Effect of WLTP CLASS 3B Driving Cycle on Lithium-Ion Battery for Electric Vehicles

Abstract

Capacity loss over time is a critical issue for lithium-ion batteries powering battery electric vehicles (BEVs) because it affects vehicle range and performance. Driving cycles have a major impact on the ageing of these devices because they are subjected to high stresses in certain uses that cause degradation phenomena directly related to vehicle use. Calendar capacity also impacts the battery pack for most of its lifetime with a capacity degradation. The manuscript describes experimental tests on a lithium-ion battery for electric vehicles with up to 10% capacity loss in the WLTP CLASS 3B driving cycle. The lithium-ion battery considered consists of an LMO-NMC cathode and a graphite anode with a capacity of 63 Ah for automotive applications. An internal impedance variation was observed compared to the typical full charge/discharge profile. Incremental capacitance (IC) and differential voltage (DV) analysis were performed in different states of cell health. A lifetime model is described to compute the total capacity loss for cycling and calendar ageing exploiting real data under some different scenarios of vehicle usage.

1. Introduction

Global demand for batteries is expected to increase 14 times by 2030, and the EU could account for 17% of that demand; this is mainly driven by the rise of the digital economy, renewable energy and low carbon mobility. The increase in electric vehicles using batteries will make this market a strategic one at the global level. At least 30 million zero-emission electric vehicles are forecasted to be on EU roads by 2030. While electric cars are expected to significantly decrease greenhouse gas emissions, their batteries are harmful to the environment [1]. However, since today the dependence on oil and gas imports is still very high, just remember the increase in prices due to the conflict in Ukraine [2], the transition to a zero-emission economy will need to be combined with other energy vectors like hydrogen.

Due to the increasing popularity of electric and hybrid vehicles, there has been great interest in the use of lithium-ion batteries. Certainly, excellent characteristics such as high-power density, high energy efficiency, excellent durability, and the ability to work efficiently for partial states of charge (SoC) without the need for continuous full charging have made them particularly attractive. Nevertheless, the energy storage system is the main critical system in an electric powertrain; indeed, the battery pack design still represents an important challenge for Electric Vehicles (EVs) in terms of safety, reliability and system integration. For instance, overloading of the Lithium-ion battery during adverse driving conditions can cause thermal runaway leading to serious fire hazards [3,4]. Thus, thermal management of the Lithium-ion battery pack is crucial [5]. Moreover, the battery is subjected to ageing as the effect of continuous charging and discharging cycles during its use. Similarly, the driver’s driving style can age battery packs differently such us a ranged driving style with a higher frequency of power peaks than a cautious driving style [6].

This will inevitably trigger an ageing process with the result of a loss of power and capacity that will progressively decrease over time.

In recent years, several studies have been carried out to evaluate the ageing of lithium-ion batteries. The two main degradation processes are SEI thickening at the anode during the battery cycling [7,8] and deformation (volume change) and fracture/crack of electrode materials caused by diffusion-induced stresses during cycling, which can result in short circuits that render electrode active materials incapable of storing Lithium-ion [9,10,11].

In [12], an important analysis of main ageing mechanisms occurring at anode, cathode, electrolyte and their interfaces is done with particular attention to carbonaceous anodes and some metal oxides cathodes, such as lithium manganese and lithium nickel-cobalt oxides. The paper describes the correlation of the causes (C-rate, temperature, DoD etc.) with various physical and chemical phenomena, which are the reasons for performance degradation (capacity reduction, power fade, impedance variation). In particular, is underlined the importance of temperature, both at a high and low value, as an accelerating factor of ageing.

An interesting and cited graphical synthesis, which summarize all the ageing mechanism inside a lithium battery, can be found in [13]. Therein, all the various degradation phenomena are clustered into three macro effects called degradation modes, which are respectively Loss of Lithium Inventory (LLI), Loss of Active Material of the Negative Electrode (LAMNE), and Loss of Active Material of Positive Electrode (LAMPE).

In the case of LLI, some lithium ions become no longer available for charge/discharge processes due to parasitic reactions (i.e., Solid Electrolyte Interphase (SEI) growth, decomposition, lithium plating). The effect is a capacity fade but also, in the case of film growth, a power fade. In LAMNE and LAMPE, active masses, useful for lithium ion insertion respectively in charge and discharge processes, become not useful due to particle cracking, loss of electrical contact, blocking of active sites, and structural disordering; these processes happen in both the anode and cathode leading to capacity fade and power fade.

In [14], after an introduction of the main ageing mechanism affecting anode and cathode materials, two main types of ageing mechanisms were identified; calendar ageing, regarding the periods in which the battery is unused, and cycle ageing, related to the application of the battery in real cases.

In [15], a calendar and cycle ageing analysis are presented in terms of capacity fade and resistance increase for Lithium-ion cells from different manufacturers. The cells were subjected to both calendar and cycle ageing, varying SoC and temperature in the former case and C-rate, DoD and temperature in the latter case; it is found that the temperature is the main parameter that affects the capacity fade and resistance increases for both calendar and cycle ageing [16]. However, identifying the ageing of an electrochemical cell is particularly difficult to understand due to its non-linear dependence on charge rate, state-of-charge and temperature [17]. In this regard, an interesting representation of the link between causes and effects in terms of ageing (evaluated with two main macro effects: capacity fade and power fade) has been presented [13]. Here the main ageing factors are identified in time, temperature, SoC level, current, stoichiometry and mechanical stress. All the causes bring different physical and chemical phenomena, with various contributions, going from SEI growth and decomposition (time, high T and SoC, current), electrolyte decomposition (high T and SoC), lithium plating and dendrite formation (low T and SoC, stoichiometry), until loss of electric contact (mechanical stress and low SoC) and corrosion of current collector (low SoC). The relations between causes and effect extracted are represented in

Table 1. Lithium-ion batteries ageing mechanisms.

