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Article

Parametric Modeling of Mass and Volume Effects for Battery Electric Vehicles, with Focus on the Wheel Components

Institute for Automotive Technology, Technical University of Munich, Boltzmannstr. 15, 85748 Garching, Germany
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Author to whom correspondence should be addressed.
World Electr. Veh. J. 2020, 11(4), 63; https://0-doi-org.brum.beds.ac.uk/10.3390/wevj11040063
Submission received: 13 August 2020 / Revised: 30 September 2020 / Accepted: 1 October 2020 / Published: 2 October 2020

Abstract

:
Defining a vehicle concept during the early development phase is a challenging task, since only a limited number of design parameters are known. For battery electric vehicles (BEVs), vehicle weight is a design parameter, which needs to be estimated by using an iterative approach, thus causing weight fluctuations during the early development phase. These weight fluctuations, in turn, require other vehicle components to be redesigned and can lead to a change in their size (secondary volume change) and weight (secondary weight change). Furthermore, a change in component size can impact the available installation space and can lead to collision between components. In this paper, we focus on a component that has a high influence on the available installation space: the wheels. We model the essential components of the wheels and further quantify their secondary volume and weight changes caused by a vehicle weight fluctuation. Subsequently, we model the influence of the secondary volume changes on the available installation space at the front axle. The hereby presented approach enables an estimation of the impact of weight fluctuations on the wheels and on the available installation space, which enables a reduction in time-consuming iterations during the development process.

1. Introduction

The CO2 emission limits for manufacturer fleets set by the European Union (EU) have become increasingly restrictive in recent years: In 2021, the tank-to-wheel limit will be lowered to 95 g CO2/km [1]. BEVs represent an efficient way to reduce the average fleet consumption since they do not cause any local CO2 emissions and are accounted as 0 g CO2/km [2].
However, for BEVs, there are currently neither established platforms nor predecessor vehicles on which the development can be based. Therefore, during the developing process of BEVs, many design parameters have to be estimated [3]. The parameter weight plays a key role because of the low energy density of lithium-ion-batteries compared to diesel or gasoline fuels. This can be shown by comparing an internal combustion engine vehicle (ICEV) and a BEV of the same model series (Table 1). To increase the range by 100 km, the Golf TSI (Table 1) would need an extra 4.1 L tank capacity, which results in approximately 3 kg additional weight. For the same range increase, the e-Golf would have to store 12.7 kWh more energy in the traction battery, which would result in a weight increase of approximately 127 kg, considering its actual energy density for the battery pack [4]. Correspondingly, the required battery volume increase is approximately 78 L.
The weight increase caused by a larger traction battery does not only affect vehicle consumption but also impacts other vehicle components. If a component becomes heavier or a new one is added during the development process, it leads to a primary weight change (PWC) [6] (p. 9). Using the above-cited example, the 127 kg of added battery weight is the PWC. A PWC, in turn, may require the resizing of other vehicle components. For example, to ensure the same driving performance, the drivetrain components must be adapted. The sum of the weight increases caused by this adaptation is the secondary weight change (SWC). On the other hand, the 78 L of battery increase represents the secondary volume change (SVC). Furthermore, the PWC, can also impact on further components, such as the wheels. A greater vehicle weight requires a greater tire volume and therefore new tire dimensions. The increase in tire volume can, in turn, impact on the available space at the front axle (SVC on the vehicle).
The modeling of vehicle weight in the early development design has already been researched by various authors. Yanni et al. [7], Mau et al. [8], and Felgenhauer et al. [9] present various empirical equations for vehicle weight estimation. However, these authors do not model SWC.
Alonso et al. [10] derive an empirical weight model by dividing the vehicle in modules and quantifying the SWC of each module. The results are further used to evaluate the effects of SWC on vehicle consumption. Nevertheless, the model considers only ICEVs.
Wiedemann et al. [11,12] develop a more detailed method for estimating BEVs weight. They derive a basis weight for the vehicle using the model of Yanni and further add to the basis weight the weight of the electric powertrain, which comprises traction battery, electric machine, power electronics, and transmission. The weight of these components is estimated by using empirical models. The Wiedemann model can estimate the SWCs, but only for the powertrain components.
Fuchs [6,13] creates a weight model for BEVs, dividing the vehicle into modules, which are, in turn, subdivided into their subcomponents. The weight of each subcomponent is modeled empirically or semi-physically. The method can estimate all SWCs.
Angerer et al. [14,15] and Del Pero et al. [16] focus on the influence of weight on BEVs consumption. Angerer uses the model of Fuchs to estimate the influence of weight fluctuations on vehicle dynamics and consumption. Del Pero and al. also focus on the effects of weight reduction on vehicle consumption. However, the model of Del Pero et al. simply consists of a longitudinal simulation and does not contain any weight modeling.
The above-cited authors mainly focus on the SWCs, without considering that a redesign of the components due to a PWC can trigger a change in the component volumes (i.e., a SVC). The SVC can further impact on the available installation space. This requires a check to ensure that the package of the vehicle remains feasible.
To our knowledge, no automatized method exists to simultaneously estimate both SWCs and SVCs. Thus, we aim to extend the existing SWC models with a package model that is capable of estimating the SVC triggered by PWC and SWC. With this method, it is possible, given a PWC, to do the following:
  • Estimate the resulting SWCs;
  • Estimate the SVC of the single components caused by the PWC and triggered SWCs;
  • Estimate the SVC on the vehicle installation spaces caused by the components SVCs.
To show exemplary how this scope can be achieved, we present, in this paper, the developed model for the vehicle wheels. We focus on the wheels at the front axle, since it is the primary steering axle, and, therefore, the wheels greatly influence the available installation space for the powertrain components. Therefore, the SVCs triggered by the wheels are particularly relevant.

2. Materials and Methods

We subdivide the wheel into three subcomponents: brake discs (Section 2.2), rims (Section 2.3), and tires (Section 2.4). To describe these subcomponents (Figure 1), we employ empirical models, which require creating a components database (Section 2.1). After explaining how subcomponent models operate (Section 2.2, Section 2.3 and Section 2.4), we combine them to describe the entire wheel and conduct an evaluation of the wheel model (Section 3.1). This allows an estimation of SWCs and SVCs of the wheel, thus enabling a quantification of the SVC on the installation space at the front axle (Section 3.2).

