1 Introduction

At racing speeds of about 40 km/h, the aerodynamic resistance or drag of a cyclist is about 90% of the total resistance [1,2,3]. Therefore many efforts in professional cycling and in cycling research are focused on the reduction of the cyclist’s drag. Especially in the past two decades, scientific research in cycling aerodynamics has rapidly increased as reported in recent review papers [4, 5]. Recent research has focused on the factors determining the aerodynamic resistance, including different cyclist positions (e.g. [6,7,8,9,10,11]) and the associated flow topologies [12,13,14], the bicycle and bicycle components [5, 15,16,17], wearable equipment such as helmets (e.g. [18, 19]) and the interaction between drafting cyclists [20,21,22,23,24,25]. Together with previous studies, these efforts have led to more and better insights in the aerodynamics of cycling.

Less attention however has been given to the aerodynamic interaction between cyclists and in-race vehicles. Cycling races contain a multitude of cars and motorcycles. The latter are present for various purposes: neutral support, commissaire activities, traffic managing, information provision, doctor and police duties and press, where the latter can be camera, sound or photographer crews. While cars generally stay behind the cyclists, motorcycles are allowed to maneuver in the proximity of the cyclists when filming or recording, and filming is only forbidden in the last 500 m of the race. Blocken and Toparlar [26] demonstrated that a team car following a cyclist can yield a drag reduction for the cyclist of 3.7, 1.4 and 0.2% for separation distances of 3, 5 and 10 m, respectively. Blocken et al. [27] assessed that a motorcycle following a cyclist can provide a drag reduction for the cyclist of 3.8, 0.3 and 0.1% for separation distances of 1, 5 and 10 m, respectively. These benefits were attributed to the upstream effect that a moving vehicle exerts on the flow around it.

While it could be argued that this upstream effect was more relevant and novel from a scientific point of view, however, in terms of practical relevance, the largest aerodynamic benefits are expected when a cyclist is drafting not before, but behind a motorcycle. Indeed, it is well-known in the cycling community that drafting behind another cyclist or a vehicle can yield a large drag reduction. This situation is relevant because unavoidably, during parts of the race, some of the motorcycles will ride in front of individual or groups of cyclists and these cyclists can exploit the drafting benefits, leading to an unfair advantage over their opponents. Examples of different situations in races are shown in Fig. 1. The relevant guidelines of the International Cycling Union (UCI) for “vehicle circulation in the race convoy” only stipulate when and which motorcycles can enter the gaps between breakaway riders and the following riders in terms of time differences, which can be 15, 30, 60 and 90 s [28]. The larger the time differences, the more motorcycles can enter the gap. However, the UCI guidelines do not specify what distance should be kept between the motorcycles and the cyclists behind them.

Fig. 1
figure 1

Photos indicating drafting behind a motorcycle in different types of situations: a wide undulating road; b narrow level road; c upward sloped road; d narrow uphill road. (Fig. sources: a Natursports/Shutterstock.com; b–d Radu Razvan/Shutterstock.com; all photos reproduced with permission)

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Drafting of cyclists behind motorcycles is common in races. Cyclists have a tendency to position themselves behind the motorcycle to reduce their drag (Fig. 1a, c). Moreover, sometimes the roads are so narrow that they are forced to ride behind the motorcycle (Fig. 1b, d). Because this happens frequently, concerns have been expressed in the professional cycling community that these aerodynamic benefits can influence the outcome of the race [29, 30]. However, to the best of our knowledge, there is no information in the scientific literature about the drag reduction for a cyclist by drafting behind a motorcycle. Therefore, this paper presents an analysis to assess these drag reductions for a range of separation distances between cyclist and motorcycle.

2 Wind tunnel experiments

Quarter-scale models of a cyclist and a motorcycle carrying two persons were made by CNC cutting from ABS (acrylonitrile butadiene styrene) (Fig. 2). The geometry of the model cyclist was obtained by scanning (Artec Eva 3D scanner) a male cyclist with height 183 cm and mass 72 kg. He was positioned in time-trial position wearing an aerodynamic helmet and a standard tight-fitting racing suit with long sleeves. The resulting frontal area was 0.34 m2. Written consent of the cyclist was obtained. After scanning, the scan facial geometry characteristics were altered/smoothened to make the athlete unrecognizable. The procedure of processing the body geometry and reporting the results was approved by the ethical board committee of Eindhoven University of Technology with reference code (ERB2020BE_1859456_WT). The bicycle was a standard race bicycle with tri-spoke front wheel and disk rear wheel and a time-trial handlebar. CAD software was used to simplify the bicycle geometry by removing gears, chain, cabling etc. The geometry of the motorcycle was created manually based on photographs of components of actual motorcycle geometries (Fig. 2). The frontal area of the motorcycle was 1.21 m2.