Cause	Degradation Mechanism	Degradation Mode	Effect
Time High Temperature High Voltage Current Load Load Temperature Stoichiometry Mechanical Stress Low Voltage	SEI growth SEI decomposition Electrolyte decomposition Binder decomposition Graphite Exfoliation Structural Disordering Lithium Plating Dendrite formation Loss of electric contact Electrode particle cracking Transition metal dissolution Corrosion of current collector	Loss of Lithium Inventory Loss of active anode material Loss of active cathode material	Capacity Fade Power Fade

.

The degradation of lithium-ion batteries is identified by two main factors, capacity loss and peak power reduction; these phenomena are connected to physical and chemical processes contributing to lithium-ion battery ageing. The most important are chemical and thermal processes.

Chemical failure mechanisms include SEI formation, electrolyte decomposition and reduction, binder decomposition, active material dissolution, and loss of lithium inventor; these mechanisms depend on several factors, such as cell and components manufacture, cell layout inside the battery pack, and so on. Thermal problems are mainly related to the use of cells outside the characteristics identified by the manufacturer, lack of monitoring controls, poor cell construction, and lack of a control system [14,18,19].

Most of the above-discussed literature is focused on the investigation of degradation mechanisms under calendar or ideal cycle ageing involving standard full charge-discharge profiles. On the other hand, there is a lack of studies on the ageing mechanism induced by a real scenario, such as automotive application.

The investigation conducted with driving cycles that simulate the real application can provide valuable information for the evaluation of ageing phenomena, providing guidance in selecting the best performing battery for the desired application. The work focuses on studying the degradation mechanisms of a commercial battery used for automotive applications, by incremental capacity (IC) and differential voltage (DV) analysis. The Lithium-ion battery considered in this paper consists of an LMO-NMC cathode and a graphite anode because it offers good performance compared with other chemistries, such as LiFePO₄, mainly used in stationary applications [20,21].

Since using a driving cycle of a real vehicle would have given information limited to that type of vehicle and the driver’s driving style, it was chosen to use the WLTP CLASS 3B driving cycle; this cycle is mainly used to determine the pollutant levels, CO₂ emissions and fuel consumption of conventional and hybrid cars, as well as the range of all-electric light-duty vehicles. The driving cycle imposed on the electrochemical cells under test was not accelerated from the point of view of temperature or current; however, the cell was subjected to continuous driving cycles without adhering to the calendar ageing times; this allowed the test times to be reduced from 8 years to only 18 months, including the time needed to perform parametric checks; this strategy, as agreed with the authors, drastically reduced the necessary ageing time of the cell under test with the consideration that calendar ageing can be estimated from real calendar tests for the same type of electrochemical cell found in the literature (commercial graphite/LMO-NMC lithium-ion cells) at different temperatures and SOC. The test time, excluding calendar ageing, was called test years. In this paper is presented a study devoted to the investigation of the degradation mechanism induced by a standard driving cycle, and to the definition of a mathematical model able to estimate the overall capacity loss as an effect of combined cycle and calendar ageing.

The methods used are summarized below:

• A dynamic model [22] of an Electric Vehicle was used for the estimation of a current profile delivery by, or supplied to, the battery pack.
• The current profile extracted from the WLTP CLASS 3B driving cycle simulation was used on a commercial electrochemical cell used for automotive applications.
• Test data were analyzed in order to understand degradation effects to identify capacity loss, resistance increase, and ageing phenomena using IC and DV curves.
• A mathematical model for capacitance loss from cycle ageing and calendar ageing was extracted.
• The model was used to estimate battery ageing over possible vehicle operating scenarios.

2. Materials and Methods

2.1. Lithium Ion Cell Characteristics

Experimental tests are performed to investigate Lithium-ion cell degradation under the WLTP CLASS 3B driving cycle. Full charge/discharge cycles at 1C (capacity test) and a 10% SOC step Pulse test from 100% to 0% SOC were interposed to the ageing cycles.

The Lithium-ion battery for Electric Vehicles applications [23] considered in this paper, hereafter referred to as Device Under Test (DUT), consists of an LMO-NMC cathode and a graphite anode with a capacity of 63 Ah, whose technical specifications are given in

Table 2. Lithium-ion battery technical specifications from the datasheet.

Cell Type	Lithium-Ion
Chemistry Cathode	LMO-NMC
Chemistry Anode	Graphite
Capacity	63 Ah
Nominal voltage	3.75 V
Operating voltage	2.7 V–4.12 V
Battery temperature	−40–65 °C

.

2.2. EV Mission Profile

The World harmonized Light-duty vehicles Test Procedure (WLTP) is a globally harmonized standard for determining levels of pollutants such as CO₂; it is used for fuel consumption of internal combustion engines (ICE) and to determine the range of electric vehicles.

The WLTP procedures include several World harmonized Light-duty vehicle Test Cycles (WLTC) for different categories of vehicles based on the power-to-mass ratio (PMR), defined as the ratio of rated power (W) to ground mass (kg) (excluding driver), and the maximum speed (vmax) of the vehicle as declared by the automaker; it includes three different WLTC test cycles, depending on the class of vehicle according to PMR:

• Class 1—low power vehicles with PMR ≤ 22;
• Class 2—vehicles with 22 < PMR ≤ 34;
• Class 3—high-power vehicles with PMR > 34;

The work is focused on high-power vehicles. Therefore, it was chosen to perform the tests using the WLTP CLASS 3B cycle. The WLTP 3b cycle is composed of four sections: low, medium, high, and extra-high. For our purposes, the WLTP CLASS 3B was selected with a length of 23.266 km to be covered in 1800 s with a peak speed of 131.3 km/h, as shown in Figure 1. Each part contains a variety of driving phases, stops, acceleration and braking phases. Usually, the four phases are associated with a high traffic density urban road for the low part, a low traffic density urban road for the medium part, a suburban road for the high part, and a highway road for the extra-high part [24].