2.1. Employed Databases and Methods

Due to the limited number of BEVs, it is necessary to include hybrid (HEVs) and plug-in hybrid vehicles (PHEVs) in the database. To ensure a homogeneous and up-to-date state of technology, we consider only vehicles built between 2010 and 2019.
To derive the parametric models for the wheel components, we employ two databases: A2Mac1 [19] and the catalog of the Allgemeine Deutsche Automobil-Club (ADAC) [20]. A2Mac1 is an automotive benchmarking service provider and offers precise and detailed component documentation for the vehicles of leading manufacturers. The ADAC is Europe’s largest automobile club [20], and its online catalog offers an extensive database with 96 current and discontinued brands and a complete list of their vehicles. The catalog assigns a map to each vehicle, which contains information on the overall vehicle level.
We use the A2Mac1 database to acquire data regarding the dimensions and weights of the wheel components. For the modeling of these components, a required variable is the vehicle weight. In this paper, we distinguish between vehicle curb weight (VCW) and vehicle gross weight (VGW). The difference between the two terms is explained below. In the automotive sector, the terms weight and vehicle weight are established definitions [6] (p. IV), which are used as synonyms for “mass”. Therefore, in the scope of this paper, we employ the term weight when referring to the mass of the vehicle or one of its components.
A model series, for example, the Audi e-tron, contains different model variants: quattro, advanced quattro, and S line Quattro [21]. Each model variant has a different weight, which depends on its equipment. We dimension the brakes and tires so that they can withstand the weight of the heaviest model variant of the model series. This ensures that the dimensioned brakes and tires are compatible with all model variants within the model series. The vehicle models contained in A2Mac1 are not necessarily the heaviest variant of the model series, and therefore their VCW cannot be used to dimension the wheel’s components. For this reason, we link each vehicle model of the A2Mac1 database with the corresponding ADAC model series. This step enables us to link the VCW of the corresponding heaviest model variant to each model documented in A2Mac1. An overview of the database can be found in Appendix Table A1, Table A2 and Table A3. In the next sections, when referring to the VCW, we mean the weight of the heaviest model variant of the model series in the vehicle empty state as defined by Reference [22].
Following §34 StVZO [23], the VGW is defined as the weight that must not be exceeded, considering the material stress, engine power, and emergency and long-lasting brake applications. The VGW is calculated from the sum of the VCW and the maximum vehicle payload, which depends on the equipment level and, therefore, on the model variant within a single model series. In this paper, when referring to the VGW, we mean the weight of the heaviest model variant of the model series.
The following subsections (Section 2.2, Section 2.3, Section 2.4 and Section 2.5) describe the developed parametric models for estimating the volume and weight of the wheel components. The content of these subsections is required to understand the results presented in Section 3.

2.2. Brake Model

Two types of wheel brakes are used in passenger cars: drum and disc brakes [24] (p. 64). In today’s vehicles, only front brakes are fitted with disc brakes, and drum brakes are used less often nowadays for rear-wheel brakes, which often use disc brakes instead [24] (p. 64). Therefore, in this paper, we will only focus on disc brakes.
BEVs, PHEVs, and HEVs can recuperate their kinetic energy during deceleration and store it in the traction battery [25]. During recuperation, the electric machine works like a generator: a deceleration of up to 0.3 g can be achieved without using the friction brakes [26]. Thus, most car journeys can be carried out without actuating the wheel brakes. This concept suggests the possibility of downsizing the brake system, which could reduce weight and costs [26]. However, for safety reasons, BEVs, PHEVs, and HEVs are tested for braking by using the same criteria as ICEVs [26]. Recuperation is completely disabled during the performance tests because, when the battery is fully charged or cold, the maximum regeneration potential is not available [27] (p. 29). The vehicle must always ensure maximum braking performance [26] under such conditions.
To provide long-range driving capability, BEVs are equipped with a large battery that can reach a considerable weight (in the case of the Audi e-tron, almost 700 kg [28]). As a result, BEVs are usually heavier than ICEVs with comparable exterior dimensions (see Table 1) [29] (p. 8). Moreover, HEVs and PHEVs are heavier than comparable ICEVs, due to the higher number of required components for the powertrain. Therefore, to comply with legal requirements, the brakes on these vehicles must be larger because the kinetic energy is higher compared to that of a similar ICEV traveling at the same speed [26] (p. 663). Thus, we do not include ICEVs in our database.

2.2.1. Volumetric Model

For the brake disc dimensions, we derive a linear regression model, which correlates the diameter of the brake disc (dependent variable) to the vehicle characteristics (independent variables). In order to identify the vehicle characteristics, which are suitable for modeling the brake disc dimensions, we must identify the central design focus for dimensioning this component.
To ensure safe driving, wheel brakes must be able to withstand heavy operating conditions. An important design criterion for braking systems is the thermal design. The thermal mass of the brake disc plays an important role in thermal stability: Larger and heavier brake discs have more heat-storage capacity and cooling properties. They are, therefore, better able to absorb the kinetic energy of the vehicle that is converted into heat during braking [30] (p. 72). The maximum value of the kinetic energy is calculated by considering the vehicle VGW mveh max and the maximum attainable speed vveh max. The VGW and its top speed are, hence, suitable variables for estimating the brake disc diameter.
The thermal load of the brake discs is also determined by the time it takes to allow the brakes to cool down between two consecutive brake applications. This amount of time relates to the acceleration capability of the vehicle. The faster the vehicle can accelerate, the shorter the time available for brake cooling. This is particularly critical for cases like the AMS consumer test, which tests the braking performance of the vehicle [31]. For this reason, the acceleration time tveh 0–100 from 0 to 100 km/h is a suitable vehicle characteristic for modeling the brake disc diameter.
We extract from A2Mac1 the brake disc diameter Dbrake for the vehicles contained in Appendix Table A1, Table A2 and Table A3. The acceleration time and the VGW are obtained from the ADAC database. We correlate both variables to the brake disc diameter, thus deriving the linear regression model in Equation (1). A list of the symbols used in Equation (1) and the following equations can be found in Appendix Table A4.
Dbrake = 238.345 mm + (0.053 mm/kg) × mveh max − (5.631 mm/s) × tveh 0–100
With this variable choice, we can model the thermal load of the vehicle, using the acceleration time, and the kinetic energy, using the VGW. For the modeling, we only consider ventilated discs, since all vehicles of the database mount ventilated discs as front brakes. The developed model achieves an R2 of 87.3%, a mean absolute error (MAE) of 9.94 mm. The corresponding normalized mean absolute error (nMAE) is 3.22%.

2.2.2. Weight Model

The weight of a brake disc is mainly related to its diameter and its thickness. However, our statistical evaluation showed that the thickness is not a significant variable for weight modeling.
We extract the disc diameter and its weight mbrake for each of the vehicles in Appendix Table A1, Table A2 and Table A3. The resulting regression model describing the correlation between Dbrake and mbrake is shown in Equation (2):
mbrake = −12.870 kg + (0.069 kg/mm) × Dbrake
The developed model achieves an R2 of 91.33%, an MAE of 0.52 kg, and an nMAE of 6.42%.
We also model the weight of the brake calipers and brake pads. In both cases, it was not possible to set up a regression model to link the component’s weight to the vehicle’s characteristics; thus, we use constant values for the modeling. We extract for the vehicles in Appendix Table A1, Table A2 and Table A3 the weight values for the front brake calipers and the brake pads from A2Mac1. We derive a mean value of 5.46 kg for the brake calipers and a standard deviation equal to 1.70 kg. We derive a mean value of 1.02 kg and a standard deviation of 0.31 kg for the weight of each pair of front brake pads.

