Profile Ni-MH
Battery Discharge
Characteristics |
| |
DISCHARGE
CHARACTERISTICS |
Ni-MH
BATTERY |
Specification
tables |
The
discharge behavior of the GREENCELL nickel-metal hydride cell is
generally well-suited
to the needs of today's electronic products - especially those requiring
a stable
voltage for extended
periods of operations. |
Overview |
Features |
Comparison
of Ni-MH
and Ni-Cd
Cells |
1.
Definitions of Capacity
|
Major
applications |
The
principal battery parameter of interest to a product designer is
usually the run time
available under a specified equipment use profile. While establishing
actual run times
in the product is vital prior to final adoption of a design, battery
screening and initial
design are often performed using rated capacities. Designers should
thoroughly understand
the conditions under which a cell rating is established and the
impact of differences
in rating conditions on projected performance.The
standard cell rating, often abbreviated as C, is the capacity obtained
from a new, but
thoroughly conditioned cell subjected to a constant-current discharge
at room temperature
after being optimally charged. Since cell capacity varies inversely
with the
discharge rate, capacity ratings depend on the discharge rate used.
For nickel-metal
hydride cells, the rated capacity is normally determined at a discharge
rate that
fully depletes the cell in five hours.The
published C value may reflect either an average or minimum value
for all cells. Typically
nickel-cadmium cells are rated based on minimum values while nickel-metal
hydride cells are rated on average values. The difference between
the two values
may be significant (Approximate to 10 percent)depending on the variability
in the
manufacturing process.Many
charge and discharge parameters are normalized by the C rate since
cellperformance
within a family of varying cell sizes and capacities is often identical
when compared
on the C basis. |
Structural
designs |
Electrochemical
processes |
Discharge
characteristics |
Charge
characteristics |
Charging
methods |
Cycle
life characteristics |
Storage
characteristics |
Safety
characteristics |
Designing
for Ni-MH cells |
Battey
pack designs |
Battery
pack configurations
designation
system |
Precautions
for using
Ni-MH batteries |
Battery
selection |
| |
| |
| |
2. Equivalent
Circuit |
| |
For
purposes of electrical analysis of the battery cell, the Thevenin
equivalent discharge
circuit shown in Figure 9 is often used. This models the circuit
as a series combination
of a voltage source(a series resistance)Rh=the effective instantaneous
resistance(and
the parallel combination of a capacitor )Cp=the effective parallel
capacitance(and
a resistor)Rd=the effective delayed resistance. |
| |
| |
| |
| |
| |
|
| |
Figure
9.Equivalent Discharge Circuit for a Nickel-Metal Hydride Cell |
| |
Eo = effective
cell no-load voltage |
| |
Re =(Rh + Rd)=
total effective internal resistance |
| |
Rh = effective
instantaneous resistance |
| |
Rd = effective
delayed resistance |
| |
Cp = effective
parallel capacitance |
| |
E = cell termination
voltage |
| |
For
steady state purposes, the cell voltage at a given current is Eo
- iRe, where Re, the
state effective internal resistance, is the sum of Rh and Rd. The
transient response
is shown in Figure 10 where the initial voltage drops immediately
to Eo - iReh
and then transfers exponentially(with a time constant =Cp*Rd)to
the steady-state
voltage. Obviously the process reverses when the load is reduced
or removed. For
many application the steady-voltage is adequate for describing cell
performance since
the time constant for most cells is small: usually less than 3 percent
of the discharge
time. When compared to a nickel-cadmium cell, the steady-state voltage
for the
nickel-metal hydride cell will be reduced since, although the instantaneous
resistance
is comparable, the delayed resistance will be on the order of 10
percent higher. |
| |
| |
| |
| |
| |
| |
| |
| |
|
| |
Figure
10.Example of Transient Voltage Profile for a Nickel-Metal Hydride
Cell |
| |
3.
Voltage During Discharge
|
| |
The
discharge voltage profile, in addition to the transient effects
discussed above, isaffected
by environmental conditions, notably discharge temperature and discharge
rate.