The driving cycle is defined in terms of speed and time. To identify the power profile required for the cell under test the vehicle model proposed in [22] was used and depicted in Figure 2. The model consists of three main blocks namely, the dynamic model of the vehicle, the AC motor model and the converter model [25]. The first block determines the traction effort on the basis of the mechanical force pushing the vehicle and computes the load torque at the motor shaft (M_e^*) and shaft speed. The AC motor model computes the electrical power P_me^*, which the inverter is tasked to provide. The model of the converter estimates the power at the poles of the battery pack. The main technical specifications of the considered Electric Vehicle are summarized in

Table 3. Electric Vehicle technical specifications extrapolated from Technical specifications of BMWi3 model [26].

Vehicle Type	Battery Electric Vehicle (BEV)
Vehicle mass	1195 kg
Frontal area	2.8 m2
Drag coefficient	0.29
Rolling friction coefficient	0.012
Transmission gear ratio	9.7
Hub diameter	48 cm
Tire width	15.5 cm
Tire aspect ratio	70%
Wheel radius	25.4 cm
Motor type	AC-PMSM
Motor rated power	75 kW
Motor rated speed	4800 rpm
Motor pole pairs	4
Battery pack	85 cells in series

.

After verifying that the driving cycle used was correctly reproduced from the model, as shown in Figure 3, the battery current profile was extracted through the model and applied to a single electrochemical cell. The current profile was used instead of the power profile because the software for the automatic creation of the cycler program did not support this option.

Since the SOC, it was found useful to limit the SOC of the cell under test to 30% maximum, furthermore for the current profile extraction has been used the nominal voltage matching with 50% SOC. Under these conditions, the operating voltage window is relatively close to the nominal value of 3.75 V. As a result, the error between the current profile extracted from the model and the current profile computed as the ratio of power and rated voltage of 3.75 V have a max error of 13.36% and a mean error of 7.78% (Figure 4). The error was deemed acceptable.

To correlate the number of driving cycles and vehicle operating times, average data of distance driven in Europe by a light-duty vehicle were taken as a reference [27]. The total distance is 12,168.12 km, equivalent to 523 driving cycles per year. The tests were then carried out in steps of 261/262 driving cycles before checking the characteristics of the DUT.

2.3. Test Procedures

A prismatic lithium-ion battery cell was used to investigate the effect of WLTP CLASS 3B driving cycles. The cell is aged with WLTP CLASS 3B driving cycle at ambient temperature (25 °C) for a number of cycles equal to 8 real years (4184 cycles) neglecting calendar ageing (test years). The sequence of cycles involves the electrochemical cell recharging at 1C when the voltage reaches 3.1 V. After the cell has reached the upper cut-off voltage of 4.12 V, the cycle continues from where it had stopped. Suitable tests are accomplished at the beginning of the ageing test and every 261/262 cycles to verify the characteristics of the cell under test; these are a capacity test (Figure 5) and a pulse test (Figure 6).

The capacity test is performed to verify the capacity of the cell; it consists of 3 complete charge and discharge cycles within the upper and lower cut-off voltage of 4.12 V and 2.7 V, respectively, at Constant Current (CC) for the discharge and Constant Current-Constant Voltage (CC-CV) for the recharge at 25 °C; this procedure, which is performed to stabilize the active materials of the cells is described in

Table 4. Capacity test procedure.

Step	Description	Parameter	Stop Condition
1	Temperature conditioning	T = 25 °C	t = 1 h
2	CC Discharge	I = 63 A	V = 2.7 V
3	CC-CV Full Charge	I = 63 A CV = 4.2 V	I = 0.2 A
4	CC Discharge	I = 63 A	V = 2.7 V
5	Repeat from 3 to 4		Counter = 3
6	CC-CV Full Charge	I = 63 A CV = 4.2 V	I = 0.2 A

.

As described in

Table 5. Pulse test procedure.

Step	Description	Parameter	Stop Condition
1	Temperature conditioning	T = 25 °C	t = 1 h
2	CC-CV Full Charge	I = 63 A CV = 4.2 V	I = 0.2 A
3	Rest		t = 1 h
4	CC Discharge	I = 63 A	t = 10 s V = 2.7 V
5	Rest		t = 3 min
6	CC Charge	I = 63 A	t = 10 sV = 4.12 V
7	Rest		t = 3 min
8	CC Discharge	I = 63 A	Discharge Capacity = 10% Capacity test V = 2.7 V
9	Rest		t = 1 h
10	Repeat from 4 to 9		Counter = 10
11	Rest		t = 1 h
12	CC-CV Full Charge	I = 63 A CV = 4.2 V	I = 0.2 A

, the pulse test encompasses a 10 s discharge at 1C (63 A), a 3-min wait phase, a 10 s charge at 1C, a 3-min wait phase. A 1C discharge of 10% of the capacity is then performed; it is assumed to be 10% of SOC. Finally, a 1-h rest is accomplished. The procedure is repeated until the lower cut-off voltage is reached.

2.4. Test Facilities

All tests were performed by using a Bitrode cycler model FTV1, whose main features are summarized in

Table 6. Cycler main features.