Fig. 2
figure 2

Geometry and main dimensions in full scale of the cyclist and motorcycle models

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The wind tunnel (WT) tests were performed in the WT of Eindhoven University of Technology [31]. A dedicated set-up with an elevated sharp-edged smooth horizontal plate and embedded force balance was developed to limit boundary layer development (Fig. 3). The blockage ratio of the set-up was about 2%, which is below the recommended maximum of 5% [32]. Due to the elevated sharp-edged plate, the resulting boundary layer height at the position of the cyclist was limited to 0.06 m and the measured longitudinal turbulence intensity above this 0.06 m was 0.3%. The height of 0.06 m corresponded to the height of the feet of the cyclist, so only a very small fraction of the frontal area of the cyclist was below this height. The drag force on the cyclist was measured with a force transducer designed specifically for high-accuracy quarter-scale cyclist WT tests [25] with an equipment accuracy of 0.001 N. Data were sampled at 10 Hz for 60 s. Tests were performed at wind speeds of 15, 20, 25 and 30 m/s to detect Reynolds number independence, which was noted above 20 m/s. The Reynolds-number independent results were retained and are reported in the results section. It was assumed that there was no crosswind, no head wind and no tail wind, therefore the WT speed represented the riding velocity. A range of wheel-to-wheel separation distances was tested, the full-scale values (i.e. 4 times larger than the WT values) of which are: d = 0.12, 0.24, 0.48, 1.32, 2.64, 4.8, 10, 15, 20, 30, 40 and 50 m. To assess the repeatability of the experimentally obtained drag values, the isolated cyclist was tested five times throughout the measurement campaign. Based on these measurements, the repeatability of the obtained drag values was found to be 0.7–0.9%, which corresponded to drag differences of about 0.3 N for the isolated cyclist. Drag measurements were corrected to match the conditions set in the computational fluid dynamics (CFD) simulations of 101,325 Pa (standard atmosphere), 15 °C, 15 m/s (a top time trial speed) and full geometrical scale. The measurement results will be reported together with the CFD results in the next sections.

Fig. 3
figure 3

a, b Photos of wind tunnel set-up; c, d line drawing of wind tunnel set-up: cyclist behind motorcycle on elevated sharp-edged plate; c side view; d front view. Dimensions in mm

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3 CFD simulations: computational settings and parameters

The CFD simulations were performed at full scale. The computational geometries of the cyclist and motorcycle were identical to those of the WT models except for the WT model bottom plate, the vertical reinforcement bars in the cycling wheels and the geometrical scale (1:1 versus 1:4). The computational domain was a rectangular prism with width 30.3 m and height 24 m. The length varied with the separation distance d. The distance between the domain inlet face and the motorcycle front wheel was 18 m. The distance between the bicycle rear end and the domain outlet face was 45 m. The lateral distance between motorcycle/cyclist and domain side face was about 14 m. The blockage ratio was 0.1%. These domain sizes were larger than those stipulated in CFD best practice guideline documents [33,34,35,36] and the resulting blockage ratio was below the recommended maximum of 5% [33,34,35,36]. In the simulations, the wheels of the cyclist and motorcycle were not touching the ground, i.e. the bottom of the computational domain. This is one of the two typical CFD modeling approaches (“gap approach” versus “step approach”) for wheel-ground contact modeling [37]. The gap approach was used to facilitate grid generation and ensure grid quality in what would be the contact area between wheel and ground. It has been shown that this modeling approach has negligible impact on the resulting drag values [37].

