
Lithium-Ion Battery Protection:
A Fully Integrated Solution
Lithium-ion
(Li-Ion) rechargeable batteries are quickly gaining popularity over nickel
based rechargeables due to their superior energy density, higher cell voltage
and low self-discharge rate. These characteristics make them perfectly suited
to today’s high performance portable products. However, safety concerns related
to overcharging and short circuit protection have driven the industry to
include battery protection circuits within the Li-Ion battery pack. Their
purpose is to monitor the cell voltage(s) and prevent over-charge or over-discharge
by opening the current path if a cell is out of the normal operating voltage
range. By monitoring the discharge current, overload and short circuit protection
is also provided. The protector control circuitry is usually implemented
using a dedicated protector IC and two external back-to-back power MOSFETs
to open the circuit, preventing charge and/or discharge current. Two MOSFETs
are required to control current in both directions due to the MOSFET’s internal
body diode.
Systems Issues The entire
system, including parasitic elements, must be considered in designing the
battery protection circuit. This includes the battery cell(s), the protection
circuitry and the load (or charger) that the user applies to the battery
pack terminals. Parasitics include the inductance and capacitance associated
with the load, the switch on-resistance and the battery’s internal ESR (Equivalent
Series Resistance) and ESL (Equivalent Series Inductance). At normal steady-state
currents of a few amperes or less, the parasitics do not play a major role
in the operation of the system. However, during high transient currents of
I OA or more, such as those encountered when a large capacitor or a short
is applied to the battery pack, the parasitics have a major effect on the
operation and robustness of the system.
Current Sensing
In some cases, the series MOSFETs are used as the current sensing elements.
One of the drawbacks to this approach is the inaccuracy of the over-current
sense due to the tolerance and temperature coefficient of the MOSFET on-resistance.
If both MOSFET’s are used as the sensing element, a problem arises. During
an over- charge condition, when one MOSFET is turned off to prohibit charge
current, the discharge current must go through its body diode. The voltage
drop across the body then causes an over-current trip, turning off the other
MOSFET as well. To solve this problem, some manufacturer’s disable the overcurrent
protection while in over-charge; precisely the wrong time. In any case, the
current must be monitored continu- ously, or at a sufficient rate such that
an overload doesn’t go undetected for too long. A delay of 1 Omsec may be
long enough for the MOSFET’s to be destroyed during a short circuit.
MOSFET Turn-off and Inductive Effects
When the protection circuit interrupts the current in response to a
short or overload, inductance associated with the load (parasitic or otherwise)
causes voltage overshoot in response to the rapid di/dt. For example, a 20A
short circuit current interrupted in 1 (sec would result in a 20V overshoot
if there was 1 (H of total circuit inductance. This overshoot can exceed
the breakdown voltage of the MOSFET used to interrupt the current. Guarding
against inductive kick is critical to surviving a short circuit condition,
when the current is at its highest. An effective way to reduce overshoot
when inter- rnpting the current is to increase the MOSFET turn-off time to
tens of microseconds by raising the gate drive impedance, limiting the di/dt.
The turn-off time cannot be made too long, however, or the MOSFET junction
temperature rise may be excessive.
An Integrated Solution
To deal with these real world applications issues, most Li-Ion protector
IC’s require a significant number of external components, in addition to
the two MOSFETs. These components raise the cost of the battery pack and
pose packaging problems, especially in the tight confines of a single cell
pack. To minimize cost and board area, a fully integrated protection circuit
was designed for single cell Li-Ion applications. The UCC3958 includes a
single integrated MOSFET switch, eliminating the two external MOSFETs normally
used in protector circuits. A block diagram of the IC is shown in Fig. 1.
The following sections describe the operation of each major circuit block
within the IC, and how a single MOSFET does the job of two.
Figure 1. Simplified Block Diagram of Integrated Single Cell Battery Protector IC
Cell Voltage Monitoring
This block consists of a precision temperature compensated, trimmed
voltage reference and a multi- tap resistor divider. The divider is made
to accommodate a number of different over-voltage and under-voltage thresholds
as mask options. Each time the battery is sampled (at a rate of approximately
200Hz), the resistor is connected across the battery and a specific tap is
compared to the reference. The sampling cycle only lasts 400(sec out of every
5msec. During this time, the reference, sampling resistor and a voltage comparator
are turned on. At all other times, these blocks are shut off to conserve
power.
System Clock Generator
The system clock generator is used to sequence theturn-on and turn-off
of the battery sampling circuits, as well as provide the clock for the MOSFET
charge pump. This block is designed to run at a nominal frequency of 20kHz,
with all the other frequencies and control signals derived from it.
State Machine
The state machine is used to determine the condition of the battery
and take appropriate action when an abnormal state has been detected (over-voltage
or under-voltage). The output of the state machine is digitally filtered
to ensure that a momentary noise spike or dip in battery voltage does not
cause an erroneous fault. A voltage fault condition (OV or UV) must persist
for at least two consecutive sampling cycles before the appropriate action
is taken. The over and under voltage thresholds have approximately 300mV
of hysteresis to prevent oscillation due to battery ESR.