Description	Characteristics
Model	Bitrode cycler FTV-1 1000/100/10–20
DC Voltage Range	0–20 V (Res. 0.001 V)
Maximum DC Current	1000 A
Maximum Data Acquisition Rate	0.1 s/Data Sample
Current Ranges Max	500 A (single channel) 1000 A (2 channels in parallel) (Res. 1 A) 100 A (Acc. 0.1 A) 10 A (Acc. 0.01 A)
Assignable Data Channel Inputs	2
Thermocouples Type	J
Temperature Range	−40 to 200 °C (Res. 0.5 °C)
Temperature Tolerance	±2 °C (for all measured temperatures)

.

Note: The instruments and equipment used to carry out the tests indicated in this paper were kindly provided by the Institute of Advanced Energy Technologies “Nicola Giordano” of the National Council of Research (CNR-ITAE) in Messina, Italy.

Current and cell voltage measurements were carried out with sensors located inside the cycler. The cells have been placed in a climate chamber (

Table 7. Climatic chamber main features.

Description	Characteristics
Model	Angelantoni Discovery 340 L
Useful Volume	337 l
External Measurement (L × D × W)	919 × 1786 × 1765 mm
Useful Internal Measurement (L × D × W)	601 × 810 × 694 mm
Temperature Range	−40 to +180 °C
Temperature Precision	0.1 ÷ 0.3 ± K
Humidity Range	10–98%
Maximum Internal Thermal Load	2300 W (+25 °C)
Cooling Gas	R404
Additional Temperature sensors	N°5 PT100

) to allow accurate control of the internal temperature, which was monitored with two Pt100 thermistors directly connected to the cycler. In Figure 7 shows the instruments used to perform the tests on the electrochemical cell.

2.5. Test Schedule

The ageing test campaign using the WLTP CLASS 3B cycle was carried out following a procedure, which involved the sequence of tests shown in

Table 8. Ageing test with WLTP CLASS 3B driving cycle.

Step	Parametric Checks	Driving Cycles	Total Driving Cycle	Total Ageing Test Years
1	Capacity + Pulse test	261	261	½ year
2	Capacity + Pulse test	262	523	1 year
3	Capacity + Pulse test	261	784	1 ½ year
4	Capacity + Pulse test	262	1046	2 year
5	Capacity + Pulse test	261	1307	2 ½ year
6	Capacity + Pulse test	262	1569	3 year
7	Capacity + Pulse test	261	1830	3 ½ year
8	Capacity + Pulse test	262	2092	4 year
9	Capacity + Pulse test	261	2353	4 ½ year
10	Capacity + Pulse test	262	2615	5 year
11	Capacity + Pulse test	261	2876	5 ½ year
12	Capacity + Pulse test	262	3138	6 year
13	Capacity + Pulse test	261	3399	6 ½ year
14	Capacity + Pulse test	262	3661	7 year
15	Capacity + Pulse test	261	3922	7 ½ year
16	Capacity + Pulse test	262	4184	8 year

.

3. Results and Discussion

3.1. Cells Inspection and Beginning of Life (BOL) Conditions

At the beginning of the work, different cells are taken into account for the ageing test. The first step before starting the ageing tests is to visually inspect the cells to make sure they are not damaged. Capacity tests are then conducted to evaluate the cell’s capacity. The cell with parameters close to those given in the manufacturer’s datasheet was chosen for ageing tests.

Cell capacity and energy were computed for the selected Cell 1 at the end of the third discharge cycle of the capacity test. The efficiency was computed as the ratio of the energy extracted to that injected during the tests. The cell has shown a 64,26 Ah capacity, a value very close to that of manufacturer’s datasheet (

Table 9. Main parameters of cells at the BOL.

	Ageing Tests	Discharge Capacity (Ah)	Discharge Energy (Wh)	Energy Efficiency (%)
Cell 1	Driving cycle 25 °C	64.26	241.03	96.01

).

3.2. Cells Cycling under Current Driving Cycle

The current driving cycle was applied to Cell 1. During each step of the ageing test the cell starts from the fully charged condition (SOC = 100%). Upon reaching the voltage of 3,1 V, identified as the minimum safety voltage, the charging phase is triggered. Under these conditions the full discharge of the Cell 1 is about 6 current driving cycles. However, current driving cycles will age Cell 1 over time, causing a degradation leading to a shorter time to reach the lower cut-off voltage than under BOL conditions. For the recharging phase, it is known that electric vehicles require rather long charging times. However, electric vehicles can be recharged faster by using high-power charging stations (e.g., DC fast stations) [28]. Therefore, a charging time below one hour has been assumed only with a CC charging until the upper cut-off limit without a CV charging phase. In Figure 8 a single-step of ageing test with a WLTP CLASS 3B driving cycle is reported. The value of SOC was computed by considering the capacity discharged from Cell 1 during the tests.

Figure 9 shows the evolution of both charge and discharge voltage profiles as a function of the capacity, along different equivalent years of driving cycle ageing. Voltage profiles have been recorded during the parametric check-up tests at 1C. A reduction in available cell capacity of 11% and alterations in the shape of the curves after a series of test equivalent to 8 years was found.

Pulse tests were accomplished to identify the internal resistance of Cell 1 during various stages of ageing at different SOC. The resistance of the battery was computed as the voltage-to-current ratio. Several phenomena contribute to the voltage drop, they can be identified with a contribution due to all electronic resistances, the battery’s electrolyte resistance, the battery’s double layer capacitance and charge transfer resistance, and the polarization resistance which accounts for ionic diffusion in the solid phase [29]. The cell internal resistance (IR) depends on the interval Δt at which voltage and current samples are taken and also depends on the SOC battery. Resistance values at various SOC levels in 10% steps were extracted from the pulse tests. The applied driving cycle did not cause a large increase in the internal resistance of the cell under test; this value is confirmed by the energy efficiency value of the cell remaining almost constant. Probably during the first ageing the cell conditioned itself by improving performance and then remained stable as shown in Figure 10.