The hybrid hexahedral–tetrahedral computational grids were generated based on grid convergence analysis (not reported here) and on CFD grid generation guidelines [34, 35, 38, 39]. This analysis indicated the necessity of a wall-adjacent cell size of 20 µm (= 0.02 mm) and 40 layers of prismatic cells near the surfaces of the cyclist and motorcycle (Fig. 4). This was required to accurately resolve the thin boundary layer including the laminar sublayer. The dimensionless wall unit y* had values that are generally below 1 and everywhere below 5. Here, y* was defined as y* = u*yP/ν where yP is the distance from the wall-adjacent cell center point P to the wall and u* = Cµ1/4kP1/2. Cµ is a constant (= 0.09) and kP is the turbulent kinetic energy in point P. Note that generally the parameters y+ and u+ are used instead of y* and u* but that the latter parameters have the advantage that they can also be used to specify grid resolution requirements at flow field positions where the shear stress is zero, such as stagnation and reattachment points. At these positions, y+ is zero, irrespective of the local grid resolution yP, and therefore the parameter y+ cannot be used to specify the grid requirements. The parameter y* however will not be zero because it is based on kP. The grid convergence analysis also indicated the necessity of a cell size of 0.03 m in the area between motorcycle and cyclist. Figure 4 shows the grid resolution on the surface of the cyclist, motorcycle and in the vertical centerplane. The total cell count varied with the separation distance d. The grid for the isolated cyclist contained 27.5 × 106 cells and the grids for d = 2.64, 10 and 50 m had 53.1 × 106, 54.6 × 106 and 76.9 × 106 cells, respectively. The high aspect ratio cells as used in the boundary layer region were suitable for the simulations in this paper. They were indeed suitable for Reynolds-averaged Navier–Stokes (RANS) simulations but also for the Scale Adaptive Simulations (SAS), because the latter apply RANS in the near-wall regions.

Fig. 4
figure 4

Computational grid on motorcycle and cyclist surfaces and in vertical centerplane for separation distance d = 2.64 m. Minimum cell size: 0.02 mm. Total cell count: 53.1 million

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At the inlet, a uniform velocity of 15 m/s was imposed, which represents the riding velocity. As in the WT tests, it was assumed that there was no crosswind, no head wind and no tail wind. At the outlet, zero static gauge pressure was set. The surfaces of the motorcycle and cyclist were no-slip walls, where the cyclist body (not the bicycle) and the motorcycle had a surface roughness with equivalent sand-grain roughness height kS = 0.1 mm. The bottom, side and top surfaces of the domain were slip walls. The inlet turbulence intensity had to be set to 0.5% to obtain the same approach-flow value of 0.3% in the region directly upstream of the motorcycle as in the wind tunnel. This was required because the turbulence intensity decayed from 0.5 to 0.3% from the inlet of the computational domain to the position of the motorcycle model.

Two sets of CFD simulations were performed. First, for all distances d, 3D RANS simulations were conducted with the Shear Stress Transport (SST) k–ω model [40] with curvature correction. Pressure–velocity coupling was taken care of by the coupled algorithm with pseudo-transient under-relaxation and a pseudo-transient time step of 0.01 s. Pressure interpolation was second order, gradient interpolation was performed with the Green–Gauss node based scheme and second-order discretization schemes were used for both the convection terms and the viscous terms of the governing equations. The simulations were performed with the commercial CFD code Ansys Fluent 16.1 and 19.1 [41, 42]. Simulations were run for a total of 5000 pseudo-transient time steps and averaging of the results was performed for the last 4000 time steps. Tests confirmed that the total number of 5000 was sufficient to obtain a constant moving average of the sampled drag force.

Second, for separation distances greater than 4.8 m, SAS simulations were performed based on the SST k–ω model. SAS is an improved URANS formulation that allows turbulence spectra to be resolved in the detached regions of the flow [43]. This results in a Large Eddy Simulation (LES)-like behavior in the unsteady regions of the flow field. The SAS-SST k–ω model works in RANS mode with the SST k–ω model for the wall-bounded flow and switches to scale-resolving mode in the large and unstable separation zones of the flow. Pressure–velocity coupling was taken care of by the PISO algorithm. Pressure interpolation was second order, gradient interpolation was performed with the Green–Gauss node based scheme. Bounded central differencing was used for the momentum equations and second-order discretization for the turbulence model equations. Time discretization was bounded second order implicit. Also the SAS simulations were performed with the commercial CFD code Ansys Fluent 16.1 [41]. For these simulations, a time step sensitivity analysis was performed to determine a suitable time step Δt. Keeping the CFL number equal or below 1 in the region between motorcycle and cyclist yielded Δt = Δx/U = 0.03/15 = 0.002 s. For the configuration with the isolated cyclist and that with cyclist behind the motorcycle at d = 10 m, Δt = 0.002, 0.001 and 0.0005 s were tested. For the isolated cyclist, Δt = 0.001 s and 0.0005 s only yielded a cyclist drag force that was 0.1 and 0.3% different, respectively, from that for 0.002 s. For d = 10 m, these deviations were 0.1 and 0.4%, respectively. Therefore, Δt = 0.002 s was retained for all SAS-SST k–ω simulations. The number of time steps required to obtain a constant moving average of the sampled drag values ranged from 8000 to 50,000. Note that e.g. for d = 2.64 m, the time to run one SAS-SST k–ω time step was about 10 times longer than for one RANS pseudo-transient time step. Therefore, RANS was the more economical approach but it is less accurate than SAS [44].

