3.1. Fuel Consumption and Electric Driving Shares
Figure 4 presents a comparison of the real-world fuel consumption of the PHEV under investigation for the hybrid driving mode (
Figure 4a) and for the sport driving mode (
Figure 4b). The boundary conditions such as ambient temperatures between the tests conducted in hybrid driving mode and the sport driving mode tests are similar and both test series are performed within 2 weeks. It should be noted that here the actual fuel consumption related to the ICE is shown, which is measured by a fuel mass flow sensor (cf.
Figure 2). The energy consumption of the electric machine is not included.
Table 4 summarizes the electric driving shares of the studied PHEV for each real-world driving test, considering the different vehicle speed categories. The electric driving shares are calculated as the relative distance share at which the ICE is inactivated, and no fuel consumption is measured.
The comparison indicates an average fuel consumption of 4.6 L/100 km for the hybrid driving mode and 6.2 L/100 km for the Sport driving mode concerning the total test route (
Figure 4). The fuel consumption values for the respective vehicle speed ranges are also about 20–25% lower for the hybrid driving mode compared to the sport driving mode. This can be explained due to the fact that when the sport driving mode is activated, the PHEV activates the ICE more frequently and follows a more dynamic operating strategy than in case of the hybrid mode.
Regarding the influence of the vehicle speed on fuel consumption, for both the hybrid and the sport driving mode, the values for urban and rural vehicle speed ranges are on a similar level, while the fuel consumption for motorway driving is considerably higher. Especially for the urban driving parts, the vehicle indicates high electric driving shares (
Table 4) and therefore low ICE driving shares, which leads to low fuel consumption values. For rural vehicle speed ranges, the ICE is activated more often, but fuel consumption values are relatively low due to more constant (or less dynamic) driving patterns and low driving resistances. At motorway vehicle speeds, the air resistance and hence the fuel consumption rise disproportionately to the vehicle speed increase [
18]. As the ICE needs to be activated most of the time to reach the high power demand, the electric driving shares of the PHEV are low.
Figure 5 shows a comparison of the real-world fuel consumption of the studied PHEV for driving in the hybrid mode in summer (
Figure 5a) and driving the same mode in autumn (
Figure 5b). Besides of the ambient temperature differences, the driving tests in autumn are conducted with winter tires, while summer tires are used for the tests during the warm season (
Table 3).
During the summer tests, the average real-world fuel consumption is about 4.6 L/100 km and in autumn it is 5.3 L/100 km, which corresponds to an increase of 15%.
Concerning the fuel consumption for urban vehicle speeds, the average value of the summer tests is 4.2 L/100 km and for the autumn tests the average fuel consumption value is 5.1 L/100 km. For rural vehicle speeds, the average fuel consumption of the summer tests is 4.2 L/100 km and 4.6 L/100 km for the autumn tests. Average motorway fuel consumptions are 6.5 L/100 km (summer tests) and 6.7 L/100 km (autumn tests). The higher variance of the motorway fuel consumption in the summer tests can be explained by the greater fluctuations of the electric driving shares for motorway driving (
Table 4). However, the average values are nearly identical. The fuel consumption increases for driving the PHEV in autumn compared to summer are approx. 10% for rural vehicle speeds and 3% for motorway vehicle speeds. Regarding urban vehicle speeds, the average fuel consumption of the autumn tests is about 21% higher than in the summer tests. As the winter tires increase the fuel consumption independently from the vehicle speed, the authors assume that the cold start and warming-up phase of the ICE and the energy demand of auxiliary consumers are the main influencing factors for the significant fuel consumption increase at urban vehicle speeds.
3.2. PN Emissions
Figure 6 presents a comparison of the average, distance-related PN emission factors of the studied PHEV for real-world driving conditions in the hybrid driving mode (
Figure 6a) and in the sport driving mode (
Figure 6b). The PN emission factors base on the PEMS raw emission data.
The average PN emission factors of the total test track are similar for both the hybrid driving mode (6.25 × 1011 #/km) and the sport driving mode (6.44 × 1011 #/km), but the variance of the hybrid driving mode values is higher than those of the sport driving mode test results.