To further investigate the cell behaviour during lifetime IC and DV analyses were also performed; these analyses are two techniques widely applied to identify and quantify degradation mechanism in Lithium-ion batteries [30]. The plateaus in charge and discharge voltage profiles represent phase transitions occurring due to electrochemical reactions, which can be highlighted after the differentiation of the curve, by the presence of well-defined peaks. IC analysis, performed by differentiating the capacity with respect to the voltage, allows obtaining peaks to correspond with the plateaus of the voltage-capacity curve, while DV analysis differentiates the terminal voltage with respect to cell capacity and shows peaks corresponding to the valleys of the IC curve. By the analysis of both techniques, a feature of interests (FOI) can be identified on the differential curves. The most relevant FOIs of the IC curve include intensity, position, and the area under the peaks, while for the DV curve the distance between the two adjacent peaks is the main FOI. In particular, the degradation mechanisms can be related to IC peak shifts toward lower voltage associated with IR, the decrease in IC peaks intensity linked to LAM, and DV peak shift coupled with both LAM and LLI [31].

In Figure 11 is shown the evolution of the IC curve obtained by differentiating the 1C discharge curves at different levels of ageing (years); it should be noted that, here a high C-rate was used to acquire the voltage capacity curve, even though IC and DV often require a signal very close to the equilibrium condition of the cell. Despite the voltage curves used in the present work to perform differential analysis were acquired at 1C, the signals provided were still useful for identifying the most relevant signature typical for the chemistry of the cell under investigation. Indeed, as already proven in previous works, a higher C-rate can still be useful for ageing mechanism identification [32,33]. By observing the IC curve three different peaks A, B and C can be identified at 3.47 V, 3.8 V and 4.1 V, respectively, which can be related to the graphite anode signatures [34]. On the other hand, the cathode phase transitions are not visible on the curve. Nevertheless, the overall shape of the curve suggests that the cathode chemistry is a combined LMO/NMC composition as already reported for the same cell [23]. The most important variations as the effect of ageing are observed on peak A, which dropped almost 36% and shifted by 5 mV to higher potential in comparison to the fresh cell. Lower decreases of the intensity close to 10% are also observed for both peaks B and C. Despite the evolution in intensity, the positions of both peaks B and C on IC curves remain almost unchanged. On the basis of previous interpretations of the IC curve to identify the degradation mechanisms [35,36], the evolution of peak A can be mainly related to LLI, while the constant decrease in both peaks B and C can be due to the LAM of the negative electrode. With regards to the peaks position, during discharging, the change in voltage is negative and the peak in the IC graph are shifted to lower potentials because of the overvoltage caused by the polarization resistance [37]. Since the shift of peak A with ageing is in the opposite direction and both peaks B and C remain unchanged, in agreement with the internal resistance evaluated by the pulse test, also IC analysis confirms that no relevant IR loss occurs.

It is worth noting that, by proceeding with ageing a small peak at about 3.62 V appears, becoming well-distinguished on the IC curve matching with 8 years ageing; this peak, representing a typical signature of cathode material, may be masked due slow kinetic of the transformation and the high C-rate of the analysis, which does not allow to detect the process. On the other hand, once the contribution from the negative electrode on the peak shape over cycling is eliminated, the effect of the cathodic reaction is made evident on the IC curve [38].

Figure 12 deals with the evolution of the DV curve when differentiating the 1C discharge voltage profiles, similarly to what was done for IC analysis. The DV curve shows two peaks, which match with the valleys 1 and 2 in the IC curve and are representative of the anode signature of the cell. No cathode signatures are instead observable in the DV curve as already reported for similar batteries when a full cell voltage profile is used for the analysis [39]. In order to deeply investigate the degradation mechanisms of the cell, peak 2, which indicates a 50% graphite lithiation, is used as a reference process; it is to be noted that for the cell under investigation, this peak is centred at about 75% of the total capacity, which suggest that the anode is overhang as typically for lithium battery [40]; this peak divides the DV spectra in two regions identified as distance Q1 and Q2 in Figure 13. The evolution of the distance Q1 with ageing can provide information about alteration on lithium storage capability of the graphite anode, then it is representative of anode degradation due to LAM. On another hand, Q2 gives information about cycling lithium between anode and cathode, therefore its change is indicative of a possible LLI side reaction [41]. Figure 14 deals with the progression of both Q1 and Q2 parameters as the effect of equivalent years of ageing under WLTP CLASS 3B driving cycles. Q1 change rapidly in the first year decreasing its value from 46.7 to 43.2 Ah then holding essentially the same value for the following cycles. On the contrary, a larger variation of the Q1 value can be observed, with a slight increase during the first year, and a progress drop proceeding with cycle ageing. The evolution of Q1 suggests that, after an initial loss of storage capability of the anode it is almost unchanged, then a slow degradation occurs with the cycles in the following years; this observed behaviour suggests that during the first driving cycles, the anode undergoes initial conditioning due to the repeated volume changes of the graphite grains during lithiation and delitiation phases. As is well known, these contractions and expansion lead to the formation of particle cracking or to the detachment of the active material from the electrode with consequent isolation of the particles and therefore to loss of active material (LAM) [42]. The lack of further evolution of Q1 after the first few cycles could mean that, following the initial rearrangement of the anode material, there is no longer a relevant LAM of the negative electrode. In contrast, Q2 follows a linear loss of capacity, suggesting that LLI is the dominant degradation mechanism induced by WLTP CLASS 3B driving cycles on the DUT; this ageing mechanism is in agreement with previous literature for the chemistry of the DUT and it is attributed to the continuously slow growth of the SEI layer on the negative graphite electrode [43,44,45]. However, a more detailed analysis of the trend of Q2 during the first year shows a slight increase in capacity compared to the fresh cell, which could be related to a larger amount of cycling lithium inside the cell. To better understand this phenomenon, it is possible to analyze the change in the shape and height of the peaks in the DV curve. Regarding peak 2, corresponding to the phase transformation of the high SOC anode, it rises in intensity also becoming sharper during the first cycles corresponding to about the first year of ageing, then shifts to the right keeping the shape and magnitude unchanged. The magnitude of the peaks is usually related to the degree of homogeneity of lithium distribution (HLD) inside the cell, and in particular, the increase in intensity due to the charge and discharge cycles could be explained by an improvement in the HLD compared to the fresh cell not yet adequately conditioned [46,47]. A result similar to the one just discussed was obtained by Sieg et al. [48] investigating the ageing phenomena induced by an EV driving profile on a cell based on an NMC cathode; they observed that the peak shown in the differential voltage curve at high SOCs corresponding to an anode transformation shows an increase during the first few cycles and then decreasing over time due to the effect of cycles on the cell. Such an evolution of peak intensity has been related to an initial enhancement of the HLD of the cell and then to a change in graphite material or microstructure. Further confirmation of the improvement in HLD comes from the analysis of peak 1 in Figure 12. As ageing progresses, a shoulder appears on the right side of peak 1. The reason for this phenomenon has been related to the enhancement of HLD as an effect of fresh cell cycling [49]. Although this phenomenon typically occurs immediately after the first full charge cycles [50], we observed it only after having carried out several driving cycles. Since this homogenization of lithium occurs when the slope in the voltage curves of one electrode is remarkably high compared to the counterpart electrode, it is plausible that since the driving cycle operates mainly within intermediates SOC, rarely reaching the end of charge or discharge delaying the phenomenon over time.