4 CFD simulations: results and validation

4.1 Velocity and pressure fields

Figure 5 presents the RANS results for d = 0.24 m in terms of contours of the mean velocity ratio K and the mean pressure coefficient CP in a horizontal plane at 1 m height and in the vertical centerplane. The velocity ratio K was defined as the magnitude of the local 3D velocity vector divided by the inlet speed (= motorcycle and cyclist riding speed) of U = 15 m/s. The pressure coefficient was defined as CP = (P  − P0)/(0.5ρU2) with P the local static pressure and P0 the reference static pressure. Figure 5a, b display the time-averaged or mean contours by averaging over the last 4000 time steps. The cyclist was clearly embedded in the near wake or slipstream behind the motorcycle where the momentum deficit is pronounced. Figure 5c, d show the mean CP contours indicating that the cyclist was substantially encompassed in the low pressure area behind the motorcycle. The resulting cyclist drag reduction was 75%.

Fig. 5
figure 5

Results of RANS simulations: a, b contours of mean velocity ratio K in horizontal plane at 1 m height and in vertical centerplane for separation distance d = 0.24 m. c, d Same for mean pressure coefficient CP

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Figure 6 presents the RANS results for d = 2.64 m. For this distance, the cyclist was situated further downstream in the wake behind the motorcycle where the momentum deficit was less pronounced as in Fig. 5. This was clearly shown in Fig. 6a, b where the cyclist was immersed in the part of the wake were momentum recovery was substantial, and in Fig. 6c, d, where the area in front of the cyclist was characterized by substantial overpressure associated with the impinging flow on the cyclist. The resulting cyclist drag reduction was 48%.

Fig. 6
figure 6

Results of RANS simulations: a, b contours of mean velocity ratio K in horizontal plane at 1 m height and in vertical centerplane for separation distance d = 2.64 m. c, d Same for mean pressure coefficient CP

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Figures 7 and 8 present the SAS-SST k–ω results for d = 10 m. The cyclist was situated in the far wake. The instantaneous images in Figs. 6a, c and 7a, c show that the slipstream with pronounced vortex shedding was resolved with an LES-like behavior of the computed flow. Figure 7b, d show that the momentum recovery in the area between the motorcycle and the cyclist was substantial, compared to d = 2.64 m. Figure 8b, d display a pressure distribution around the cyclist that resembles that of an isolated cyclist [27], due to the large distance between motorcycle and cyclist. The resulting cyclist drag reduction was 23%. Animations of the SAS-SST k–ω simulations for d = 10 m and d = 20 m are provided in (Supplementary Material 1–5).

Fig. 7
figure 7

Results of SAS simulations: contours of velocity ratio K in horizontal plane at 1 m height and in vertical centerplane for separation distance d = 10 m. a, c Instantaneous; b, d mean

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Fig. 8
figure 8

Results of SAS simulations: contours of pressure coefficient CP in horizontal plane at 1 m height and in vertical centerplane for separation distance d = 10 m. a, c Instantaneous; b, d mean

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4.2 Drag reduction percentages

Figure 9a shows the drag reductions as a function of d. For every distance, the values by the WT tests and the RANS simulations are shown. For d up to 4.8 m, the agreement between the RANS and the WT results was good to fair, with deviations between 0.7 and 1.7% for d = 0.12 m and 4.8 m, respectively. Larger deviations however occurred for d = 10 m and beyond. These deviations are attributed to the well-known deficiencies of RANS simulations based on the Boussinesq eddy-viscosity hypothesis that overpredict the length of the wake and underestimate the velocity magnitude in this wake. These deficiencies have been reported in wind engineering studies (e.g. [45, 46]), and start acting particularly in the far wake, rendering the results from the RANS simulations for d = 10 m and beyond insufficiently accurate. For that reason, scale-resolving simulations (SAS) needed to be engaged, which provided a better agreement with the WT tests, with deviations between 8.0 and 1.5% for d = 10 m and 50 m, respectively.