2.3. Rim Model

To model the rims, we use the nominal rim diameter, which is specified in inches by the manufacturer. It is not possible to create an empirical model, which estimates the rim diameter from dimensions of other components such as the tire diameter. Due to its importance as a design element, the rim and its dimensions do not depend exclusively on the tire diameter, but rather on the specific design strategy the manufacturer specifies. Therefore, we choose to use the rim diameter as the model input.

2.3.1. Minimum Rim Diameter

Since the rim diameter is an input for this model, we do not need to model the rim dimensions. Nevertheless, it must be guaranteed that the input rim diameter is compatible with the brake disc, i.e., that no collision occurs between the brake caliper and rim. To model this effect, we derive a minimum radial clearance, which must be maintained between brake and rim to avoid a collision.
The minimum radial clearance must be calculated, taking as reference the smallest rim offered in the model series, since this rim size represents the worst-case scenario. However, the vehicles documented in A2Mac1 are not necessarily the model variant with the smallest rim diameter. Therefore, we link each model variant of A2Mac1 with the corresponding model series in ADAC and extract from ADAC the smallest rim diameter offered inside the model series Drim min ADAC. With these data, we calculate the minimum radial clearance Drim clearance, as shown in Equation (3):
Drim clearance = Drim min ADAC − Dbrake
We calculate the radial clearance for the vehicles in Appendix Table A1, Table A2 and Table A3 and derive a mean value of 122.24 mm, with a standard deviation of 27.25 mm.

2.3.2. Weight Model

To calculate the rim weight mrim, we develop a regression model, which correlates mrim with the rim diameter Drim (expressed in inches). Equation (4) shows the resulting linear regression model:
mrim = −13.063 kg + (1.405 kg/inch) × Drim
The model achieves an R2 of 88.48%, an MAE of 0.64 kg, and an nMAE of 5.56%. Initially, we also tried to employ the rim material (aluminum or steel) as an independent variable, but it was categorized as statistically irrelevant. The same effect has also been observed by Fuchs [6] (p. 42).

2.4. Tire Model

The European Tire and Rim Technical Organization (ETRTO) defines a tire as a flexible element made of rubber and reinforcement materials [32] (p. G2). The significant tire parameters are the tire diameter, Dtire, the nominal aspect ratio, h%, and the section width, wtire, which are described in the ETRTO manual [32] (pp. G2–G13). In this paper, when referring to the tire diameter, we mean the outer diameter of the wheel. The tires have a great impact on vehicle design [33], and their diameter also depends on the design strategy of the individual manufacturer. Thus, we decide to implement the tire diameter as model input.

2.4.1. Volumetric Model

The volumetric model is implemented as follows: First, the axle load is calculated, thus deriving the required tire load capacity. Subsequently, the tire volume is estimated, empirically, according to the required tire load capacity. Finally, using the rim diameter and tire diameter inputs, the empirically estimated volume is corrected, and the further tire dimensions’ section width and aspect ratio are derived. The exact implementation of these steps is explained below.
The tire volume, Vtire, is defined as the volume of gas contained between the rim and tire under pressure. Given the tire diameter, the corresponding volume can be calculated by using Equation (5):
Vtire = 0.25 × π × wtire × (Dtire2 − Drim2)
To dimension the tire, engineers select the appropriate section width and aspect ratio, which can provide the air volume needed to support the VGW and is compatible with the desired rim diameter. Wider tires provide better traction when accelerating: A large contact area helps powerful vehicles reduce tire slippage when accelerating from standstill and improve acceleration time. Therefore, we set minimal values for the tire width, depending on the vehicle’s power and drivetrain (front-wheel drive, rear-wheel drive, or all-wheel drive) according to Reference [34] (p. 22).
The required tire volume depends on the required tire load capacity, which is the maximum load a tire can carry under specified conditions of use [32] (p. G5) and is coded by the load index. Depending on the structure of the tire, we need to distinguish between standard and extra-load tires. Tires with the additional “extra-load” marking are designed for loads and inflation pressures higher than the standard version [32] (p. G10).
The required tire load capacity depends on the load at the axle. To calculate the axle load and to select the appropriate tire dimensions, the ETRTO manual defines two loading conditions: the 88% rule and the 100% rule [32] (pp. P15–P17). The manual further prescribes for each loading condition the number of passengers aboard and the load stowed in the luggage compartment. Starting with the VCW, the vehicle must be loaded with the prescribed number of passengers and luggage load, thus yielding the loaded weight for the 88% rule (m88%), and the loaded weight for the 100% rule (m100%).
By applying the described loading conditions and knowing the positions of the rows of seats, the position of the luggage compartment, and the axle load distribution of the empty vehicle, it is possible to compute the new axle distribution according to the 100% and 88% rules. We can then derive the distances lF,88% and lF,100% between the center of mass and the front axle for both load cases. Finally, by using l to denote the vehicle wheelbase, we can calculate the tire load (in kg) according to the 88% rule, using Equation (6):
Ltire88% = (m88% × (l − lF, 88%))/(2 × l × 0.88)
Using the same method, we calculate the tire load for the 100% rule (Equation (7)):
Ltire100% = (m100% × (l − lF,100%))/(2 × l)
For the following tire dimensioning, we consider the loading condition, which generates the highest tire load. We then derive a regression that correlates the required tire volume (dependent variable) to the occurring tire load (independent variable). The data needed for this purpose are collected from the ETRTO manual [32]. The ETRTO lists for every tire contained in the manual the corresponding volume and the maximum tire load capacity (in kg), which allows us to set up calculate a regression linking these two variables. For the modeling, we consider all the standard- and extra-load tires listed in the manual section “Passenger car tires”. The tire volume, VtireSL, allowing a standard-load tire to carry a given load, Ltire (in kg), is defined by Equation (8):
VtireSL = −13462233.892 mm3 + (87651.102 mm3/kg) × Ltire
The developed model achieves an R2 of 98.68% and an nMAE of 2.83%. For extra-load tires, the tire volume is calculated according to Equation (9). The developed model achieves an R2 of 98.82% and an nMAE of 2.63%:
VtireEL = −13548645.429 mm3 + (77990.623 mm3/kg) × Ltire
The main drawback of the empirical models in Equations (8) and (9) is that, although they estimate a minimum required tire volume, they do not ensure that the resulting volume is realistic. In fact, the tire volume cannot assume arbitrary values, since the tire dimensions have specific proportions regarding section width and nominal aspect ratio, which are documented in the ETRTO manual. Regarding the tire section width, the manual prescribes values ranging between 125 and 355 mm. The tire section width is always expressed as a multiple of five but not ten, with an interval of 10 mm between two consecutive values. For the nominal aspect ratio, the manual prescribes values between 25% and 80%. The aspect ratio is always expressed as a multiple of five with an interval of 5% between two consecutive values. Therefore, the tire volumes resulting from the regression models have to be corrected to ensure that the volume can be generated from admissible values of tire width and aspect ratio. Figure 2 shows the correction method, which is divided into three steps.
In the first step (Figure 2), we combine the input rim diameter, Drim (in mm), with every possible nominal aspect ratio and section width combination and derive the tire diameter, as shown in Equation (10):
Dtire = Drim + (2 × wtire × h%)/100
The result is a tire diameter matrix (Figure 2) containing all the possible diameters that are compatible with the input rim size. From this matrix, we use Equation (5) to derive the matrix for the corresponding volumes (volume matrix, Figure 2).
In the second step (Figure 2), the diameter and volume matrices are compared with the input tire diameter and the minimum tire volume from Equations (8) and (9). Based on this comparison, we generate two matrices that describe the percentual deviation from the single elements of the diameter matrix or volume matrix to the input tire diameter or minimum tire volume.
Finally, in the third step (Figure 2), we choose from the two deviation matrixes the tire that has the smallest deviation from the calculated volume and the desired diameter. This results in the final values for the tire diameter and volume, as well as the aspect ratio and width. After this step, the dimensions of the tire are fully defined.