3.3. Lifetime Modeling

In order to estimate the overall capacity loss of an electrochemical commercial graphite/LMO-NMC lithium-ion cell, it is necessary to estimate the capacity loss related both to the driving cycle and calendar ageing. A mathematical representation of the capacity loss resulting from the two contributions is given in the Equation (1):

$$C_r=C_{BOL}-C_{driving\_loss}-C_{calendar\_loss}$$

(1)

where $C_r$ is the residual capacity of the cell at time $t$, $C_{BOL}$ is the initial capacity of the cell under test at the beginning of its life, $C_{driving\_loss}$ is the capacity loss when it is working due to the driving cycle, and $C_{calendar\_loss}$ is the capacity loss related to the time in which the cell is not working.

As earlier mentioned, only the effect of driving loss was experimentally evaluated using the WLTP CLASS 3B driving cycle. The effect of calendar ageing was not considered because the test would have provided results in an unreasonable time frame.

To evaluate the effects of ageing of the cell undergoing driving cycles, capacity tests performed at different ageing intervals were evaluated as described in Table 8. An expression describing the percentage capacity loss of the DUT was then extracted (2):

$$C_{driving\_loss}=A+B·t^C$$

(2)

$C_{driving\_loss}$ represents the capacity loss due to driving cycle ageing expressed in percentage, A is the initial capacity of electrochemical cell, B is a parameter that depends on the vehicle operation (journey time, time of use, C-rate, SOC, Temperature), t is the time while C is a constant as shown in

Table 10. Fixed parameters of the fitted function (2).

	A	B	C
Parameters	100	−0.0875	0.6

. In Figure 15 the loss of capacity is shown for each time step considered and the fitting curve (2).

The results reported in [51] were used to evaluate the effects of calendar ageing. When not operating, the battery pack of an electric vehicle is subjected to calendar ageing. Batteries used in EVs spend approximately 98% of their lifetime on stand-by, during which calendar ageing will occur [52].

In order to evaluate the effect of calendar ageing, some curves were extracted from [51] for a cell with the same characteristics as the DUT. The model proposed by the authors was identified and validated by performing calendar ageing tests on commercial graphite/LMO-NMC lithium-ion cells at different temperatures (0 °C, 25 °C, 45 °C, 60 °C) and SOC (100%, 80%, 65%, 30% 0%). The calendar ageing curves from the last cited work are, however, limited to 600 days ageing. For the purpose of the present work, it was necessary to predict the ageing up to 8 real years. Usually, it is reported that calendar capacity loss follows a square root time dependence, related to SEI growth, as reported in [53,54]. However, different functions might fit this behaviour better. For example, it was reported in [55] that a superposed linear and square root function or a function with $t^{0.75}$ match the data very well. The advantage of this particular function is the presence of a single ageing factor to evaluate both effects of the temperature and SOC. In our case, it was found that an equation similar to that of the driving cycle ageing fitted very well the calendar ageing curves and it is described in (3).

$$C_{calendar\_loss}=a+b·t^c$$

(3)

$C_{calendar\_loss}$ represents the capacity loss due to calendar ageing expressed in percentage value, a is the initial capacity of the electrochemical cell, b is a parameter that depends on the temperature and SOC, t is the time period, while the power coefficient $c$ is a constant as reported in

Table 11. R-square fitting curve (3).

Temperature [°C]	SOC [%]	a	b	c	R2
0	0/30/45/80/100	100	−0.0899	0.6	0.9692
25	80	100	−0.1796	0.6	0.9987
45	0	100	−0.0446	0.6	0.8357
45	30	100	−0.3097	0.6	0.9829
45	65	100	−0.5609	0.6	0.9487
45	80	100	−0.5277	0.6	0.9790
45	100	100	−0.5380	0.6	0.9941

. The coefficient of determination (R square) of the fitting performed is also given in Table 11 for the ageing curves considered. Under these conditions, the only temperature- and SOC-dependent parameter that can describe the evolution of the cell capacity fading related to calendar ageing is b. The following figures deal with experimental data of capacity loss as an effect of calendar ageing for the available combination mentioned above. Moreover, the dotted lines represent the fitting curves according to Equation (1) with the parameters of Table 11. As shown in Figure 16 and Figure 17 the decay is higher when the battery is in stand-by at high SOC.