Fig. 9
figure 9

a Drag reduction percentage as a function of the separation distance d, as obtained by wind tunnel tests, RANS CFD and SAS CFD. b Time gains per kilometer and per minute at a non-drafting speed of 54 km/h and as a function of the separation distance d

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5 Potential time gains

To convert the drag reduction percentages to potential speed increases and potential time gains, the power model by Martin et al. [47] was employed. In this model, the required power is expressed as:

$$P_{{{\text{tot}}}} = (P_{{{\text{ad}}}} + P_{{{\text{rr}}}} + P_{{{\text{wb}}}} + P_{{{\text{pe}}}} + P_{{{\text{ke}}}} )\left( {\frac{1}{\eta }} \right).$$
(1)

With Pad the power loss due to aerodynamic drag, Prr the power loss due to rolling resistance, Pwb the power loss due to friction in the wheel bearings, Ppe the power changes due to a change in potential energy (terrain slopes) and Pke the power changes due to changes in kinetic energy, i.e. the power to accelerate or that becomes available when the system decelerates. The efficiency \(\eta\) is that of the cyclist power transmission, associated to the friction in the drivetrain. For simplicity, we assumed level terrain and constant cycling speed so Ppe = Pke = 0, and no crosswind, headwind or tailwind. Then, Eq. (1) can be written more explicitly as [47]:

$$P_{{{\text{tot}}}} = \left[ {0.5\rho U^{3} \left( {C_{{\text{D}}} A + F_{{\text{w}}} } \right) + UC_{{{\text{rr}}}} mg + U\left( {91 + 8.7U} \right) \times 10^{ - 3} } \right]\frac{1}{\eta }.$$
(2)

The following values were considered for each of the parameters. The density \(\rho\) = 1.225 kg/m3, the reference riding velocity of the isolated cyclist U = 15 m/s, the drag area \({C}_{\mathrm{D}}A\) = 0.21 m2, the rotational drag area for three-spoke/disk wheels \({F}_{\mathrm{w}}\) = 0.001 m2, the rolling resistance coefficient \({C}_{\mathrm{rr}}\) = 0.002, the mass of the cyclist-bicycle system m = 75 kg, the gravitational constant g = 9.81 m/s2 and the chain efficiency η = 0.97698. With these values and the above-mentioned assumptions, for the isolated cyclist at 15 m/s, Ptot = 472.5 W. This is a high value but not unrealistic for professional cyclists, even for long durations. Note that Bradley Wiggins is expected to have delivered 440 W during his successful world hour record attempt in London in 2015 [48]. While this power for an hour is exceptional, larger power values for shorter durations–as in moments of drafting behind a motorcycle—are common in professional cycling [49]. To calculate the speed increase and the potential time gains by drafting, it was assumed that the cyclist provides the same power Ptot (= 472.5 W) when drafting as when riding alone. In this case and using the WT drag reduction percentages as input, Table 1 presents the associated speed increase and the potential time gain per km and per minute, and Fig. 9b presents the time gains graphically.

Table 1 Drag reduction and potential speed increases and time gains for the cyclist drafting behind a motorcycle as a function of separation distance d
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6 Discussion

Table 1 indicates that the potential time gains for a cyclist drafting behind a motorcycle are large, even when drafting at large distances such as between 30 and 50 m. Time trials are sometimes won by fractions of a second. For example, in the 2016 Giro d’Italia individual time trial in Apeldoorn, the Netherlands, Tom Dumoulin gained the victory with only 0.02 s ahead of Primoz Roglic. Considering these tiny time differences between first and second place, it is clear that drafting behind a motorcycle can influence the outcome of races. Therefore, the concern in the cycling community that drafting behind motorcycles can provide benefits that can influence the outcome of cycling races (e.g. [29, 30]) is justified. The distances d in Table 1 could be divided in four categories: (1) very small (d = 0.12–1.32 m), small (d = 2.64–4.8 m), moderate (d = 10–30 m) and large distances (d = 40–50 m). The very small distances do not tend to occur in races and are merely provided to give a more complete view of possible drafting effects. Note however that they do occur in record speed attempts or in some track races. The small distances can occur but generally only for a short period of time. The moderate distances do occur quite often (Fig. 1), and the associated time gains are large. Note that the precise values of drag reduction and time gains provided in this paper are specific to the cyclist and motorcycle geometry tested and the meteorological conditions mentioned above. Finally, while very large separation distances also occur often, the presence of crosswind can render it impossible for the cyclist to benefit from the motorcycle slipstream.