2.4.2. Weight Model

For the weight analysis, we implement a regression model that estimates the tire weight, mtire, based on the tire diameter and its section width. The regression is derived from the evaluation of the vehicles in Appendix Table A1, Table A2 and Table A3 and shown in Equation (11):
mtire = −16.890 kg + (0.023 kg/mm) × Dtire + (0.054 kg/mm) × wtire
The developed model has an adjusted R2 of 85.85%, an MAE of 0.71 kg, and an nMAE of 6.63%.

2.5. Wheelhouse Model

Given the tire dimensions, we can estimate the wheelhouse dimensions. In this paper, we focus on the wheelhouse width, wwheelhouse. Given the wheelhouse width, the position of the side roll rail can be identified. Then, knowing the vehicle width at the front axle (W106) and the width of the side roll rail wsrr, we estimate the available space at the front axle, wavailable, as shown in Equation (12):
wavailable = (W106 − 2 × wwheelhouse + wsrr)
In the further steps of the product specification, wavailable can be compared with the actual space required by the powertrain components, wrequired, to test the vehicle concept feasibility. Figure 3 illustrates the above-cited measures.
In the later sections, we consider the wsrr as constant, since our focus is on the wheelhouse dimensions. A change in the wheel dimensions leads to a variation of wwheelhouse, which depends on the tire diameter, the tire section width, and the maximum wheel steering angle, δmax. If we simplify the model by assuming that the wheel steers at its center (located at the half of the tire width), the wheelhouse width can be derived according to Equation (13):
wwheelhouse = 0.5 × wtire × cos δmax + 0.5 × Dtire × sin δmax + 0.5 × wtire
The δmax is usually reached when driving slowly or during parking. For this scenario, we assume an Ackermann characteristic for the steering [35] (pp. 379–380). The inner wheel steering angle is always bigger than that of the outer wheel and thus determines the width of the wheelhouse. Therefore, in Equation (14), we can estimate the δmax from the vehicle turning radius (Rturning), wheelbase (L101), front overhang (L104), maximum width (W103), and track width (W101):
δmax = atan(L101/(–W103 × 0.5 + (Rturning2 − (L101 + L104)2)0.5 − W101 × 0.5))
By combining the result of Equation (14) with the wheel dimensions (Section 2.4), it is possible to estimate the wheelhouse width using Equation (13).

3. Model Evaluation and Results

In the first part of this section, we carry out an evaluation based on a vehicle database, to assess the accuracy of the wheel model. In the second section, we apply a parameter variation to the model in order to quantify the SWC on the wheel and SVC on the wheel and on the vehicle.

3.1. Model Evaluation

To model the SVCs, the accuracy of the estimation of the tire volume and the tire width must be tested. To reach this scope, we first need to create an evaluation database.
We set up the evaluation database, using A2Mac1, ADAC, and the ETRTO manual. We extract from the A2Mac1 database the following information: vehicle axle distribution, the position of the rows of seats, position of the luggage compartment, and the tire load index. The ETRTO manual lists every available tire dimension and the related load indexes. Therefore, using the load indexes, we link the A2Mac1 database with the ETRTO manual, thus identifying which model variants of the A2Mac1 database mount a standard and which an extra load tire. We further link the A2Mac1 models with the corresponding model series in ADAC, thus identifying the VCW of the heaviest model variant for each A2Mac1 model and the exact dimensions of the tires. It was not possible to conduct the above-cited linking for all the vehicles of Appendix Table A1, Table A2 and Table A3 because some information was missing for some vehicles, or no ADAC model series could be found. Appendix Table A5 shows an overview of the evaluation database.
To evaluate the tire volume model, we assign as inputs the vehicle empty axle load, the tire diameter, the rim diameter, the vehicle’s outer dimensions, the VCW, and the vehicle payload. With these inputs, we calculate the VGW for each vehicle of the database. We then calculate the tire load as in Equations (6) and (7), using the positions of the row of seats and the luggage compartment. We suppose that the axle distribution for the heaviest model variant corresponds to the axle distribution given in A2Mac1. Subsequently, we estimate the required tire volume according to the mounted tire type, using Equations (8) and (9). Finally, we conduct the correction method shown in Figure 2. The results are presented in Figure 4.
The X-axis in Figure 4 presents the tire volume resulting from the model, and the Y-axis shows the real tire volume. The resulting estimation has an R2 of 91.0%. For most of the vehicles, the volume is slightly underestimated. This depends on the fact that the different manufacturers use safety factors, dimensioning the tire by using loads, which are higher than the real load. With this strategy, it is possible to compensate for weight estimation errors that can occur in the later specification phase. The volume is overestimated for the BMW 5-Series, the Jaguar I-Pace, and the Kia Niro. Regarding the BMW and the Kia, the error can be attributed to slightly inaccurate load-distribution data, which lead to an overestimation of the required tire volume. The reason for overestimating the Jaguar is explained in the tire-model-width-evaluation section.
We use the same database to evaluate the precision of the tire width estimation. Our wheel model calculates the tire dimensions that fulfill the conditions given on the required tire diameter, the calculated tire volume, and the desired rim diameter, according to the method described in Section 2.4.1. The tire width is calculated for each vehicle listed in Appendix Table A5 and compared with the real values (Figure 5). The tire width model achieves a R2 of 77.0%. The tire width is overestimated for the BMW 5-er (G30), the Jaguar I-Pace (X590), and the Kia Niro (DE). The slightly overestimated tire volume leads to an overestimated tire width for the BMW and the Kia. The required tire volume would be estimated correctly for the Jaguar; however, the calculated value for the tire width of 265 mm is higher than the real one (245 mm). This result is caused by the constraint on the minimal tire width, which is set equal to 255 mm due to the high power of this car’s drivetrain. For the same reason, the resulting volume is also overestimated.
Another cause of deviations from the real tire width values is that our model calculates the tire dimensions only in dependency on the vehicle weight and power without considering lateral dynamic requirements. We do not have enough data to model the lateral dynamic requirements; therefore, we cannot consider this influence.

