Fast Cell Balancing Using External MOSFET
Fast Cell Balancing Using External MOSFET
Fast Cell Balancing Using External MOSFET
ABSTRACT
The need for cell balancing comes from the fact that cell-to-cell differences in
self-discharge, capacity, and impedance can lead to different charge states among the
cells. However, the charger terminates charging based on the summed voltage only,
which may leave some cells undercharged and others overcharged. To remedy this
imbalance and to achieve the goal of having all cells reaching 100% state-of-charge at
charge termination, it is necessary to reduce the charge added to the overcharged cells
by creating a current bypass during charging.
Contents
1 Internal Cell Balancing in bq20zxx Solution ..................................................... 1
2 External FET for Accelerated Cell Balancing ................................................... 2
3 Discussions .......................................................................................... 5
4 Summary............................................................................................. 6
5 Acknowledgment.................................................................................... 6
List of Figures
1 Internal Cell-Balancing Circuit of bq29330 AFE ................................................ 2
2 External Cell-Balancing Circuit With Cell 1 Bypassing Active ................................ 3
3 Fast Cell Balancing of Two Series Cells......................................................... 5
4 Issues With Balancing Two Adjacent Cells (a) and Every Other Cell (b) ................... 6
List of Tables
1 Select Correct Duty Cycle D-Value .............................................................. 2
SLUA420A – May 2007 – Revised January 2009 Fast Cell Balancing Using External MOSFET 1
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External FET for Accelerated Cell Balancing www.ti.com
Note: In firmware versions bq20z80 v102, bq20z70 v110, and bq20z90 v110, D is variable,
depending on the number of series cells and is 0.4 for 4-cell, 0.3 for 3-cell, and 0.22 for
2-cell. D is a constant value of 0.4 in the latest firmware versions. Use Table 1 to determine
the correct D-value based on the device and firmware versions. Also note that bq20z80 v110
and earlier devices (which includes v102) are replaced by bq20z80A v110 and are not
recommended for new design (NRND).
PACK+
VCC DSG
100
bq29330
100n
CELL 2
100 AFE
100
2 Fast Cell Balancing Using External MOSFET SLUA420A – May 2007 – Revised January 2009
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www.ti.com External FET for Accelerated Cell Balancing
Note: The previous edition of this application report indicates that 10 kΩ can be used. Recent study
shows that due to the different finite input impedance between each VCx pin, the leakage
current at each VCx pin is different. With a 10-kΩ filter resistor, even though the stack
voltage can be calibrated accurately, individual cell voltages will not be accurate; the error is
typically 10~20 mV. As the Impedance Track™ gauge requires high voltage measurement
accuracy for gauging and cell balancing, this error must be minimized. Therefore, the
recommended maximum filter resistor value is 1 kΩ, and the resulting voltage error is about
2 mV per cell
When the internal cell-balancing FET is turned on, the two external filter resistors and the Rds(on) of the
integrated cell-balancing FET form a resistor-divider, generating a voltage dividing ratio of 0.426 across
the 1-kΩ resistor. This is a typical value when cell voltage varies from 3 V to 4.2 V; the ratio can vary
between ~0.413 to 0.435 when only a single cell is being balanced. Therefore, if the turnon Vgs for Q1
and Q2 is 1.5 V, for instance, the cell voltage must be higher than 1.5/0.426 = 3.52 V in order for Q1 or
Q2 to turn on. For the external, fast cell balancing to work for lower cell voltages, such as the LiFePO4
chemistry, this exercise is especially important. Dual N-channel MOSFETs with lower Vgs thresholds,
such as DMN2004DWK, NTZD3154N, and Si1024X, can be considered in this case. Care must be taken
to evaluate these devices in terms of maximum Vgsth, absolute maximum rating for Vds and Vgs, and to
ensure a drain current of more than 100 mA at low Vgs voltage (such as 1.2 V).
