The document summarizes key concepts about lead-acid batteries, including:
1) Lead-acid batteries use lead and lead dioxide electrodes with a sulfuric acid electrolyte. Chemical reactions at the electrodes involve the transfer of electrons between the electrodes and ions in the electrolyte.
2) As the battery charges and discharges, the concentration of the sulfuric acid electrolyte changes. This affects the voltage according to the Nernst equation.
3) Factors like internal resistance and surface chemistry effects cause the terminal voltage to differ from the theoretical voltage. Battery models account for these factors.
1. ECEN 4517 1
Lecture: Lead-acid batteries
ECEN 4517/5517
How batteries work
Conduction mechanisms
Development of voltage at plates
Charging, discharging, and state of charge
Key equations and models
The Nernst equation: voltage vs. ion concentration
Battery model
Battery capacity and Peukert s law
Energy efļ¬ciency, battery life, and charge proļ¬les
Coulomb efļ¬ciency, voltage drops, and round-trip efļ¬ciency
Battery life vs. depth of discharge
Charging strategies and battery charge controllers
2. ECEN 4517 2
Lead-acid battery: construction
Pb PbO2
H2O
H2SO4
Positive
electrode:
Lead-dioxide
Negative
electrode:
Porous
lead
Electrolyte: Sulfuric acid, 6 molar ā¢ How it works
ā¢ Characteristics and
models
ā¢ Charge controllers
3. ECEN 4517 3
Electrical conduction mechanisms
Pb PbO2
H2O
SO4
-2
SO4
-2
H
+
H
+
H
+
H
+
Lead and lead-dioxide are good
electrical conductors. The conduction
mechanism is via electrons jumping
between atoms.
The electrolyte contains aqueous ions
(H+ and SO4
-2). The conduction
mechanism within the electrolyte is via
migration of ions via diffusion or drift.
Q: What are the physical mechanisms of conduction in the complete path from
one terminal, through an electrode, into the electrolyte, onto the other electrode,
and out the other terminal?
4. ECEN 4517 4
Conduction mechanism
at the surface of the electrode
Oxidation-reduction (Redox) reaction transfers charge from ions in solution
to conducting electrons in the electrode
At the surface of the lead (negative) electrode:
Pb0
Pb0
Pb0
Pb
0
Pb
0
Pb0
Pb0
SO4
-2 SO4
-2
H+
H+
H+
H+
H2O
Lead
electrode
Sulfuric acid electrolyte
Charged sulfate ion approaches
uncharged lead atom on surface of
electrode
Pb0
Pb0
Pb0
Pb
+2
Pb
0
Pb0
Pb0
SO4
-2 SO4
-2
H+
H+
H+
H+
H2O
Lead
electrode
Sulfuric acid electrolyte
ā
ā
Lead atom becomes ionized and forms
ionic bond with sulfate ion. Two electrons
are released into lead electrode
5. ECEN 4517 5
The chemical reaction (āhalf reactionā)
at the lead electrode
Pb + SO4
ā2 PbSO4 + 2eā
solid aqueous solid in conductor
Pb0
Pb0
Pb
0
Pb
+2
Pb
0
Pb0
Pb0
SO4
-2 SO4
-2
H
+
H
+
H+
H+
H2O
Lead
electrode
Sulfuric acid electrolyte
ā
āThis reaction releases net energy
E0 = 0.356 eV
ā the āGibbs free energyā, under standard
conditions (T = 298ĖK, concentration = 1
molar)
Units: Energy = (charge)(voltage)
Energy in eV = (charge of electron)(1 V)
So the charge of the aqueous sulfate ion is transferred to two conducting
electrons within the lead electrode, and energy is released.
6. ECEN 4517 6
Conduction mechanism
at the surface of the positive electrode
Charged sulfate and hydrogen ions
approach lead-dioxide molecule (net
uncharged) on surface of electrode
Lead atom changes ionization and forms
ionic bond with sulfate ion. Two water
molecules are released into solution
SO4
-2
SO4
-2
H
+
H
+
H
+
H
+
H2O
Lead-
dioxide
electrode
Sulfuric acid electrolyte
Pb
+4
O
ā2
O
ā2
Pb
+4
O
ā2
O
ā2
Pb
+4
O
ā2
O
ā2
ā
ā
SO4
-2
SO4
-2
H2O
Lead-
dioxide
electrode
Sulfuric acid electrolyte
Pb
+2
Pb
+4
O
ā2
O
ā2
Pb
+4
O
ā2
O
ā2
H2O
H2O
ā¢ Lead changes oxidation state from +4 to +2
ā¢ Two electrons are removed from conduction band in electrode
7. ECEN 4517 7
The chemical reaction (āhalf reactionā)
at the lead-dioxide electrode
PbO2 + SO4
ā2 + 4H+ + 2eā
solid aqueous aqueous in conductor
PbSO4 + 2H2O
solid liquid
This reaction releases net energy
E0 = 1.685 eV
Net charge of two electrons is transferred
from the electrode into the electrolyte
Both half reactions cause the electrodes
to become coated with lead sulfate (a poor
conductor) and reduce the concentration
of the acid electrolyte
SO4
-2
SO4
-2
H
+
H
+
H
+
H
+
H2O
Lead-
dioxide
electrode
Sulfuric acid electrolyte
Pb
+4
O
ā2
O
ā2
Pb
+4
O
ā2
O
ā2
Pb
+4
O
ā2
O
ā2
ā
ā
8. ECEN 4517 8
How the battery develops voltage
Consider the following experiment:
New electrodes are placed inside electrolyte, with no external electrical
circuit connected
Pb PbO2
SO4
-2
H2O
Pb
0
Pb0
Pb
0
Pb
+2
Pb
0
Pb
0
Pb
0
SO4
-2 SO4
-2
H+
H+
H+
H+
H2O
SO4
-2
SO4
-2
H+
H+
H+
H+
H2O
Pb+4
O
ā2
Oā2
Pb
+4
Oā2
Oā2
Pb
+4
Oā2
O
ā2
ā
ā
ā
ā
ā¢ The reactions start to occur
ā¢ They use up aqueous ions near
electrodes
ā¢ Diffusion within electrolyte
replenishes ions near electrodes
ā¢ Excess electrons are created in
lead electrode, and electron
deļ¬cit is created in lead-dioxide
electrode
ā¢ Electric ļ¬eld is generated at
electrode surfaces. This electric
ļ¬eld opposes the ļ¬ow of ions.