3.2. Quantification of the Secondary Effects on the Wheel Components

In this section, we apply the wheel model to four reference vehicles, each belonging to a different segment. We intend to evaluate the SVCs and SWCs resulting from a stepwise increase in the VCW, which is denoted in the following sections as the PWC. The reference vehicles are shown in Table 2; the data are collected from the ADAC catalog. Table 2 shows the initial VCW and the tire and rim diameter, which are simulated. The further vehicle data required for implementing Equations (12) to (14) are collected from the A2Mac1 database and are not shown in the table.
Regarding the tire diameter, it can vary of a few mm inside a model series, depending on the chosen rim. For the simulation, we take for each reference vehicle the mean value of all the offered tire diameter of the corresponding model series. Therefore, our method dimensions the tire so that the resulting diameter is as close as possible to the diameter shown in Table 2.
In our analysis, we dimension the tires considering the maximum rim size inside of the model series (Table 2). If the diameter is kept constant, a bigger rim reduces the tire sidewall and requires a wider tire to fulfill the volume requirement. Furthermore, the wheel equipped with the biggest rim is the heaviest wheel variant. Therefore, focusing on the maximum rim size allows us to consider the worst-case scenario for both volume and weight analysis. Nevertheless, the minimum rim size cannot be ignored, since the more the PWC increases, the bigger the brake disc diameter becomes, which could cause incompatibility between the minimum rim size and the brake disc. We discuss this subject in the next section.
We do not consider the limitation on the minimal tire width, due to the vehicle’s power (Section 2.4.1), in order to highlight the effects of the weight increase alone.
We subdivide the quantification of the secondary effects in four steps. In the first step (Section 3.2.1), we analyze the influence of the PWC on the wheel volume, thus quantifying the SVC of the wheel. In the second step (Section 3.2.2), we quantify the influence of the PWC on the wheel, thus estimating the SWC. In the third step (Section 3.2.3), we combine the SVC of the wheel with the wheelhouse model (Section 2.5) and the dimensional chain presented in Equation (12) and Figure 3. This allows an estimation of the SVC on the wavailable (Section 2.5). Finally, in the last step (Section 3.2.4), we invert Equation (12) to simulate a strategy, where the SVC of the wheel is compensated by increasing the vehicle width.

3.2.1. Influence on the Wheel Volume (SVC on Component Level)

An increased PWC leads to a greater tire load, which requires a redesign of the tire, thus affecting its volume (Figure 6). The X-axis in Figure 6 represents the PWC (in %) with respect to the initial VCW. For example, for the Audi e-tron, a PWC of 5% with respect to the initial VCW of 2565 kg (see Table 2) corresponds to a weight increase of approximately 128 kg. The steps in Figure 6 represent the points where the PWC requires a redesign of the tire, i.e., causes a SVC.
As the model also dimensions the brake disc sizes (Section 2.2.1), we can test if the smallest rim size offered for the vehicles of Table 2 has enough radial clearance from the brake disc. This is particularly interesting for the case of the Audi e-tron. The increment of the brake disc diameter caused by a PWC of approximately 0.7% (corresponding to a VCW increase of 17 kg) causes an incompatibility with the given minimum rim size of 19”, as the minimum radial clearance (see Equation (3)) is not fulfilled. To overcome this problem, we distinguish between two possible strategies.
In the first strategy (Audi e-tron 55, two rim variants), the rim size of 19” is simply excluded from the model series, which means that the customer can configure the vehicle with only two rim sizes (20” and 21”). With this strategy, the minimum rim size changes to 20”, thus avoiding the collision between the brake disc and rim. The tire volume does not have to be changed until a PWC of around 8% (Figure 6). The maximum rim size remains unchanged (21”).
In the second strategy (Audi e-tron 55, three rim variants), we impose the requirement that, despite the unfulfilled radial clearance, the vehicle must be configurable by using three rim variants. Such a strategy could be imposed for design reasons or to offer a high product range to the customer. Therefore, since the 19” rim is incompatible with the brake disc after a PWC of 0.7%, it is necessary to start from a minimum rim of 20” and also offer the variants 21” and 22”, shifting the maximum rim size from 21” to 22”. Increasing the maximum rim diameter leads to a decrease in tire volume (because the tire diameter remains constant), which requires a change of the tire section width and nominal aspect ratio in order to comply with the minimum volume requirement. In this particular case, it is possible to find a section width and aspect ratio combination that comes closer to the minimum required volume than the previous one, which explains the slight volume reduction at 0.7% (Figure 6). Nevertheless, this tire combination has a greater section width than the initial one. The effects caused by this redesign are shown in Section 3.2.3.
Regarding the other vehicles, the same effect as the Audi e-tron occurs also for the Nissan Leaf at a PWC of around 6.5% (corresponding to a weight increase of 102 kg). For the sake of simplicity, we do not distinguish between two cases for this vehicle and suppose that a strategy corresponding to the “Audi e-tron 55, three rim variants” is applied, i.e., the number of offered rim variant does not change.
The remaining volume changes, such as the step at 5.2% for the Renault Zoe or the step at 5.8% for the Jaguar I-Pace, are caused by an increase of the tire section width, which is required to compensate for the increase of the minimum required tire volume.

3.2.2. Influence on the Wheel Weight (SWC on Component Level)

For each PWC, we recalculate the dimensions of the brake disc (Section 2.2.1), rim (Section 2.3.1), and tire (Section 2.4.1). The hereby calculated dimensions can be further employed for the weight models of Section 2.2.2, Section 2.3.2, and Section 2.4.2, thus allowing an estimation of the total wheel weight. Figure 7 shows the SWC of the wheel caused by the PWC.
The small steps are related to an increase of the brake disc diameter, while the bigger ones are caused by an increase of the tire width. The great SWC at 0.7% for the strategy “Audi e-tron three rim variants” results from the change in the maximum rim size needed to offer the same number of rim variants: Both the weights of tire and rim change significantly. Figure 7 shows how limiting the maximum rim diameter on the Audi e-tron to 21” allows a wheel weight reduction of approximately 3 kg (for a VCW increase of 6%) with respect to the 22” variant. Reducing the number of rim variants from two to one would also avoid the step at 6.5% for the Nissan Leaf.
In conclusion, if we do not consider the cases of the Audi e-tron and the Nissan Leaf, where the rim size must be changed, we can conclude that the SWC caused by a PWC of 6% is comprised in a range between 0.5 and 1.5 kg per wheel. If we further assume that the vehicles mount the same wheel components at the front and rear axles, this corresponds to a total SWC between 2 and 6 kg.

3.2.3. Influence on the wavailable (SVC on Vehicle Level)

The outer tire diameter is an input of the model and remains constant regardless of PWC. The maximum rim diameter also remains constant as long as no collision between the brake disc and base rim occurs. Therefore, to compensate for the volume increase shown in Section 3.2.1, the tire must necessarily become wider. A change in the tire dimensions leads to a variation of the wheelhouse width as shown in Section 2.5 and Equation (13). Figure 8 shows the increase of wheelhouse width in mm, using the initial wheelhouse width as reference.
Finally, using the results shown in Figure 8, we evaluate the variation of wavailable caused by the PWC. We apply to the four vehicles the dimensional chain depicted in Equation (12). For this calculation, we only model the wheelhouse width variation caused by the PWC, while keeping the values W106 and wsrr constant. Figure 9 shows the loss, in percentage, of wavailable, using the initial wavailable as reference.
For the reference vehicles, a PWC of approximately 6% leads to a loss in wavailable of up to 12%. Regarding the Nissan Leaf, it is clearly shown that keeping the same number of rim variants is not a good strategy, since it can lead to a loss in wavailable greater than 10%. Limiting the Audi e-tron number of rim variants to two can avoid loss of approximately 6% at the front end (for a PWC above 8%).