The fitting carried out on experimental data allowed parameter b to be computed only for the available combinations of SOC and Temperature. Since only experimental data of eleven storage conditions were available, it was therefore necessary to estimate this parameter for different values of SOC and Temperature within the range of interest. For the purposes of this work, the range of temperatures considered is between 0 °C and 45 °C while the SOC is considered from 0% to 100%. The variation of parameter b with respect to temperature and SOC is shown in Figure 18. In the surface, it can be seen that parameter b takes higher values as SOC and temperature increase indicating that the loss of capacity due to calendar ageing is amplified under these conditions. However, the fit does not account for some degradation curves, for example, those with SOC between 5 and 50 percent and a temperature variation between 5 and 40 °C, which could change the surface trend at these points. However, the approximation for known ageing curves is considered excellent.

The overall ageing of an electrochemical cell subjected to driving cycle and calendar ageing was then evaluated. The effects are considered to be separated in time because calendar ageing applies when the vehicle is parked and is not being used, unlike the driving cycle ageing. In order to identify real vehicle usage, average data on distance travelled in Europe were used [27] with an average distance travelled on a weekday of 32.8 km and an average distance travelled on a public holiday of 34.6 km. Assuming a typical year consisting of 365 days including 261 weekdays and 52 weekends (104 days), the total distance is 12,168.12 km; it was then assumed that the WLTP_CLASS_3B driving cycle was used as the standard route as reported in

Table 12. Typical yearly vehicle utilization according to distance travelled in Europe.

	Weekdays	Driving Cycles	Weekdays	Driving Cycles
WLTP CL. 3B (23.266 km)	154	1	53	1
	107	2	51	2
Yearly Distance	8.562 km		3.606 km

.

An average daily temperature for the 8 years of the test was considered to make this calculation, in particular, referring to a real situation in Messina, Italy [56]. Similarly, considering the effect of range anxiety involving a driver of an electric vehicle, it was assumed that the driver would never want to find himself with a residual range of less than 30% [57,58]. To better define range anxiety, it is the fear of not being able to find an electric recharging station before the battery runs out. Therefore, the SOC value variation due to the driving cycle is between 30% and 100% and depends on the previous SOC value of the cell reached after the last driving cycle is done and computed from the vehicle model described above. Instead, the calendar ageing was computed for each partial day (excluding the time required to perform the driving cycle and the recharging phase if required), and it is affected by reached SOC and temperature. A typical year variation of Temperature, initial daily SOC and number of driving cycles are depicted in Figure 19.

A time period of 8 years was considered to evaluate the capacity loss for the calendar and driving cycle. A cell charging is done when the voltage is below 3.1 V assessed as a SOC lower than 30%. After the charging period, the upper voltage cut-off of the cell is 4.12 V (100% SOC). The number of daily WLTP driving cycles was distributed as shown in Table 12. The total capacity loss was then computed for an 8-year time frame, and the annual percentages are shown in

Table 13. Typical yearly vehicle utilization.

Year	${\mathit{C}}_{\mathit{c}\mathit{a}\mathit{l}\mathit{e}\mathit{n}\mathit{d}\mathit{a}\mathit{r}\_\mathit{l}\mathit{o}\mathit{s}\mathit{s}}$	${\mathit{C}}_{\mathit{d}\mathit{r}\mathit{i}\mathit{v}\mathit{i}\mathit{n}\mathit{g}\_\mathit{l}\mathit{o}\mathit{s}\mathit{s}}$	${\mathit{C}}_{\mathit{r}\mathit{e}\mathit{m}\mathit{a}\mathit{i}\mathit{n}\mathit{i}\mathit{n}\mathit{g}}$
0	0	0	100.00
1	5.03	3.02	91.95
2	2.76	1.56	87.63
3	2.25	1.26	84.12
4	1.97	1.10	81.06
5	1.78	0.99	78.29
6	1.64	0.92	75.73
7	1.54	0.86	73.34
8	1.45	0.81	71.08

.

A number of possible scenarios were then evaluated in order to predict the capacity loss as shown in Table 13. Scenarios 1 and 2 describe a situation in which both the environment temperature and the battery pack conditioning system hold the battery operating temperature at 15 °C (Scenario 1) or 35 °C (Scenario 2). The other scenarios simulate more intensive uses of the vehicle, for example with commercial vehicles. Scenario 3 describes a daily vehicle driving the use of 1 h, Scenario 4 describes a daily vehicle driving use of 2 h, and Scenario 5 describes an intensive daily vehicle driving the use of 6 h. The last three scenarios are repeated from scenarios 3, 4 and 5 with the difference that the ambient temperature is 35 °C. For each Scenario, the WLTP CLASS 3B driving cycle is used as a reference as shown in

Table 14. Annual vehicle use scenarios.

Scenario	Battery Working Temperature [°C]	Ambient Temperature [°C]	Yearly Distance [km]
1	15	15	12,168
2	35	35	12,168
3	15	15	16,984.18
4	15	15	50,952.54
5	15	15	101,905.08
6	35	35	16,984.18
7	35	35	50,952.54
8	35	35	101,905.08

. The scenarios were defined considering that the working temperature of a battery pack during the driving cycle ranges from 15 to 35 °C. From data computed at 25 °C for the driving cycle, the temperature-related ageing factor is reported in [22]. To evaluate the scenarios, the number of actual driving cycles was related to the number of daily driving cycles required for the scenarios limiting to 4184 the number of actual driving cycles performed. According to these considerations, a calendar capacity loss was computed as the difference between the daily time (24 h) and the time needed to perform driving cycles. Figure 15 deals with the loss of capacity for each step of driving cycles considered and the fitting curve.

