5. Energy Amount for Fleet Different Power Train Vehicles
In the previous chapter, we presented the theory of cumulative energy demand (energy carrier consumption) using operational data from one of the analyzed vehicles as an example. The question arises whether, or rather how, this theory can be used to generate arguments for a discussion on future directions of automotive development. Therefore, we decided to present a developed method for generating arguments for the aforementioned discussion, but arguments based on energy issues.
For the analysis, mid-size cars with similar performance (power, acceleration, etc.) were randomly selected from the spritmonitor.de database. The selected cars were ICEVs, HEVs, BEVs, and H2EVs; four types of drive. Fifteen vehicles of each type were selected for analysis.
Therefore, the operating data of 4 x 15 = 60 cars was analyzed.
ICEVs and HEVs are vehicles powered directly by an internal combustion engine, with HEVs assisted by an electric motor located in the gearbox. HEVs are vehicles without the ability to be charged from the mains (not plug-in hybrids).
BEVs and H2EVs are essentially electric vehicles. In the BEV, the electricity is stored on board (in an electric energy battery) and then used to power the electric motors, while in the H2EV, the energy carrier is hydrogen (stored on board in hydrogen tanks). The electricity powering the electric motors is generated on board the H2EV using a fuel cell.
Fifteen items were assumed to constitute a minimum statistical sample, which also allowed for demonstrating the feasibility of conducting a broader statistical analysis of the obtained results.
As mentioned, the theory of cumulative fuel (energy carrier) consumption, presented in the previous paragraph, was used in the research.
It was assumed that for each vehicle group, the analysis results would be presented in summary tables containing:
information about the vehicles, their operational period, mileage, and the coefficients c and a of model (3), as well as the R squared coefficient for each vehicle,
simulations of energy carrier consumption up to a mileage of 300,000 km for each vehicle,
statistical analysis of energy carrier consumption for each of the analyzed vehicles after selected mileages up to 300,000 km.
The information data of operation data of analyzed ICEV’s are given here in the
Table 4.
Table 4 shows that operational data were not always recorded from the beginning of the vehicle’s operation. This did not significantly impact the quality of model (3). The model’s (3) adequacy coefficients were never lower than R
2>0.99, which, considering the randomness of measurements of fuel amount during vehicle refueling, seems to be a very good result.
Trip distance values and period of operational data notice that all vehicles were operated over long term.
The measured cumulative fuel consumption and the one determined using model (3) with coefficients
c and
a (
Table 4) as well as the predicted fuel consumption for 300,000 kilometers of each of the analyzed ICEVs are shown in
Figure 5.
It is clear that as mileage increases, the differences in the individual cumulative fuel consumption curves also increase. These differences demonstrate the feasibility of statistically analyzing the results at the assumed mileage values.
With statistical data, it is possible to create other useful curves as a function of vehicle mileage, such as average cumulative fuel consumption (
CFC AV) and the range of variability of cumulative fuel consumption (
CFC(AV-SD) to
CFC(AV+SD)). The course of these curves for the analyzed ICEVs is also shown in
Figure 5.
Analyses similar to those for ICEV’s are also presented here for the remaining vehicle groups, i.e., HEV’s, BEV’s, and H2EV’s. The results of these analyses are presented in the following table and pictures.
For HEV information data of operation of HEV’s are given I
Table 5.
Measurement data and simulation results with the Model (3) of the cumulative fuel (gasoline) consumption values as a function of the mileage of individual HEV’s are given in the
Figure 6.
Statistically analyzing results at the assumed mileage values for HEV’s are like follow.
For the battery electric vehicles (BEV’s) the consideration result are as follow.
Information of operation data of analyzed BEV’s are given in the
Table 6.
The graphical presentation of the results of cumulative electricity consumption of each the analyzed BEV show the
Picture 7.
And for the analyzed hydrogen fuel cell vehicles (H2EV’s) the achieved results are as follow.
Information of operation data of analyzed H2EV’s are given in the
Table 7.
The graphical presentation of the results of cumulative electricity consumption of each the analyzed H2EV show the Picture 8.