Concerning the PN emission factors for urban and rural vehicle speeds, the emission values for sport mode driving are approx. 6% (urban) and 13% (rural) higher than for hybrid mode driving. For both test series, the average emission factors for urban vehicle speeds are higher than those for the rural speed category and the variances are also comparable. The higher PN emissions for urban vehicle speeds relative to rural vehicle speeds—in spite of higher electric driving shares and comparable fuel consumptions (
Figure 4)—can be associated with cold start emission peaks, which appear when the ICE is activated the first time (
Figure 3). At cold start conditions and during the warming up phase, the fuel consumption can increase. In addition to that, the three-way catalyst (TWC) is not fully warmed up yet during this phase, which leads to high CO and hydrocarbon (HC) emissions. These effects can also favor particle formation. Furthermore, it is important to note that the PHEV under study is not equipped with a gasoline particle filter (GPF).
For motorway vehicle speeds,
Figure 6 shows an average emission factor of 8.6 × 10
11 #/km for the hybrid driving mode and 6.9 × 10
11 #/km for the sport driving mode. Thus, PN emissions are significantly higher (+25%) in the hybrid driving mode compared to the sport driving mode, although lower fuel consumptions and higher electric driving shares are observed within the hybrid driving mode tests (
Figure 4 and
Table 4). In order to identify possible causes for this anomaly,
Figure 7 shows a comparison of the cumulative PN emissions over time for a test drive in the hybrid driving mode (
Figure 7a) and a test drive in the sport driving mode (
Figure 7b). In addition, the differentials of the fuel consumption are presented as an alternative indicator for the activity of the ICE as the engine speed could not have been tracked during the tests in the sport driving mode.
During the first half of the test track, the cumulative PN emissions in the hybrid driving mode test are marginally higher than in the sport driving mode test. In the second half of the test track, which mainly consists of rural and motorway vehicle speed parts, the increase in cumulative particle emissions in the hybrid driving mode test becomes much greater than in the case of the sport driving mode test. The fuel consumption differential curve shows that there are generally less spikes in the hybrid driving mode test which means that the ICE is activated less frequently than in the sport driving mode test. However, the amplitude of the fuel consumption differential spikes is significantly higher for the hybrid driving mode (
Figure 7a) than for the sport driving mode (
Figure 7b). The authors assume that the observed dynamic operation pattern of the ICE in terms of its regular activation and deactivation causes these higher fuel consumption differentials, which in turn leads to the strong increase in PN emissions during the rural and especially the motorway driving parts. In contrary, the cumulative PN emissions for driving in the sport mode show a lower increase than in the hybrid mode, because the ICE is operated more continuously, which avoids major particle formation, even though the average fuel consumption is higher. Suarez-Bertoa et al. [
19] show for a GPF-equipped vehicle that the PN emissions are shaped by accelerations and the engine speed. Similarly, in case of the investigated PHEV of this study, the differentials of the fuel consumption and therefore the engine speed are decisive for PN formation. Furthermore, the observed PN emission increase during motorway driving events is not related to a potential low operating temperature of the PHEV, as in contrast to [
7], the test drives are not performed in the electric driving mode. Due to the frequent ICE operation phases in the hybrid and sport driving modes, the operating temperature of the vehicle is sufficiently high during rural and motorway driving. This is proven by the level of the TWC temperatures of +300 °C during the second half of the tests (e.g.,
Figure 3). Therefore, the authors conclude that the obtained results are representative in spite of the mentioned relatively small motorway share of the test route.
Figure 8 shows a comparison of the average, distance-related PN emission factors of the studied PHEV for driving in the hybrid mode in summer (
Figure 8a) and driving the same mode in autumn (
Figure 8b). It should be noted that in the test series during summer particle sizes of up to 23 nm are captured, while the test series in autumn include the measurement of UFP with up to 10 nm diameter.