Crosswind, head wind or tail wind will change the drag reductions and time gains reported above. When crosswind is present, the slipstream behind the motorcycle will be at an offset from the straight line behind the motorcycle, making it more difficult for the cyclist to be positioned in this slipstream. This is similar to cyclists trying to remain in each other’s slipstream in crosswind conditions, which is attempted by forming echelons, where the riders are riding in staggered rather than in-line arrangement. Therefore, as the separation distance becomes larger, it might become increasingly difficult or even impossible for the cyclist to remain positioned in the slipstream of the motorcycle. For head wind, the difference in aerodynamic drag behind a rider drafting behind a motorcycle and an unsheltered rider will become larger. Therefore, also the time gains in Table 1 will increase. Conversely, for tailwind, the opposite holds, and the time gains will decrease.

The present rules and guidelines of the UCI do not prevent drafting situations where cyclists can gain large aerodynamic and time benefits over their opponents. The most recent guidelines for “vehicle circulation in the race convoy” [28] only stipulate when and which motorcycles can enter the gaps between breakaway riders and the following riders in terms of time differences. The larger the time differences, the more motorcycles can enter the gap. However, interestingly, in the UCI Cycling Regulations Part 2 for Road Races [50], the motorcycles are sometimes specifically referred to as "motorcycles" but often also as "vehicles". This is shown for example in Article 2.3.023 that lists vehicles including different types of motorcycles. Chapter XII of these regulations deals with race incidents and item 4.7 in the table in article 2.12.007 refers to penalties for sheltering behind or taking advantage of the slipstream of a vehicle. However, no further specifications are provided. This suggest that the issue with drafting behind motorcycles is not a total lack of regulation but rather the lack of specific and clear rules for motorcycles and a lack of effectiveness in imposing such rules. Therefore, it seems imperative that the UCI modifies their rules and guidelines to prevent these undesired and unfair aerodynamic benefits by drafting behind motorcycles. Nevertheless, solutions might not be straightforward. Motorcycles might be asked to ride not directly in a straight line in front of the cyclists, as they do in Fig. 1. However, as motorcycles will position themselves more laterally, the cyclists will have the natural tendency to also change their own lateral position to remain positioned in the motorcycle slipstream. In other cases, e.g. Fig. 1b, d, the roads might be too narrow to allow a staggered position of motorcycle and cyclist. A potential solution could be the use of drones for television recording, to reduce the number of motorcycles in the race convoy to a minimum.

7 Conclusion

While it is well-known that drafting behind a motorcycle provides aerodynamic benefits, to the best of our knowledge, the extent of these benefits had not yet been reported in the scientific literature. Therefore, in the present study, wind tunnel measurements and CFD simulations were performed. Drag reductions were measured and computed for a situation without crosswind, head wind or tailwind. A power model was used to convert these drag reductions into potential time gains. Hereby it was assumed that the isolated cyclist speed is 54 km/h. The study showed that the drag reductions could be accurately assessed by RANS simulations with pseudo-transient under-relaxation, however only up to a distance of about 4.8 m. For larger distances, more advanced and computationally expense scale-resolving simulations with the SAS-SST k–ω model were performed. For drafting distances of 2.64, 10, 30 and 50 m, the drag reductions were 48, 23, 12 and 7%, respectively. The associated time gains were 12.7, 5.4, 2.7 and 1.6 s per km. Because cycling races are sometimes won by a few seconds or less, these time gains can influence the outcome of the races. Therefore, the common concern in the cycling community that drafting behind motorcycles can influence the outcome of races is correct. The current rules and guidelines of the International Cycling Union (UCI) do not prevent situations where drafting can occur. The rules and guidelines need to be adjusted to prevent these undesired aerodynamic benefits.