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Impedance-Based Simulation Models of Supercapacitors and Li-Ion ...

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BULLER et al.: IMPEDANCE-BASED SIMULATION MODELS OF SCs AND <strong>Li</strong>-ION BATTERIES 745<br />

Fig. 8.<br />

Current pr<strong>of</strong>ile for the verification <strong>of</strong> the SC model.<br />

Fig. 10. Comparison <strong>of</strong> the measured voltage response <strong>and</strong> the data obtained<br />

from different simulation models.<br />

TABLE I<br />

COMPARISON OF MEASURED AND SIMULATED EFFICIENCY DATA.WORKING<br />

POINT: 1.5 V, ROOM TEMPERATURE, CYCLE DEPTH 615% Q<br />

Fig. 9.<br />

Measured <strong>and</strong> simulated voltage response to the current pr<strong>of</strong>ile.<br />

V. VERIFICATION AND APPLICATION OF THE MODELS<br />

As a final step, the results <strong>of</strong> the simulation models are compared<br />

with measured data in the time domain. Both, the SC<br />

model as well as the model <strong>of</strong> the <strong>Li</strong>-ion battery have been verified<br />

in detail [1]. In this section, some examples <strong>of</strong> these verification<br />

measurements are given.<br />

For the verification <strong>of</strong> the SC model, the current pr<strong>of</strong>ile depicted<br />

in Fig. 8 has been employed [2]. The imposed charging<br />

<strong>and</strong> discharging pulses model a highly dynamic load at the beginning<br />

as well as deeper charging <strong>and</strong> discharging periods at<br />

the end <strong>of</strong> the evaluation. The corresponding voltage curves are<br />

depicted in Fig. 9. The measured <strong>and</strong> the calculated data show<br />

excellent agreement.<br />

The influence <strong>of</strong> the porous structure <strong>of</strong> the SC electrodes<br />

can be illustrated by means <strong>of</strong> a comparison <strong>of</strong> the full simulation<br />

model with the voltage response <strong>of</strong> the simplified model<br />

which only consists <strong>of</strong> a series connection <strong>of</strong> the ohmic resistance<br />

<strong>and</strong> the capacitance <strong>of</strong> the SC. For this comparison,<br />

Fig. 10 provides an enlarged view <strong>of</strong> the first current pulses <strong>of</strong><br />

the verification pr<strong>of</strong>ile. Once more, the excellent agreement <strong>of</strong><br />

the measured <strong>and</strong> simulated voltage data becomes obvious. In<br />

addition, remarkable deviations due to the neglect <strong>of</strong> porosity<br />

are observed for the simplified model. For low frequencies, i.e.,<br />

for comparably long relaxation times, these deviations could be<br />

overcome by replacing the ohmic resistance by the larger dc<br />

resistance with being the resistance <strong>of</strong> the<br />

electrolyte in the pores <strong>of</strong> the electrodes [2]. In this case however,<br />

the fast voltage transients would not be well represented<br />

anymore.<br />

One advantage <strong>of</strong> SCs used as energy storage devices is their<br />

good energy efficiency. This efficiency is also influenced by<br />

the porous structure <strong>of</strong> the electrodes which means that the increasing<br />

real part <strong>of</strong> the impedance with decreasing frequency<br />

has to be taken into account.<br />

To compare measured <strong>and</strong> simulated efficiency data, an SC<br />

is partly charged <strong>and</strong> discharged with constant dc currents <strong>of</strong><br />

various amplitudes. The cycle depth is chosen to be 540 A s<br />

which corresponds approximately to . For each current<br />

amplitude, the charge/discharge cycle is repeated ten times<br />

but only the last five cycles, which start <strong>and</strong> finish at the same<br />

internal conditions (quasi-stationary), are used for the efficiency<br />

calculation. In a second step, the same current pr<strong>of</strong>ile is simulated<br />

by means <strong>of</strong> the newly developed capacitor model. Measured<br />

<strong>and</strong> simulated efficiency data are compared in Table I.<br />

Again, very good agreement is observed.<br />

Next, a simulation example <strong>of</strong> the <strong>Li</strong>-ion battery model is<br />

presented. For the model verification, the dynamic discharge<br />

current pr<strong>of</strong>ile depicted in Fig. 11 has been selected. The<br />

comparison <strong>of</strong> the simulated <strong>and</strong> the measured voltage response<br />

to this current pr<strong>of</strong>ile at a state <strong>of</strong> charge <strong>of</strong> 77.5% <strong>and</strong><br />

room temperature is shown in Fig. 12. Excellent agreement<br />

<strong>of</strong> the measured <strong>and</strong> the simulated voltage curves is found.<br />

The outst<strong>and</strong>ing accuracy <strong>of</strong> the simulation model is due to<br />

the exact representation <strong>of</strong> the complex battery impedance<br />

including all important nonlinearities.<br />

An important precondition for the high quality <strong>of</strong> the simulation<br />

results is the nearly perfect reproducibility <strong>of</strong> the battery<br />

Authorized licensed use limited to: GOVERNMENT COLLEGE OF TECHNOLOGY. Downloaded on June 22,2010 at 10:29:03 UTC from IEEE Xplore. Restrictions apply.

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