Picture 8 shows that the cumulative hydrogen consumption (CFC) profile of one H2EV (No. 1195603) clearly differs from the others. A closer analysis indicates that this vehicle was operated primarily on country roads – 60%. Furthermore, the vehicle was operated in the city – 24%, with only 16% on highways. Analyzing this data, one can conclude that the operating conditions of this vehicle differed significantly from those of the other H2EV’s. At the same time, the correlation coefficient (R squared) of model (3) is 0.996066, which is relatively high. The “anomaly” in the cumulative fuel consumption profile was the reason why the data from this vehicle were selected to present the procedure for obtaining the coefficients of model (3).
If one element from the set of statistical sample elements differs from the others, then, in accordance with statistical analysis practice, such an element should not be taken into account, otherwise it may “falsify” the analysis results. This was the case here. However, the data for vehicle 1195606 were included in the analysis because the reason this vehicle’s data differs from the data of the other vehicles is not due to measurement errors (R2 > 0.99), but due to different operating conditions. Furthermore, this paper presents a method based on actual operating data, not specific conclusions for application under defined conditions.
With the coefficients c and a, i.e., practically model (3), and consequently also models (4) and (5), determined based on data from long-term operation of each of the analyzed vehicles, and taking into account the very high values of the correlation coefficient (R-squared), it is possible to forecast the energy carrier consumption of each vehicle up to selected mileage (e.g., as here, 300,000 km). Such simulations were conducted, and their results are presented in the figures above, relating to groups of vehicles with defined drive systems (15 vehicles in each of the 4 drive groups). For each group, there is a scatter of consumption values after each assumed mileage. Further analysis allows for the determination of statistical data regarding these value scatters, i.e., the determination of means, standard deviations, etc., and, for example, the mean 100CFC values. Selected results from this analysis are presented in
Table 8.
It’s worth noting that to this point present is a complete analysis of fuel consumption versus mileage for vehicles with specific drive types. However, this publication does not present a method for further analysis of these results or the results of that analysis. A separate publication on this topic is currently being prepared. This publication focuses solely on presenting average energy carrier consumption values and the conclusions derived from them.
But it can ask the general question of how much energy is required to drive vehicles with different types of powertrains over a given distance under long-term, natural operating conditions. Another question might be, for example, whether there is a reliable way to compare different types of vehicle drives, especially in terms of energy efficiency.
It seems that the answer to the first question can be obtained by analyzing, among other things, the SCFC relationship (5). Table shows the 100SCFC values as a function of vehicle mileage for each vehicle groups.
The mileage presented is rather unexpected. It results in a completely different character of the curves for combustion engine-powered vehicles (both ICEV and HEV) and for electric motor-powered vehicles (BEV or H2EV).
It is standard practice to assume that fuel economy (FE) values, and especially averaged fuel economy (AFE), increase with increasing mileage for combustion engine-powered vehicles. This is due, for example, to the degree of engine degradation. In this case, however, with increasing mileage, specific cumulative fuel consumption decreases. This decrease is not significant – it is worth noting the values presented on the vertical axes.
It seems important, however, that
SCFC is not a constant value as a function of vehicle mileage. Therefore, values appropriate for the maximum mileage analyzed for the vehicles were adopted for further analysis. The 100
SCFC results for the 300,000 km mileage of the individual vehicle groups are presented in
Table 9.
Row 1 of the
Table 9. shows the
SCFC values multiplied by 100. It seems that such a presentation of
SCFC values corresponds to the current “habits” in assessing the fuel consumption of vehicles (
FE and
AFE) in their natural long-term operation. It was assumed that each vehicle’s life cycle mileage was at least 300,000 km, which is typical for European passenger cars (considering that in some European countries, cars are used for more than a dozen years - Eurostat). Energy consumption in normal operation can therefore be extrapolated to total energy consumption over the assumed period of use.
The analysis of energy consumption employs a well-to-wheel (WTW) framework, which divides the energy chain into two components:
Well-to-Tank (WTT): the energy required to extract, refine, produce, and deliver usable energy carrier (fuel or electricity) to the vehicle energy storage system (tank or battery).
Tank-to-Wheel (TTW): the energy consumed by a vehicle in motion, determined by analyzing data from the long-term operation of random vehicles of a given brand and type (data treated as statistical data).