3.2.4. Influence on the Vehicle Outer Dimensions (SVC on Vehicle Level)

As shown in the previous section, the PWC greatly influences the wavailable. The size of the powertrain components can be only roughly estimated due to the lack of known design parameters during early development design. Therefore, it is advisable to reserve some extra space for these components, thus enabling more freedom in the later course of the development.
For this reason, if the manufacturer does not want to accept a loss of wavailable, another possibility is to increase the vehicle width. While inverting the dimensional chain shown in Equation (12), the increase in wheelhouse width (Section 3.2.2) can be compensated by increasing vehicle width (W106). This inevitably increases the vehicle outer dimensions (Figure 10).
Although this strategy counters the SVC of the wheel, it has a major drawback. The increase in the vehicle outer dimensions directly impacts the VCW. This can be shown by using the empirical model presented by Fuchs [6] (p. 40) for estimating the weight of the body in white (BIW). The BIW weight, mBIW, can be modeled from the vehicle volume, Vveh, as presented in Equation (15) [6] (p. 40):
mBIW = (37.45 kg/m3) × Vveh − 66.38 kg
To model the Vveh, Fuchs distinguishes among different body frames. For example, for the “hatchback” body frame, the volume can be modeled by using the vehicle width (W103), the front and rear overhangs (L104, and L105), the vehicle height (H100), and its wheelbase (L101) as in Equation (16) [6] (p. 39):
Vveh = (0.5 × L104 + 0.75 × L105 + L101) × W103 × H100
It can be seen that a percentual increase in the W103 causes the same percentual increase in the Vveh, thus influencing mBIW. By applying the model for the three rim variants of the Audi e-tron, a 4% increase of the W106 would correspond to a VCW increase of 20 kg based solely on the BIW.
In conclusion, although this strategy avoids a loss of wavailable, it also causes further SWC in other parts of the vehicle. These SWCs can, in turn, cause additional SVCs.

4. Discussion and Conclusions

The presented model enables us to quantify the SWC and SVC of the wheels and to further model the triggered SVC at the front end of the vehicle. It further allows us to estimate the effects of various design strategies.
After introducing the subcomponent models (Section 2.2, Section 2.3, Section 2.4 amd Section 2.5), we combine them to create a complete wheel model and further evaluate it (Section 3.1). For the subcomponent models, such as brake disc weight and dimensions, no evaluation is required, since the performance of the model is already described by the R2, nMAE, and MAE, which are listed in the corresponding model section. Regarding the evaluation of the wheel volume and width, the deviations from the real values mainly depend on the employed tolerances from the manufacturers, which we are not able to estimate. Additional errors may also be caused by the fact that we do not know the exact position of the center of gravity (and therefore the axle distribution) of the heaviest model variant, and we have to suppose that it corresponds to the distribution of the model variant given in A2Mac1.
The model shows that, depending on the vehicle and the applied design strategy, the SWC on the wheels is contained in a range between 2 and 6 kg. If the design strategy is poorly chosen, the SWC can increase up to 20 kg (as in the case we simulated for the Nissan Leaf). These SWC are still too low to trigger further SVCs. Nevertheless, it must be considered that the wheels are not the only components that are affected by SWCs. The same tendency will be observable for components such as the electric machine, body in white, axles, and, most importantly, the traction battery. The sum of the SWCs of these components can, in turn, cause further SWCs [10] and SVCs. Furthermore, an increase in the wheel weight impacts on its inertia, which can lead to higher vehicle consumption. This, in turn, can require a higher battery capacity and generate further SWCs. These effects can be only modeled by coupling the weight model with a longitudinal dynamic simulation. This topic will be addressed in further publications.
While the SWC is relatively low, the SVC on the vehicle shows great relevance. A PWC corresponding to 6% of the initial VCW can cause a loss in wavailable of up to 12%, depending on the applied strategy and on the vehicle characteristics. These results highlight the importance of a SVC estimation in early development, most of all for BEV, which are particularly subject to weight fluctuations. The SVC on the vehicle is highly dependent on the vehicle segment, the design strategy, and the VCW. Nevertheless, the presented methodology is capable of taking into account all of these effects and can be employed to identify SVC already in the early development phase. The approach is developed by following the actual dimensioning methods used by the manufacturers, which enable integration in the manufacturer developing process and can thus minimize the errors and reduce the number of iterations and costs.
In conclusion, in this paper, we quantify the SVC and SWC caused by the wheels and propose an effective approach for addressing the problems they cause. In future publications, we will apply the presented method to further vehicle components, thus expanding the SWC estimation to all the relevant vehicle components. This will allow precise modeling of SWCs and SVCs on other vehicle areas, such as the rear end and the installation space for the battery.

Author Contributions

As first author, L.N. defined the approach for the development of the presented model, identified the relevant components, and detailed the method and the data evaluation. A.R. supported during his semester thesis with the creation of the database, the derivation of the regression models, and the evaluation. A.K. and F.S. supported by the definition of the concept and proofread the paper. M.L. made an essential contribution to the conception of the research project. He revised the paper critically for important intellectual content. M.L. gave final approval of the version to be published and agrees to all aspects of the work. As a guarantor, he accepts responsibility for the overall integrity of the paper. All authors have read and agreed to the published version of the manuscript.

Funding

The research of L.N. was funded by the AUDI AG and the Technical University of Munich. The research of A.K. and F.S. is accomplished within the project “UNICARagil” (FKZ 16EMO0288). A.K. and F.S. acknowledge the financial support for the project by the Federal Ministry of Education and Research of Germany (BMBF).

Acknowledgments

The author L.N. would like to thank the colleagues of the AUDI AG in the persons of Maximilian Heinrich, Martin Arbesmeier, and Alois Stauber, who provided support during concept development. The authors would like to thank A2Mac1 EURL, in the person of Pir Ivedi, for the access to the A2Mac1 automotive benchmarking database.

Conflicts of Interest

The authors declare no conflict of interest, and the funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript; or in the decision to publish the results.