CHG FET DSG FET
PACK+
VCC DSG
1k
bq29330
100n
50
CELL 2
Q2
1k AFE
Q1
1k
Rs 100n
The operation principle of this circuit is simple. The state of the internal cell-balancing FETs is controlled
by the gas gauge. In the circuit of Figure 2, if any internal FET is turned on by the gas gauge, a small
current flows from the cathode (the positive tab) of the cell through the top 1-kΩ filter resistor, the internal
FET, and the bottom 1-kΩ filter resistor and returns to the anode (the negative tab) of the cell. The two
filter resistors and the internal FET on-resistance form a voltage divider, providing the Vgs for the external
bypassing FET; the main bypassing current flows through the 50-Ω resistor.
SLUA420A – May 2007 – Revised January 2009 Fast Cell Balancing Using External MOSFET 3
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The average on-resistance of Q1, Q2 is about 5 Ω when Vgs ≥ 2 V. With a 50-Ω resistance placed in
series with the external MOSFET, the external bypassing path resistance is summed to 55 Ω. At a
nominal cell voltage of 3.6 V, the bypassing current is 65 mA. The same calculation for balancing a 10%
difference in SOC for a 2000-mAh battery leads to 14 hours of total charge time (using D = 0.22 for a
2-cell battery pack, assuming the use of the bq20z70 v110 firmware).
Note that the bq20zxx gas gauge data flash (DF) constant “Min Cell Deviation” must be calculated and
configured based on D and the bypassing current. The DF:MinCellDeviation governs the charging time
required to balance the difference of one mAh in cell capacity. The default value of DF:MinCellDeviation is
calculated using a nominal voltage of V = 3.6 V, total bypassing R = 700 Ω and duty cycle D = 40% (D =
0.4), and the value is calculated as
DF:MinCellDeviation = R × 3.6/(V × D) = 1750 seconds/mAh, where R is in Ω and V is volts, usually
taking a nominal value of 3.6 V.
Applying the same calculation to the external cell-balancing circuit: By using the fast cell-balancing circuit
in Figure 2, if the application is a 2-series pack using bq20z70 v110 firmware, D = 0.22 (see Table 1), and
R = 50 + 5 Ω, it is necessary to program DF:Min Cell Deviation = 250 seconds/mAh.
Note: The typical Rds(on) of the integrated cell-balancing FET is not a constant value – it is a
function of Vds, the drain-to-source voltage of the FET as well as the current through the
FET. The higher the cell voltage (and hence the higher the Vds), the lower the Rds(on).
Bench measurement of a few bq29330 devices indicates that the typical Rds(on) ranges
from 420 Ω (at 3 V) to 300 Ω (at 4.2 V) if only a single internal cell-balancing FET is
turned on at a time. If multiple adjacent internal cell-balancing FETs are turned on at the
same time, Rds(on) is even lower. When balancing two adjacent cells, Rds(on) is ~260 Ω,
and when balancing three adjacent cells simultaneously, 220 Ω . For Internal cell
balancing, it is recommended to use the smallest possible Rds(on), which is 220 Ω, instead
of the 500 Ω in the technical reference, when calculating DF:MinCellDeviation.
A demonstration of the circuit was done on two new, 1900-mAh battery cells with a bq20z70 v110
evaluation module. The cells were artificially unbalanced and left sufficiently rested. The open-circuit
voltage (OCV) of cell 1 was 3595 mV, corresponding to a state-of-charge (SOC) of 5.6%; the OCV of cell
2 was 3492 mV, corresponding to an SOC of 3.5%. The imbalance in SOC was 5.6% – 3.5% = 2.1%.
Then, a charger was applied to the circuit in Figure 2; the [CB] flag was set, indicating that the cell
balancing was activated (in this case, the bypassing FET Q2 for cell 1 was turned on). The cell-balancing
status is indicated by the orange curve, ChgStat in Figure 3; when ChgStat is high (numerical value
0x240), cell balancing is active. The test charge current is 208 mA. After 2.57 hours, cell balancing was
automatically turned off (ChgStat= 0x200) by the gas gauge, indicating that the cell balancing was
completed. When the charger was disconnected, the cells were allowed to rest until voltages were
stabilized. The resulting voltages were 3784 mV for cell 1 and 3785 mV for cell 2. This test demonstrated
that with the fast cell-balancing circuit, a 2.1% SOC deficit of a 1900-mAh cell can be eliminated in 2.57
hours of cell-balancing time. The 1-mV difference between the OCV of the two cells falls within the voltage
calibration tolerance. With the internal cell balancing, the bypassed charge in the same time period would
have been only 3.2 mAh, less than 0.2% of SOC.