The average total PN emission factor of the autumn test series is 9.34 × 10
11 #/km, which is approx. 49% higher than the measured average emission factor in the summer tests. While the differences of PN emission factors for rural and motorway vehicle speeds are smaller (6.67 × 10
11 #/km and 5.07 × 10
11 #/km for rural driving and 1.00 × 10
12 #/km and 8.58 × 10
11 #/km for motorway driving), the average urban PN emission factor of the autumn tests is approx. 79% higher than in the summer tests (
Figure 8). One possible cause for this observation could be the influence of the lower ambient temperature in the autumn test series. According to
Table 3, the ambient temperature of the autumn test series is 10–14 °C and 24–29 °C during the summer test series. Worldwide harmonized Light vehicles Test Procedure (WLTP) tests of the same vehicle show that for the hybrid driving mode, PN emissions are marginally higher at −7 °C ambient temperature compared to 23 °C ambient temperature and for the case of urban PN emissions, the values can be even lower at the lower ambient temperature [
20]. Considering these findings and the fact that within the test series of this study the ambient temperature differences are actually smaller, the authors assume that the influence of ambient temperature differences on PN emissions can be neglected in this comparative case. Hence, the significantly higher PN emission factors of the autumn tests are primarily associated with the UFP share, which is particularly dominant at urban vehicle speeds.
3.3. Particle Size Distribution
The development of the particle size distribution is shaped by the non-constant operation of the engine (
Figure 9). The initial emission peak is broad, ranging from <10 nm to 500 nm. Subsequent engine operation yields a high concentration of particles in the 10 nm range. A second mode can be observed at approx. 50 nm. Since the volatile fraction of particles was not stripped from the aerosol, the sub-23 nm fraction increases the fluctuation in the total particle number concentration. The bimodal size distributions are in good agreement with the results of [
12] who analyzed the emissions from a light-duty gasoline vehicle with the EEPS.
The non-volatile particle number concentration from the PEMS and the total particle number concentration of the EEPS feature an acceptable correlation at concentrations below 1.0 × 10
7 #/cm
3 (
Figure 10). Above, the condensation particle counter switches into the photometric mode which lowers the precision of the instrument [
21]. It must be noted, however, that the EEPS also operated at the upper concentration limit of the instrument. A dilution of the aerosol would have been advised to prevent electrometer artifacts but could not be realized in the mobile setup. In the present results no significant shifts were observed which could result from the non-constant engine operation.
Overall, a general impact of the different driving scenarios on the particle size distribution could not be observed. In particular, the motorway section shows a well-repeatable size distribution between the different operation phases. At the beginning of the experiment, the variation is slightly higher. This can be attributed to the warm-up of the engine.
3.4. NOx Emissions
Figure 11 shows a comparison of the average, distance-related real-world NO
x emissions of the studied PHEV for driving in the hybrid mode in summer (
Figure 11a) and driving the sport mode in summer (
Figure 11b).
In total, the average NO
x emission factor of the studied PHEV is about 8 mg/km for hybrid driving and almost 6 mg/km for the sport driving mode. While the emissions for rural and motorway vehicle speeds are similar for both driving modes and generally are on a low level, the urban NO
x emissions differ significantly. For the sport driving mode, the average urban NO
x emission factor is approx. 10 mg/km and the variance within the tests is small (
Figure 11b). The average urban NO
x emissions for hybrid driving are nearly 16 mg/km, which is 52% higher than for the sport driving mode. Furthermore, the variance of urban NO
x emissions is considerably greater within the hybrid driving mode tests, which ranges from approx. 10 mg/km till 24 mg/km (
Figure 11a).
Figure 12 presents the average, distance-related real-world NO
x emissions of the studied PHEV for hybrid mode driving in summer (
Figure 12a) and in autumn (
Figure 12b).