Appendix A

This appendix presents the database we used for developing our parametric models. Table A1, Table A2 and Table A3 give an overview of the database. For each vehicle model, the brand, the ADAC model series, the production year, and the drivetrain type are listed. The ADAC Model Series column is empty for the vehicles not sold in Germany. The “Wheel model” column specifies the parametric model for which each vehicle was used.
For simplicity’s sake, we use the following abbreviations to identify the parametric models:
Table A1. Database overview, part 1.
Table A1. Database overview, part 1.
BrandVehicle ModelADAC Model SeriesProduction YearWheel Model
Audie-tron 55 quattroe-tron (GE) (from 03/19)2019All
AudiA3 Sportback e-tronA3 (8V) Sportback e-tron (01/15–05/16)2015BV, RD
BAICEX360 Fashion-2018BW, TW, RW
BMW2 Series Active Tourer 225 xe Luxury2-er Reihe(F45) Active Tourer (09/14-02/18)2016All
BMW5 Series 530e iPerformance5-er Reihe (G30) Limousine (from 02/17)2018All
BMWi3 Range Extender Urban Lifei3 (11/13–08/17)2014All
BMWi3 Range Extenderi3 (from 11/17)2018BV, RD
BMWX1 xDrive 25Le-2018BW, TW, RW
BMWX5 2.0 xDrive40eX5 (F15) (11/13–07/18)2016BV, RD
BYDE6 Jingying Ban-2015BW, TW, RW
BYDSong DM 1.5 comfort-2017BW, TW, RW
BYDTang 2.0 Ultimate-2015BW, TW, RW
BYDTang EV 600D ChuangLing-2019BW
BYDYuan EV 360 Cool-2017BW, TW, RW
ChevroletMalibu Eco 2.4-2011BV
ChevroletVolt 1.4 VoltecVolt (11/11–08/14)2011All
ChevroletVolt 1.5 Premier-2015BV
CitroenDS5 Hybrid4 So ChicDS 5 (03/12–05/15)2012All
FordC-Max Energi SEL 2.0C-MAX (II) (11/10–05/15)2013BV
DenzaEV Executive-2014BW, TW, RW
Gac NeAion S Max 630-2019BW
GeelyEmgrand EV300 elite-2015BW, TW, RW
GeometryA Standard range power edition-2019BW
HondaCR-V 2.0 Hybrid ComfortCR-V (V) (from 10/18)2019All
HyundaiIoniq 1.6 Plug-inIONIQ (AE) Hybrid (10/16–07/19)2017All
HyundaiKona electric Executive 64 kWhKona (OS) Elektro (from 08/18)2018All
JaguarI-Pace EV 400I-Pace (X590) (from 10/18)2018All
All = the vehicle is used for all models; BV = brake volume; BW = brake weight; RD = minimum rim diameter; RW = rim weight; TW = tire weight.
Table A2. Database overview, part 2.
Table A2. Database overview, part 2.
BrandVehicle ModelADAC Model SeriesProduction YearWheel Model
KiaNiro 1.6 GDi HEV ActiveNiro (DE) (09/16–05/19)2016All
LexusGS 450h F-SportGS (L10) (06/12–08/15)2012All
MaxusEG10 Luxury 2017BW, TW, RW
MercedesEQC 400 4MATIC 1886 EditionEQC (293) (from 06/19)2019All
MercedesGLE 550e 3.0 4MaticGLE (166) (08/15–10/18)2016BV, RD
MitsubishiI-Mievi-MiEV (12/10–04/14)2011RD
MitsubishiOutlander PHEV Business Nav SafetyOutlander (III) Plug-In Hybrid (05/14-10/15)2014All
MitsubishiOutlander PHEV GT S-AWCOutlander (III) Plug-In Hybrid (10/15-08/18)2017BV, RD
NioES8 Base-2019BW, TW, RW
NioES8 founding-2019TW, RW
NissanLeaf 24Leaf (ZE0) (04/12–06/13)2011All
NissanLeaf 30Leaf (ZE0) (06/13–11/17)2016BV, RD
NissanLeaf Tekna 40Leaf (ZE1) (from 01/18)2018All
OpelAmpera-eAmpera-E (07/17–06/19)2017All
PorscheCayenne e-HybridCayenne (9YA) (from 11/17)2018All
PorscheCayenne S-HybridCayenne (958) (10/14–12/17)2014BV, RD
RenaultKangoo Maxi Z.E. 33Kangoo (II) Z.E. Rapid (from 05/13)2017BW
RenaultZoe R135 Edition OneZoe (from 10/19)2019BW
RenaultZoe ZE IntensZoe (06/13–09/19)2013All
Roewe550 1.5 Plug-in hybrid-2016BW, TW, RW
Roeweei5 Topline-2018BW, TW, RW
RoeweMarvel X AWD-2018BW, TW, RW
RoeweRX5 1.5 plug-in Hybrid-2017BW, TW, RW
RoeweRX5 EV400-2017BW, TW, RW
TeslaModel-S 60 kWhModel S (08/13–04/16)2013BV, RD
TeslaModel-X P90DModel X (from 06/16)2016BV, RD
ToyotaAuris 1.8 HSD Dynamic nav. comfortAuris (E18) (01/13–08/15)2013All
ToyotaCamry HybridNo match found in ADAC2018BV
ToyotaC-HR 1.8 HybridC-HR (X10) (10/16–11/19)2018All
ToyotaCorolla 1.8 Hybrid eliteCorolla (E17) (12/16–12/18)2017All
Table A3. Database overview, part 3.
Table A3. Database overview, part 3.
BrandVehicle ModelADAC Model SeriesProduction YearWheel Model
ToyotaCorolla 2.0 Hybrid CollectionCorolla (E21) (from 04/19)2019All
ToyotaLevin 1.8 Hybrid CVT ZunxiangNo match found in ADAC2018BW, RW
ToyotaPrius 1.8 Hybrid Four TouringPrius (XW3) (04/12–02/16)2015BV
ToyotaPrius 1.8 PHVPrius (XW5) Plug-In (from 03/17)2017All
ToyotaPrius 1.8 Plug-in HybridPrius (XW3) Plug-In (10/12–12/16)2012BV, RD
ToyotaPrius 1.8 VVT-i Hybrid LoungePrius (XW5) (from 03/16)2016All
ToyotaRAV4 2.5 Hybrid LoungeRAV4 (XA5) (from 01/19)2019All
VolkswagenGolf VII e-Golf 85 kWGolf (VII) e-Golf (03/14–10/16)2014All
VolkswagenGolf VII e-Golf 100 kWGolf (VII) e-Golf (04/17–05/20)2018BV
VolkswagenGolf VII GTEGolf (VII) GTE (12/14–10/16)2015All
VolkswagenJetta Hybrid 1.4Jetta IV (01/11–08/14)2013BV, RD
VolkswagenUp! e-Up!up! e-up! (04/13–06/16)2013All
VolvoXC60 2.0 T8 Twin Engine AWD R-DesignXC60 (U) (from 07/17)2018All
VolvoXC90 T8 InscriptionXC90 (L) (from 01/15)2015BV, RD
WeltmeisterEX5 500 ExtraNo match found in ADAC2019BW, TW, RW
ZotyeE200No match found in ADAC2016BW, TW, RW
Table A4. List of employed symbols.
Table A4. List of employed symbols.
SymbolDescriptionUnit
mveh maxVehicle gross weightkg
vveh maxMaximum vehicle speedkm/h
tveh 0–100Acceleration time from 0 to 100 km/hs
DbrakeBrake disc diametermm
mbrakeBrake disc weightkg
Drim min ADACSmallest rim diameter in a model seriesmm
Drim clearanceRim radial clearancemm
mrimRim weightkg
DrimRim diametermm or inches
DtireTire diametermm
h%Nominal aspect ratio/
wtireTire section widthmm
VtireTire volumemm3
m88%Loaded vehicle weight according to the 88% rulekg
m100%Loaded vehicle weight according to the 100% rulekg
lF, 88%Distance between the center of mass and the front axle for the 88% rulemm
lF,100%Distance between the center of mass and the front axle for the 100% rulemm
Ltire88%Tire load according to the 88% rulekg
Ltire100%Tire load according to the 100% rulekg
LtireTire loadkg
VtireSLTire volume allowing a standard-load tire to carry a given loadmm3
VtireELTire volume allowing an extra-load tire to carry a given loadmm3
mtireTire weightkg
wwheelhouseWheelhouse widthmm
W106Vehicle width at the front axlemm
wsrrWidth of the side roll railmm
wavailableAvailable space at the front axlemm
wrequiredSpace required by the powertrain componentsmm
δmaxMaximum wheel steering angledeg
RturningVehicle turning radiusmm
L101Vehicle wheelbasemm
L104Vehicle front overhangmm
W103Vehicle maximum width (without side mirrors)mm
W101Vehicle front track widthmm
mBIWBIW weightkg
VvehVehicle volumem3
L105Vehicle rear overhangmm
H100Vehicle heightmm
BIW = body in white.
Table A5. Database for the evaluation of the wheel model.
Table A5. Database for the evaluation of the wheel model.
BrandADAC Model SeriesVCW in kgVGW in kg
Audie-tron (GE) (from 03/2019)25653130
BMW2er-Reihe (F45) Active Tourer (09/14–02/18)17352180
BMW5er-Reihe (G30) Limousine (from 02/17)18452440
BMWi3 (11/13–08/17)14151755
BMWX5 (F15) (11/13–07/18)23052980
HyundaiIONIQ (AE) Hybrid (10/16–07/19)15801970
HyundaiKona (OS) Elektro (from 08/18)17602170
JaguarI-Pace (X590) (from 10/18)22082670
KiaNiro (DE) (09/16–05/19)15942000
MitsubishiOutlander (III) Plug-In Hybrid (05/14–10/15)19452310
NissanLeaf (ZE1) (from 01/18)17072140
OpelAmpera-E (07/17–06/19)16912056
PorscheCayenne (9YA) (from 11/17)23703030
RenaultZoe (06/13–09/19)15751954
ToyotaAuris (E18) (01/13–08/15)14201915
ToyotaC-HR (X10) (10/16–11/19)14601930
ToyotaPrius (XW5) Plug-In (from 03/17)16051855
ToyotaPrius (XW3) Plug-In (10/12–12/16)15001840
ToyotaRAV4 (XA5) (from 01/19)17952185
VWGolf VII e-Golf (03/14–10/16)15851980
VWup! e-up! (04/13–06/16)12151500
VolvoXC60 (U) (from 07/17)22232660
VolvoXC90 (L) (from 01/15)23843010