4 Fast Cell Balancing Using External MOSFET SLUA420A – May 2007 – Revised January 2009
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www.ti.com Discussions
3900 1200
3750 900
Charging Status
Voltage, mV
3700 800
3650 700
OCV=3595mV, SOC=5.5%
3600 600
OCV=3492mV, SOC=3.5%
3550 500
3500 400
Cell Balancing Time: 2.57 hrs
3450 300
3400 200
0 2000 4000 6000 8000 10000 12000
Time, sec
3 Discussions
Two design aspects are important with the external cell balancing when using the bq29330 or bq29312
AFEs. First, two or three adjacent cells cannot be fast-balanced at the same time. Figure 4a shows the
circuit of attempting to balance two adjacent cells simultaneously. When the adjacent internal FETs M1
and M2 are turned on, no current is flowing through Rext2 because Ibias through M1 and M2 cancel at
Rext2; therefore, Q2 remains off even when the internal switch M2 is enabled. In practice, it is not an
issue because the amount of time required for balancing each cell is evaluated on a per charging-cycle
basis by the Impedance Track™ algorithm. Once the balancing of the lower cell is finished, which
happens fairly quickly given the fast external balancing, Q2 will be enabled when the gas gauge
determines to turn off M1 and keep M2 on. Similarly, in the case when three adjacent cells are
simultaneously balanced, the lowest cell of the three is actually balanced first, and then the middle, and
lastly the upper one.
The other aspect is the Vds voltage stress when every other cell is being balanced. As illustrated in
Figure 4b, the top and the bottom cells are being balanced. Due to the cell-balancing bias, the middle
internal switch M2 is seeing a higher Vds, which may exceed the maximum Vds it can sustain. In fact, the
Vds of M2 can be calculated based on the worst-case Rds(on) on M1 and M3. Assume that the cells are
at approximately 4.2 V, when Rds(on) for M1 and M3 is at the lowest value ( about 300 Ω when no
adjacent cells are being balanced). Assuming a maximum recommended Rext of 1 kΩ, Vds of M2 can be
as high as 4.2 V + 2 x 4.2 x 1000/(2 x 1000 + 300) = 7.85 V. The maximum Vds under this setting is still
below the absolute maximum value of 8.5 V for the internal balancing FETs; so, this is fine. Apparently,
with higher Rext, Vds stress seen by M2 can be worse and can even exceed the maximum voltage. This
is another reason that the maximum recommended Rext is 1 kΩ.
SLUA420A – May 2007 – Revised January 2009 Fast Cell Balancing Using External MOSFET 5
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Summary www.ti.com
I balance
RBAL3 RBAL3 I bias
OPEN
+ M3
+ M3
Battery - Battery
Cell
Q3
Cell
- Q3
Rext3 Rext
V↑
I balance +
RBAL2 I bias RBAL2
OPEN
+ M2 + M2 Vds ↑
Battery - Battery
Cell
Q2
Cell
- Q2 -
Rext2 Rext
V↓
I balance I balance
RBAL1 I bias RBAL1 I bias
+ M1 + M1
Battery - Battery
Cell
Q1
Cell
- Q1
Rext1 Rext
(a) (b)
Figure 4. Issues With Balancing Two Adjacent Cells (a) and Every Other Cell (b)
4 Summary
This application report documents a fast cell-balancing circuit using existing bq29330/bq29312 AFE for
bq20z80/z70/z90/z75/z95 Impedance Track™ gas gauges and a couple of various design aspects when
implementing this circuit.
5 Acknowledgment
This application report has adopted results from some insightful discussions with Lon Schneider, Nexergy,
Inc.
6 Fast Cell Balancing Using External MOSFET SLUA420A – May 2007 – Revised January 2009
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