Estimating the residual capacity of an EV battery at the end of its operational life is another important aspect for possible further uses, because it still has usable residual capacity. Refurbished EV batteries can be and advantageous alternative to brand new batteries in less stressful applications such as stationary applications. The results obtained can also be used to estimate the maximum range of a vehicle with a second-life battery. The analysis presented through the proposed scenarios is an example of possible use, and the data obtained are shown in

Table 15. Estimated capacity loss percentage in the vehicle according to the scenarios @ 15 °C.

Years	Scenario 1	Scenario 3	Scenario 4	Scenario 5
0	100.00	100.00	100.00	100.00
1	93.78	93.53	91.51	89.40
2	90.58	90.18	87.13	83.93
3	87.99	87.47	83.59	79.50
4	85.73	85.11	80.50	75.64
5	83.69	82.98	77.71	72.15
6	81.80	81.01	75.13	68.93
7	80.04	79.17	72.72	65.92
8	78.38	77.43	70.45	63.08
9	76.80	75.78
10	75.28	74.19
11	73.83	72.68
12	72.43	71.21
13	71.07	69.79
14	69.76
Overall km at 30% capacity loss	167.189	218.328	417.392	576.810
$C_{calendar\_loss}$ [%]	20.23	18.56	13.13	9.51
$C_{driving\_loss}$ [%]	9.77	11.44	16.87	20.49

and

Table 16. Estimated capacity loss percentage in the vehicle according to the scenarios @ 35 °C.

Years	Scenario 2	Scenario 6	Scenario 7	Scenario 8
0	100.00	100.00	100.00	100.00
1	84.45	84.16	80.08	75.13
2	76.48	75.99	69.79	62.30
3	70.04	69.38	61.47	51.92
4	64.42	63.60	54.21
5	59.34	58.39
6	54.66	53.58
7	50.28
Overall km at 30% capacity loss	36.550	49.230	100.788	139.316
$C_{calendar\_loss}$ [%]	21.28	19.59	14	10.56
$C_{driving\_loss}$ [%]	8.72	10.41	16	19.44

. Herein a reported the remaining capacity of the battery pack for the different Scenarios along the years. Moreover, the overall C reached within the thirty percent of capacity loss and the single contributes of calendar and capacity loss.

In order to compare the effect of the different Scenarios, a 30% of capacity loss as the limit to define the useful life of the battery was assumed. In Table 15, the remaining capacity under different scenarios at the fixed temperature of 15 °C and for different yearly distances is shown. Comparing the different scenarios, a 30% of loss of capacity is reached after about 13 years for the best Scenario (Scenario 1–12.168 km/year). While in the worst case (Scenario 5–101.905 km/year) the same loss of capacity is reached after only 5 years with a consequence reduction in vehicle life of about 8 years. Similarly, in Table 16 the same yearly distance as in Table 15 is reported but at a fixed temperature of 35 °C. The proposed scenarios show a strong impact of temperature on the ageing of the electrochemical cell, which decreases from 14 years to about 3 in the best case in terms of kilometres travelled (Scenario 1 vs. Scenario 2). In the worst case in terms of kilometres (Scenario 5 vs. Scenario 8), the temperature impact decreases the lifetime of the battery pack from 5 years to about 1 year. In conclusion a data comparison of all Scenarios highlights a strong impact of temperature on both calendar and cycling ageing capacity loss; it is worth noting that in case of less intensive scenarios, calendar ageing is the most relevant contribution on the overall capacity loss because the battery spends most of the time in resting condition. On the other hand, in the case of more intensive scenarios in terms of yearly distance, the battery spends more time in driving conditions with the consequence that cycle ageing contributes more than calendar ageing.

4. Conclusions

In this manuscript are described experimental ageing tests on a lithium-ion battery for electric vehicles with up to 10% capacity loss. Experimental tests are performed to investigate Lithium-ion cell degradation under the WLTP CLASS 3B driving cycle. The Lithium-ion battery considered in this paper consists of an LMO-NMC cathode and a graphite anode with a capacity of 63 Ah used in EV applications. A vehicle model [22] was used to convert the WLTP CLASS 3B driving cycle into an electrochemical cell-level scaled current profile. The cell under test was aged at room temperature (25 °C) for a number of cycles equal to 8 test years (4184 cycles) excluding calendar ageing. IC and DV analyses were also performed to understand the evolution of the ageing process. The main outcomes of the present study are summarized below:

• A reduction in available cell capacity of 11% after 8 test years from BOL condition is found and it does not cause a large increase in the internal resistance.
• IC curve shows three different peaks mainly related to LLI and LAM of the negative electrode. Important variations are observed on the first peak, which dropped almost 36% and shifting of 5 mV to higher potential in comparison to the fresh cell after ageing.
• DV analysis shows an alteration on the lithium storage capability of the graphite anode, then it is representative of anode degradation due to LAM. Q2 changing is indicative of possible LLI side reaction. An increment of peaks is noted in the first year; this evolution of peak magnitude has been related to an initial enhancement of the HLD of the cell and then to a change in graphite material or microstructure.
• From real data coming from the WLTP CLASS 3B driving cycle a mathematical model for capacitance loss from cycle ageing was extracted.
• Real data retrieved from a literature article [51] were analyzed and a mathematical curve dependent on temperature and SOC were extracted to estimate the calendar ageing.
• Total ageing was computed as the sum of the calendar and driving cycle contributions for 8 years, and different Scenarios were then evaluated in order to predict the capacity loss.