used as the reference stem in this study. Both suspension stems are made of two main articulated parts that rotate relatively to one another about a horizontal axis (i.e.,
a–
a axis in
Figure 1b,c). One of these parts is attached to the fork steerer tube and the other is attached to the handlebar. An elastomer component is inserted between them, providing compliance and damping to the system. The elastomer component for the Redshift ShockStop stem is interchangeable, and, in this study, was selected to match the cyclist’s mass according to the manufacturer’s guidelines. The elastomer component for the TranzX ANTISHOCK stem is not interchangeable.
Tests were carried out using a bicycle treadmill (
Figure 2a) and a Cervélo R3 carbon fibre road bicycle (size: 56 cm; tyre: Continental Grand Prix 4000s II—700×23C; pressure: 800 kPa). The treadmill platform was 76 cm wide by 196 cm long, and allowed for ample freedom of movement for cycling. The rear wheel was placed on a raiser board and was thus not touching the treadmill belt. Impact load excitation at the front wheel was provided using a circular aluminium dowel of 15.7 mm in diameter, attached to the treadmill belt. The bicycle and the cyclist were kept vertically stable with an elastic rope wrapped around the seat tube and attached to a fixed structure on each side of the treadmill. The elastic rope was selected to be compliant enough in the vertical direction in order to make sure it did not affect the bicycle’s dynamics in that direction.
The vertical force and acceleration transmitted to the cyclist’s hands were measured with a strain gauge instrumented brake hood [
10] and a PCB 352C68 uniaxial accelerometer under the hands (
Figure 2b). Each instrumented brake hood was composed of two main parts bolted together—the hand rest and the instrumented body equipped with strain gauges in a full Wheatstone bridge configuration. The instrumented brake hoods were statically and dynamically calibrated for transmitted power measurements at a cyclist’s hands [
15]. Because of their high stiffness, their deflection in the
x–
z plane did not introduce any significant inclination of the measurement axis relative to the
z axis (i.e., <0.05
° at maximum load), and therefore did not impair the force and acceleration measurements along that axis. The force and acceleration signals were collected using a LMS SCADAS 24-bit acquisition system (model SCR01-08B) at a sampling frequency of 8192 Hz. LMS Test.Lab software was used for the data processing. The instantaneous power transmitted to the cyclist’s hands,
P, was calculated using Equation (1), where
F and
v are the instantaneous vertical force and speed, respectively (obtained by integrating the acceleration signal).
The energy transmitted to the cyclist’s hands,
E, for each impact was calculated using Equation (2).
An experienced male cyclist (age: 49 years old; height: 180 cm; mass: 77 kg) was seated on the bicycle during the measurements. The bicycle was properly adjusted to achieve an adequate body position. The cyclist kept a natural constant position on the bicycle with his hands on the instrumented brake hoods with no grip force. He remained seated at all times and did not pedal. The bicycle cranks were fixed in a horizontal position.
Three runs of 20 impacts per stem were carried out for a total 60 impacts per stem. The order of the runs was randomised across the stems. For each stem, the average total (i.e., left hand (LH) and right hand (RH) combined) transmitted energy,
, was calculated using Equation (3).
where
and
are the transmitted energy measured by the left and right instrumented brake hoods, respectively, for the
ith impact.
For comparison purposes, using the same methodology, the average total transmitted energy was also assessed for the front tyre pressure, ranging from 300 to 800 kPa with 100 kPa increments. This assessment was carried out for the Kalloy Uno 7 stem only.
4. Discussion
The results show an important reduction in vibrational energy transmitted to the cyclist’s hands when using the suspension stems compared with the regular stem (i.e., Kalloy Uno 7 stem). Indeed, as disclosed in
Table 2, the transmitted energy was reduced by 18.9% when using the TranzX ANTISHOCK stem, and was almost halved (−45.8%) when using the Redshift ShockStop stem. In the tested conditions, the Redshift ShockStop stem was therefore found to be more than twice as efficient in reducing transmitted energy than the TranzX ANTISHOCK stem. The reduction in transmitted energy obtained with the suspension stems is also much more important than the one obtained in a previous study in similar test conditions when using cycling gloves or handlebar tape. In that study, the reduction in transmitted energy was at most (i.e., when gloves and handlebar tape were used together) 8.3% [
14].
Figure 3b allows us to relate the reduction in transmitted energy to the cyclist’s hands using the instrumented stems to a change in front tyre pressure, which will yield a similar reduction in transmitted energy. This comparison is meaningful to cyclists, as tyre pressure has a direct effect on their perception of bicycle comfort [
11]. Tyre pressure is also a parameter that cyclists are likely to have made adjustments to in an attempt to improve comfort or performance, and reducing tyre pressure is the quickest way to reduce transmitted energy to the cyclist—thereby increasing comfort. However, there is a potential trade-off between tyre pressure and other considerations, such as the rolling resistance.
Figure 3b shows that in order to obtain a reduction in transmitted energy comparable to that obtained with the TranzX ANTISHOCK and Redshift ShockStop stems (compared to the regular stem), a deflation of the front tyre from 800 kPa (or 116 psi) to ~700 kPa (or ~102 psi) and ~550 kPa (or ~78 psi), respectively, would be required. So, the suspension stems allow for a reduction of transmitted energy associated with deflating the front tyre somewhere between 100 and 250 kPa (depending on the stem), without having to compromise on other considerations related to tyre pressure selection.
The measured reduction in transmitted energy associated with both suspension stems (i.e., 383 mJ and 928 mJ for the TranzX ANTISHOCK stem and the Redshift ShockStop stem, respectively) was vastly higher than the 100 mJ perceptual threshold determined in a previous study involving 10 participants and carried out in similar test conditions [
12]. It is therefore expected that cyclists will perceive an improvement in comfort when using the tested suspension stems. However, the added comfort provided by these stems comes at the expense of the mass of this component, due to their increased mechanical complexity. The suspension stems were 1.9 and 2.6 times heavier (for the TranzX ANTISHOCK stem and the Redshift ShockStop stem, respectively) than the regular stem, which, in absolute terms, correspond to mass increases of 89 g and 168 g, respectively, when compared to the regular stem (103 g). This should be an area for further study, focusing on how the increase in mass and other properties (e.g., stiffness and damping characteristics) of suspension stems affect the amount of energy transmitted to the cyclist.