The system boundary explicitly includes:
Electricity consumption for “refining” and distributing gasoline (ICEV, HEV);
Electricity for hydrogen generation (electrolysis), compression, and dispensing (H2EV);
Electricity generation and grid losses for BEV charging;
It excludes:
Vehicle manufacturing and recycling;
Maintenance energy inputs;
Energy use in building infrastructure (e.g., refineries, charging stations, hydrogen pipelines).
This boundary ensures comparability by focusing solely on operational energy carriers consumption, consistent (or similar) with EU Well-to-Wheels methodology [
26] .
To ensure consistency across technologies, all energy flows are expressed in three metrics:
Fuel consumption (L/100 km) – standard for ICEV’s and HEV’s;
Energy consumption (kWh/100 km) – for direct or indirect electricity use (BEV’s, H2EV);
Primary energy (MJ/100km) – to allow cross-comparison between chemical and electrical energy.
Conversion factors used in this study are summarized below (
Table 10):
As mentioned above, there is a need for a two-stage energy input: generating energy carriers (WTT stage) and energy for driving the vehicle along the planned route (TTW stage). TTW energy typically comes from commercial installations (e.g., power plants or combined heat and power plants). These installations utilize both: renewable resources (photovoltaics or wind farms) and non-renewable resources (e.g., hard coal, lignite, also petroleum derivatives in combined heat and power plants operating in refineries, etc.). The type of commercial installation used to generate energy and the type of resources used in the TTW stage naturally vary from country to country, for example, within the EU. The proportions of resource use (non-renewable vs. renewable) also vary from country to country.
For this reason, this paper proposes to present only a general method for determining energy demand for a WTW. At the WTT stage, assume that electricity comes exclusively from natural gas-fired installations. The properties (efficiency, emissions) of such installations generally fall between those of installations powered by non-renewable and renewable fuels.
Since only BEVs use electricity at both the WTT and TTW stages, it can be assumed that it comes entirely from natural gas-fired installations. Therefore, it seems appropriate to also conduct an estimate of the electricity required for the WTT and TTW stages from these types of natural gas-fired installations when using ICEVs, HEVs, and H2EVs.
The assumptions and results of further analyses are as follows.
Four representative powertrain types are considered:
a) Internal Combustion Engine Vehicle (ICEV)
Engine efficiency (TTW): 22–25%.
Average fuel (gasoline) consumption on mileage of 300,000km: 8.860 L/100 km.
Indirect energy consumption (for extraction, transport and refining of crude oil, gasoline production and distribution) is equivalent to the energy content of 0.500 liter of gasoline:
0.500L×31.700 MJ/L= 15,850MJ/L. Assuming by fuel economy of 8.860 L/100 km, indirect energy consumption is therefore
WTT = 8.860 L/100 km ×15.850MJ/L = 140.430MJ/100 km.
Direct chemical energy consumption by car driving is:
TTW = 8.860L/100km×31.700MJ/L=280.860MJ/100 km.
Total energy consumption = indirect energy consumption (used achieving of the gasoline) + direct energy consumption (from gasoline used by car driving)
WTW = 140.430MJ/100 km + 280.860MJ/100km = 421.290MJ/100 km.
From this amount of energy (chemical) it is possible to generate electricity, in a power plant, with an average efficiency of 0.400. Assuming that the loss of electricity transmitted from the power plant to the charging station is 8%, the amount of electricity that can be hypothetical collected from the charging station:
WTWe(ICEV) = (0.400×421.290MJ/100 km/3.600)/0.920 = 46,810 kWh/100km /0.920 = 50.880 kWh/100km
WTWe(ICEV)≈ 51 kWh/100km
b) Hybrid Internal Combustion Engine Vehicle (HEV)
Powertrain efficiency (TTW): 30–35%.
Average fuel (gasoline) consumption on mileage of 300,000km: 5.269 L/100 km.
Producing the equivalent of electricity and hypothetically using that electricity to power a car is the same process as for pure internal combustion engine vehicles.
Indirect energy for achieving the gasoline:
WTT = 5.269L/100km×0.500×31.700MJ/L=83.514MJ/100km.