The average NO
x emission factor for the total Stuttgart test route is 6.5 mg/km considering the autumn tests, which is about 18% less compared to the summer tests. The variance of the total emissions is very similar between summer and autumn tests. In comparison with the summer test results, NO
x emissions during rural and motorway driving are on an even lower, near zero-level in the autumn tests and thus can be neglected. The average urban NO
x emission factor of the autumn tests is approx. 14 mg/km, which is 9% lower than for the summer tests. The variance of the test results for urban driving is also similar to the respective bandwidth of the summer test results, ranging from 7 mg/km to 19 mg/km (
Figure 12b). As the NO
x emissions of the summer tests are generally higher than within the autumn tests considering all vehicle speed classes, the authors conclude that the lower ambient temperatures do not influence NO
x emissions in this study. As already discussed regarding the PN emissions, the ambient temperature differences between the summer and autumn tests are small and can be neglected. In contrast, the driving mode seems to be the main influencing factor, as especially for urban vehicle speeds the hybrid driving mode raises the NO
x emissions. Similar to PN emissions, the urban NO
x emissions are mainly determined by the emission peaks resulting from the activation of the ICE during low TWC temperature situations (
Figure 3). Besides the generally higher values of these cold start peak NO
x emissions, the greater variances of the urban emissions within the hybrid driving mode tests and sport driving mode tests also prove that the uncertainty regarding the height of these peak emissions increase for hybrid driving.
3.5. Conformity Factors
The conformity factor (CF) of 1.0 represents the Euro 6 legal emission limit for vehicle type approval and first registration, which is 6.0 × 10
11 #/km for PN emissions and 60 mg/km for NO
x emissions regarding vehicles with SI engines. As these values shall apply for laboratory conditions, respectively, the WLTP margins for PN and NO
x are introduced to consider the measurement uncertainties of the PEMS for (mobile) RDE tests. Indeed, this study does not evaluate valid RDE tests, but a real-world driving scenario. However, it must be noted that most of the RDE trip requirements are fulfilled by the Stuttgart test route (
Table 1).
For PN, the current margin value is 50%, which equals a CF of 1.5 or 9.0 × 10
11 #/km [
22]. For NO
x, the PEMS measurement uncertainty is recently quantified by a margin of 43% [
23], corresponding to a CF of 1.43 or approx. 86 mg/km.
Figure 13 presents the CFs for the PN emissions of each performed real-world driving test with the PHEV under investigation, taking also the different driving situations (urban, rural, motorway vehicle speeds) into account.
For the total real-world driving test route, the tests no. 10 and 11 exceed the CF of 1.5 (both tests show CFs of approx. 1.7), while the other tests show CFs between 0.9 and 1.2, partially even achieving the laboratory limit value. It must be noted that the tests no. 9–11 represent sub-23 nm PN emission measurements, and that the current Euro 6 legislation including the RDE margins only consider PN emissions up to 23 nm, but not below. Additionally, as the investigated PHEV is not equipped with a GPF, the UFP fraction might increase significantly. This is furthermore indicated by the sharp increase in PN emissions for urban vehicle speeds considering these tests (CFs between 1.5 and 2.3), which could indicate a significant UFP share in cold start emissions. In the first 8 tests, the urban PN emissions are within the not-to-exceed limit of 1.5. For rural driving conditions, all tests reveal CFs below 1.5 and the majority is even below the laboratory limit value. For the tests no. 1, 3, 10 and 11 the CFs for motorway driving exceed the limit of 1.5. On the one hand, this again highlights that the hybrid driving mode can increase PN emissions significantly at motorway vehicle speeds (
Section 3.2). On the other hand, considering tests no. 1 and 3, it shows that this increase is not immediately related to the UFP fraction.
Figure 14 gives an overview of the NO
x CFs of each performed real-world driving test with the PHEV under investigation for the different vehicle speed categories.
Even though the current NO
x CF for RDE tests is set to 1.43, the
y-axis in
Figure 14 only ranges to CF 1.0, as in all performed real-world driving tests, the NO
x CFs are below 0.4. Regarding the total test route, the NO
x emissions are at least 5-times lower than the laboratory limit value.
Section 3.4 shows that the main part of NO
x emissions is related to the initial emission peak from the first activation of the ICE, which is also indicated by the relatively high urban CFs (
Figure 14). In comparison, the CFs for rural and motorway driving are below 0.1, partly on a near-zero level. Even if high relative differences are observed within the NO
x CFs, compared to the Euro 6 and the not-to-exceed limits, the NO
x emissions are generally on a low absolute level, considering all tests and driving situations.