On-chip MOSFET
A single internal MOSFET acts as a bi-directional switch for charging
and discharging the battery. Because the voltage across the MOSFET can be
of either polarity, the substrate of the device is always switched to its
most negative terminal. The substrate switch guarantees that the MOSFET will
never conduct current through its substrate diode. By eliminating the need
for two back-to-back MOSFETs, a lower on- resistance is achieved. There is
also no time at which current is conducted through a MOSFET body diode. This
greatly reduces losses and power dissipation during the over-charge and under-charge
modes, when one of the external MOSFETs would be turned off. The gate of
the MOSFET is driven by an internal charge-pump to a voltage approximately
four times the battery voltage. This assures the lowest possible on- resistance,
even at low cell voltages. The gate drive impedance was chosen to provide
a MOSFET turn-off time of about 20(sec, minimizing di/dt. Another advantage
to having the MOSFET switch integrated onto the die is the ability to sense
die temperature and turn off the MOSFET in the event that the steady state
current has caused excessive temperature rise.
Charge Pump
This block provides the gate drive voltage for the MOSFET. The charge
pump circuitry is the largest noise generator in the circuit. To improve
measurement accuracy, the charge pump is turned off when the battery is being
sampled. During this short interval, the MOSFET drive voltage remains virtually
unchanged.
Over-Current Protection
The over-current protection block guarantees that the steady-state
discharge current cannot exceed 5A nominal. This threshold was chosen to
allow adequate design margin over the maximum required current draw of 2A
in most single cell applications. The current sensing scheme utilizes metallization
resistance around the MOSFET and is temperature compensated for the shift
in metal resistance. There is a fixed internal delay of 360(sec from the
time the overcurrent is detected to the time the MOSFET is shut off. The
user can extend this time by adding a small external capacitor. This feature
allows charging of large bypass capacitors without tripping the overcurrent
protection. If the overcurrent condition persists, the MOSFET is turned off
and remains off until the load is removed. A bypass capacitor, connected
to the cell by an internal resistor, keeps the IC powered during a hard
short, when the cell voltage may fall very low. This feature assures proper
operation of the IC and its overcurrent protection, even under the worst
short circuit conditions.
Over and Under-Voltage Operation
When the cell voltage is out of its normal operating voltage range
(typically 2.3V to 4.2V), the direction of battery current must be controlled
to prohibit charge current if the voltage is too high, or discharge current
if the voltage is too low. This is done using a linear control loop, which
regulates the polarity of the differential voltage across the internal MOSFET.
When an over-voltage condition is sensed, the MOSFET gate voltage is
controlled to only allow discharge current by regulating the differential
voltage across the MOSFET’s drain to source terminals to lOOmV. The polarity
of the l00mV offset is such that the direction of current must be out of
the battery pack (discharge only). As the load varies, the impedance of the
MOSFET is adjusted to maintain the l00mV drop. In this manner, the MOSFET
can be mlide to function as a diode with a forward voltage drop of 100mV,
guaranteeing that battery current is in only one direction. The offset of
l00mV was chosen to be much larger than all other internal offsets. The
MOSFET voltage drop in this mode is much lower than that of the conventional
solution of two back-to-back MOSFETs, where the body diode of one MOSFET
is conducting. Once the battery voltage has dropped 300mV below the over-charge
threshold, normal operation is resumed and the MOSFET is fully enhanced to
minimize voltage drop.
If an under-voltage condition is sensed, the load is disconnected from
the battery pack (by turning off the MOSFET) to prevent further discharge.
Most circuit functions are put into a sleep mode to minimize current drain
form the battery. Several key circuits remain powered to detect the application
of a charger. Once the charging voltage is detected, the linear control
loop is again activated, and only charge current is allowed. The polarity
of the 100mV control circuit is reversed, since the desired direction of
battery current is opposite that of the discharge condition. Afain the MOSFET
acts like a diode with a low forward drop, but the polarity has been reversed.
This linear control mode of operation remains in effect util the battery
voltage is 300 mV above the under voltage threshold, at which time normal
operation resumes.
Fig. 2 Single Cell Protector Application Circuit
A complete application schematic of a single cell Lithium-Ion protector
is shown in figure 2. by incorporation the MOSFET into the low current BiCMOS
IC, only one small external capacitor is required. This capacitor (Cl) provides
ample energy storage to power the IC during a hard short. Capacitor C2 is
optional, and extends the over-current delay time for charging large capacitive
loads. Without an external cap, the built-in delay of 360(sec allows charging
up to 1 ,000(F of load capacitance.
The controlled MOSFET turn-off time of 20(sec results in little or no voltage
overshoot. No snubber capacitors or clamp diodes are necessary on the pack
output or across the Li-Ion cell.
The typical on-resistance is 45m( (from pin-to-pin of the IC) at room
temperature. A plot of the on-resistance as a function of cell voltage is
shown in Fig. 3. Because of the internal charge pump, the on-resistance remains
very low, even at cell voltages below 2.6V.
Fig 3. Total on-resistance vs. Cell voltage
Other features incorporated in the UCC3958 are: a Chip Enable pin to turn
the pack output off, a Low Power Warn output to warn of a low battery condition,
and an output which indicates if the protector is in an over or undervoltage
condition.
The total current draw is just 5(A in normal mode, and only 1 (A during
under-voltage (sleep) mode. Note that the normal self-discharge rate of 6%/month
for a typical 1.2 Amp-Hour Li-Ion cell corresponds to a current of 103(A.
Therefore, the added current draw of the protection circuit in normal operation
represents an increase of only 5% in the self-discharge rate of the battery.
In sleep mode, when the cell is in under-voltage, the self-discharge rate
is increased by less than 1%.
David Salerno (salerno@unitrode.com) is a Principal Applications Engineer
for portable products at Unitrode Corporation, a manufacturer of linear and
mixed signal integrated circuits, located in Merrimack, NH.
Source: Battery Power, March 1st, 1998
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