However, under most conditions the voltage curve retains the flat
plateau desirable for electronics
applications. |
| |
| |
| |
Shape
of Discharge Curve |
| |
A
typical discharge profile for a cell discharged at the 5-hour rate(the
0.2C rate)is
shown in Figure 11. The initial drop from an open-circuit voltage
of approximately 1.4
volts to the 1.2 volt plateau occurs rapidly. |
| |
| |
| |
|
| |
Figure
11.Typical Discharge Voltage Profile for a Nickel-Metal Hydride
Cell |
| |
Then,
as with nickel-cadmium cells, the nickel-metal hydride cell exhibits
a sharp "knee"
at the end of the discharge where the voltage drops quickly.As
can be seen by the flatness of the plateau and the symmetry of the
curve, the mid-point
voltage(MPV - the voltage when 50 percent of the available capacity
is discharged)provides
a useful approximation to average voltage throughout the discharge. |
| |
| |
| |
| |
Environmental
Effects |
| |
The
principal environmental influences on the location and shape of
the voltage profile are
the discharge temperature and discharge rate.As
indicated in Figure 12, small variations from room temperature(¡À10
Celsius)so not
appreciably affect the nickel-metal hydride cell voltage profile.
However major excursions,especially
lower temperatures, will reduce the mid-point voltage while maintaining
the general shape of the voltage profile. |
| |
| |
| |
| |
| |
|
| |
Figure
12. Mid-Point Voltage Variation with Temperature |
| |
Discharge
Rate |
| |
The
effect of discharge rate on voltage profile is shown in Figure 13.
There is nosignificant
effect on the shape of the discharge curves for rates under 1C;
for rates over
1C, both the beginning and ending transients consume a larger portion
of the discharge
duration. |
| |
| |
| |
| |
|
| |
Figure
13.Discharge Chracteristics |
| |
4. Discharge
Capacity Behavior |
| |
As
with the voltage profile, the capacity available during a discharge
is dramatically affected
by the cell temperature during discharge and the rate of discharge.
The capacity
is also heavily influenced by the operating history of the cell,
i.e. the recent charge/discharge/storage
history of the cell. Obviously a cell can only discharge the capacity
which has been returned to it from the previous charge cycle less
whatever is
lost to self discharge. Charging/charge return issues are discussed
in the next section
while storage and self-discharge is addressed in a later section. |
| |
| |
| |
| |
| |
Effect
of Temperature |
| |
The
primary effects of cell temperature on dischargeable capacity, assuming
adequate
charging, are at lower temperatures(<0)as shown in Figure 14.
Use of
nickel metal hydride cells in cold environments may force significant
capacity derating
from room-temperature values. |
| |
| |
| |
|
| |
Figure
14.Variation of Discharge Capacity with Temperature |
| |
Effect
of Discharge Rate |
| |
Figure
15 illustrates the influence of discharge rate on total capacity
available. There is
no significant effect on capacity for discharge rates below 1C.
At the discharge rates
above 1C and below the current maximum discharge rate of 4C, significant
reductions
in voltage delivery occur. This voltage reduction may also result
in capacity
reduction depending on the choice of discharge termination voltage. |
| |
| |
| |
| |
| |
|
| |
Figure
15. Effect of Discharge Rate on Capacity |
| |
Discharge
Application Considerations |
| |
In
general, the discharge behavior of nickel-metal hydride cells closely
follows that of similar
nickel-cadmium cells used in the same environment. Thus much of
the design
expertise gathered for nickel-cadmium cells is directly applicable
to nickel-metal
hydride cells. Discussed below are some specific issues often raised
by designers
using nickel-metal hydride cells. As the nickel-metal hydride experience
base builds,
additional information that will help designers optimize the use
of nickel-metal
hydride cells is becoming available. For this reason, close consultation
with the
factory during the design effort is encouraged. |
| |
| |
| |
| |
| |
| |
5. State-of
Charge measurement |
| |
A
major issue for users of portable electronics is the run time left
before they need torecharge
their batteries. Users of portable computers, in particular, expect
some
form
of "fuel gauge" to help them determine when they need
to save their work. A variety
of schemes for measuring state-of-charge have been suggested. In
general, experience
with nickel-metal hydride cells indicates that, due to the flatness
of the voltage
plateau under normal discharge rates, voltage sensing cannot be
used to accurately
determine state-of-charge. To
date, the only form of state-of-charge sensing found to consistently
give reasonable
results is coulometry-comparing the electrical flows during charge
and discharge
to indicate the capacity remaining.Many devices already have the
electronics
available to perform sophisticated tracking of charge flows including
estimation
of self-discharge losses. Some off-the-shelf charging circuitry
includes this
form of charge tracking as part of the package.With careful
initial calibration and appropriate
compensation for environmental conditions, predictions accurate
within 5 to
10 percent of actual capacity can be obtained. |
| |
| |
| |
| |
| |
| |
| |
| |
| |
| |
| |
| |
6. Memory/Voltage
Depression |
| |
The
issue of "memory" or voltage depression has been a concern
for many designers of
devices, using nickel-cadmium cells. In some applications where
nickel-cadmium cells
are routinely partially discharged, a depression in the discharge
voltage profile of
approximately 150 mV per cell has been reported when the discharge
extends from
the routinely discharged to rarely discharged zones. While the severity
of this problem
in nickel-cadmium cells is open to differing interpretations, the
source of the effect
is generally agreed to be in the structure of the cadmium electrode.