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Figure 1. Overview of the subcomponent models, based on References [17,18].
Figure 1. Overview of the subcomponent models, based on References [17,18].
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Figure 2. Overview of the correction method for the tire dimensions.
Figure 2. Overview of the correction method for the tire dimensions.
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Figure 3. Overview of the relevant measures at the front end of the vehicle, based on Reference [3].
Figure 3. Overview of the relevant measures at the front end of the vehicle, based on Reference [3].
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Figure 4. Whole-model plot for the tire-volume evaluation.
Figure 4. Whole-model plot for the tire-volume evaluation.
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Figure 5. Whole-model plot for the tire-width evaluation.
Figure 5. Whole-model plot for the tire-width evaluation.
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Figure 6. Interdependency between secondary volume change (SVC) of the wheel and the primary weight change (PWC).
Figure 6. Interdependency between secondary volume change (SVC) of the wheel and the primary weight change (PWC).
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Figure 7. Interdependency between SWC of the wheel and PWC.
Figure 7. Interdependency between SWC of the wheel and PWC.
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Figure 8. Interdependency between wheelhouse width and PWC.
Figure 8. Interdependency between wheelhouse width and PWC.
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Figure 9. Interdependency between the SVC at vehicle front end and the PWC.
Figure 9. Interdependency between the SVC at vehicle front end and the PWC.
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Figure 10. Interdependency between the vehicle width and the PWC.
Figure 10. Interdependency between the vehicle width and the PWC.
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Table 1. Comparison between the internal combustion engine vehicle (ICEV) [5] and the battery electric vehicle (BEV) [5] variants of the Golf model series.
Table 1. Comparison between the internal combustion engine vehicle (ICEV) [5] and the battery electric vehicle (BEV) [5] variants of the Golf model series.
Vehicle CharacteristicVW Golf 1.0 TSI BMTVW Golf (VII) e-GolfDelta
Length4258 mm4270 mm12 mm
Width1799 mm1799 mm0 mm
Height1492 mm1482 mm10 mm
Curb weight (with driver)1026 kg1615 kg589 kg
Power63 kW100 kW37 kW
Top speed180 km/h150 km/h30 km/h
Range1219 km231 km988 km
Energy consumption4.1 L/100 km12.7 kWh/100 km-
Table 2. Reference vehicles used for analyzing secondary effects on the wheel components.
Table 2. Reference vehicles used for analyzing secondary effects on the wheel components.
Vehicle Model
(Model Series)
Initial VCWMin–Max Diameter
Rim Variants
Mean Outer
Tire Diameter
Renault Zoe 22 kWh
(Zoe (06/13-09/19))
1547 kg16”–17”621 mm
Nissan Leaf 40 kWh
(Leaf (ZE1) (from 01/18))
1580 kg16”–17” 640 mm
Audi e-tron 55 quattro
(e-tron (GE) (from 03/19))
2565 kg19”–21”765 mm
Jaguar I-Pace
(I-Pace (X590) (from 10/18))
2208 kg18”–22”759 mm
VCW = vehicle curb weight.

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Nicoletti, L.; Romano, A.; König, A.; Schockenhoff, F.; Lienkamp, M. Parametric Modeling of Mass and Volume Effects for Battery Electric Vehicles, with Focus on the Wheel Components. World Electr. Veh. J. 2020, 11, 63. https://0-doi-org.brum.beds.ac.uk/10.3390/wevj11040063

AMA Style

Nicoletti L, Romano A, König A, Schockenhoff F, Lienkamp M. Parametric Modeling of Mass and Volume Effects for Battery Electric Vehicles, with Focus on the Wheel Components. World Electric Vehicle Journal. 2020; 11(4):63. https://0-doi-org.brum.beds.ac.uk/10.3390/wevj11040063

Chicago/Turabian Style

Nicoletti, Lorenzo, Andrea Romano, Adrian König, Ferdinand Schockenhoff, and Markus Lienkamp. 2020. "Parametric Modeling of Mass and Volume Effects for Battery Electric Vehicles, with Focus on the Wheel Components" World Electric Vehicle Journal 11, no. 4: 63. https://0-doi-org.brum.beds.ac.uk/10.3390/wevj11040063

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