Direct energy for using (energy content in gasoline):
TTW = 5.269L/100km×31.700MJ/L=167.027MJ/100 km.
WTW (chemical energy) of HEV = 83.514MJ/100 km + 167.027MJ/100 km ≈250.541MJ/100km.
Hypothetically production of electricity in power plant and sending this electrify to charging station:
WTWe(HEV) = (0.400×250.541MJ/100km/3.600)/0.920 = 27.838 kWh/100km/0.920 = 30.259 kWh/100km
WTWe(HEV)≈ 30 kWh/100km
c) Battery Electric Vehicle (BEV)
Direct electricity use by mileage of 300,000 km: 20.475 kWh/100 km (electricity from charging station to driving 100 km) =TTWe
Indirect electricity (electricity lost as a result of energy being transferred from the power plant to the charging station). Assuming that the grid efficiency from power plant to the charging station is 0.920,
WTTe = 20.475 kWh/100 km×0.080 = 1,638 kWh/100 km
Required electricity generation for charging station
WTWe = WTTe + TTWe = 20.475 kWh/100 km + 1,638 kWh/100 km = 22.255 kWh/100km
WTWe(BEV’s)≈ 22 kWh/100 km.
d) Hydrogen Fuel Cell Electric Vehicle (H2EV)
Average hydrogen consumption on mileage of 300,000 km: 1.087 kg/100 km
Hydrogen production.
Due to the fact that water electrolysis efficiency: 70%, compression/dispensing of hydrogen efficiency: 90% and LHV of hydrogen is 120.000MJ/kg, the production of 1.000 kg of hydrogen requires the input of primary energy 120.000 MJ/kg/(0,700×0.900) = 190.476 MJ/kg
Indirect energy need:
WTT = 1.087 kg/100km×190.476 MJ/kg= 207.047 MJ/100km
Direct energy need:
TTW = 1.087 kg/100km×120.000 MJ/kg = 130.440 MJ/100km
The total energy demand is therefore:
WTW = 207.047 MJ/100km + 130.440 MJ/100km = 337.478 MJ/100km
Generating electricity from this amount of (chemical) energy will reach the value:
WTWe = 0.400 × 337.478 MJ/100km/3.600 = 37.499 kWh/100km
The hypothetical assumption is that electricity must be delivered to the charging station but there are losses in the transmission network equal to 8% and the final result is:
WTWe = 37.499 kWh/100km/0.920 = 40.759 kWh/100km
WTWe(H2EV)≈ 41 kWh/100km
The data presented show that obtaining hydrogen as an energy carrier is more energy-intensive than using it to power a vehicle.
Assuming that the travel distance is 100 km, then over a distance of 300,000 km, a hypothetical comparison of the average electricity demand of the analyzed drive types can be presented, as follows:
a) ICEV consumed 8.860 L of energy carrier (gasoline). WTWe ≈ 51 kWh of electricity.
b) HEV consumed 5.269 L of energy carrier (gasoline). WTWe ≈ 30 kWh of electricity.
c) BEV consumed 20.475 kWh energy carrier (electricity). WTWe ≈ 22 kWh of electricity.
d) H2EV consumed 1.087 kg of energy carrier (hydrogen). WTWe ≈ 41 kWh of electricity.
Average energy carriers need for driving the analyzed cars with different types of propulsion are given in
Picture 9.
The simulation results presented in Figure 10. demonstrate that operating combustion engine vehicles, even hybrid versions, is not the best energy solution. The energy demand of hydrogen-powered vehicles falls between that of combustion engine vehicles (ICEVs) and hybrid vehicles (HEVs) and is not optimal in energy terms. Interestingly, estimates indicate that the energy required to produce hydrogen exceeds the energy required to propel the vehicle. The lowest energy demand occurs in the long-term, natural operation of electric vehicles, and this situation is unlikely to change in the near future.
While cumulative fuel consumption in long-term, natural operation of vehicles from individual fleets does not seem to raise any major concerns (e.g., very high adequacy coefficients for the mathematical model (3) were obtained, based on data entered by individual vehicle users), the conversions into kWh of energy used to travel 100 km may raise legitimate concerns. However, they are provided here not to demonstrate specific values, but rather to demonstrate the algorithm for arriving at them.