With the elimination
of cadmium in the nickel-metal hydride cell, memory is no longer
a concern. |
| |
| |
| |
| |
| |
| |
| |
7. Discharge
Termination |
| |
To
prevent the potential for irreversible harm to the cell caused by
cell reversal in discharge,
removal of the load from the cell(s)prior to total discharge is
highly recommended.
The typical voltage profile for a cell carried through a total discharge
involves
a dual plateau voltage profile as indicated in Figure 16. The voltage
plateaus are
caused by the discharge of first the positive electrode and then
the residual capacity
in the negative. At the point both electrodes are reversed, substantial
hydrogen
gas evolution occurs, which may result in cell venting as well as
irreversible
structural damage to the electrodes. It should be noted that the
nickel-metal hydride cell,
because it uses a negative electrode that absorbs hydrogen, may
actually be
somewhat less susceptible to long-term damage from cell reversal
than the sealed nickel-cadmium
cell.The
key to avoiding harm to the cell is to terminate the discharge at
the point whereessentially
all capacity has been obtained from the cell, but prior to reaching
the second
plateau where damage may occur. Two issues complicate the selection
of the
proper voltage for discharge termination: high-rate discharges and
multiple-cell effects
in batteries. |
| |
| |
| |
| |
| |
| |
| |
| |
| |
| |
| |
| |
|
Figure
16.Nickel-Metal Hydride Cell Polarity Reversal Voltage Profile |
| Voltage
Cutoff at High Rates |
Normally
discharge cutoff is based on voltage drops with a value of 0.9 volts
per cell(75
percent of the 1.2 volt per cell nominal mid-point voltage)often
being used. As can
be seen in Figure 12, 0.9 volts is an excellent value for most medium
to long-term
discharge applications(<1C). However,
again as seen in Figure 13, with high drain-rate usage(1-4C), the
change in shape
in the voltage curve with the more rounded "knee" to the
curve means that an arbitrary
0.9V/cell cutoff may be premature, leaving a significant fraction
of the cellcapacity
untapped. For this reason, a better choice for voltage cutoff in
high-rateapplications
is 75 percent of the mid-point voltage at that discharge rate. Note,
however,
that this choice of end-of-discharge voltage (EODV)is dictated only
by considerations
of preventing damage to the cell. There may be end-application justification
for selection of a higher voltage cutoff with the resulting sacrifice
of some
potential additional capacity. |
| Discharge
Termination in Batteries |
Normal
manufacturing variation produces a range of capacities for battery
cells. As these
cells are combined in batteries, the effects of cell capacity variations
are amplified
by the number of cells in the battery. Use of termination voltage
based on a simple
multiple of 0.9V/cell times the number of cells may result in a
weaker cell being
driven into reverse significantly before the battery reaches the
termination
voltage. Both charging techniques that minimize the amount of overcharge
applied to the
cell and frequent repetitive discharging of the battery may exacerbate
the problem.
The result may be premature battery failure due to the damage caused
by reversal
of the weak cell. Experience
indicates selection of the EODV by the following formula providesacceptable
margin to minimize battery failure from repeated cell polarity reversal: |
EODV=
[(MPV-150mV)(n-1)]-200mV |
where
MVP is the single-cell mid-point voltage at the given discharge
rate and n is the
number of cells in the battery.Selection
of the proper discharge termination voltage, especially for large
batteries or complicated
application profiles, should be done in consultation with the cell
manufacturer. |