9. ECEN 4517 9
Battery voltage at zero current
Energy barriers at electrode surface
The chemical reactions at the
electrode surfaces introduce
electrons into the Pb electrode,
and create a deficit of electrons
in the PbO2 electrode
These charges change the
voltages of the electrodes
The system reaches equilibrium
when the energy required to
deposit or remove an electron
equals the energy generated by
the reaction
Total voltage (at T = 298ĖK and 1
molar acid electrolyte) is Vbatt =
0.356 + 1.685 = 2.041 V
Pb PbO2
H2O
SO4
-2
SO4
-2
H+
H+
H+
H+
v
Vbattā +
Ibatt
Eo
/qe = 0.356 V
Eo
/qe = 1.685 V
Diffusion
Drift
Diffusion
Drift
10. ECEN 4517 10
Discharging
Connection of an electrical load allows
electrons to flow from negative to
positive terminals
This reduces the charge and the
voltages at the electrodes
The chemical reactions are able to
proceed, generating new electrons
and generating the power that is
converted to electrical form to drive
the external electrical load
As the battery is discharged, the
electrodes become coated with lead
sulfate and the acid electrolyte
becomes weaker
H2O
SO4
-2
SO4
-2
H+
H+
H+
H+
v
Vbatt < 2.041 V
ā +
Ibatt
< 0.356 V
< 1.685 V
Pb PbO2
PbSO4
Diffusion
Drift
Diffusion
Drift
R
11. ECEN 4517 11
Charging
Connection of an electrical power
source forces electrons to flow
from positive to negative
terminals
This increases the charge and the
voltages at the electrodes
The chemical reactions are driven in
the reverse direction, converting
electrical energy into stored
chemical energy
As the battery is charged, the lead
sulfate coating on the electrodes
is removed, and the acid
electrolyte becomes stronger
H2O
SO4
-2
SO4
-2
H+
H+
H+
H+
v
Vbatt > 2.041 Vā +
Ibatt
> 0.356 V
> 1.685 V
Pb PbO2
PbSO4
External source of electrical power
Diffusion
Drift
Diffusion
Drift
12. ECEN 4517 12
Battery state of charge (SOC)
Fully Completely
Charged Discharged
State of charge: 100% 0%
Depth of discharge: 0% 100%
Electrolyte concentration: ~6 molar ~2 molar
Electrolyte speciļ¬c gravity: ~1.3 ~1.1
No-load voltage: 12.7 V 11.7 V
(speciļ¬c battery types may vary)
13. ECEN 4517 13
Battery voltage vs. electrolyte concentration
The Nernst equation relates the chemical reaction energy to electrolyte
energy:
E = E0 + (kT/qe) ln [(electrolyte concentration)/(1 molar)]
(idealized)
with
E = energy at a given concentration
E0 = energy at standard 1 molar concentration
kT/qe = 26 mV at 298 ĖK
Implications:
At fully charged state (6 molar), the cell voltage is a little higher than E0 /qe
As the cell is discharged, the voltage decreases
14. ECEN 4517 14
Voltage vs. electrolyte concentration
R. S. Treptow, āThe lead-acid battery: its voltage in theory and practice,ā J. Chem. Educ., vol. 79 no. 3, Mar. 2002
Voltage of lead-acid electrochemical cell
vs. electrolyte concentration, as
predicted by Nernst equation
Fully charged
Time to recycle
Usable range
15. ECEN 4517 15
Mechanisms that affect terminal voltage
1. Equilibrium voltage changes with electrolyte concentration (as
described above ā Nernst equation)
2. With current ļ¬ow, there are resistive drops in electrodes, especially in
surface lead-sulfate
3. With current ļ¬ow, there is an electrolyte concentration gradient near
the electrodes. Hence lower concentration at electrode surface;
Nernst equation then predicts lower voltage
4. Additional surface chemistry issues: activation energies of surface
chemistry, energy needed for movement of reacting species through
electrodes
5. Physical resistance to movement of ions through electrodes
(2) - (5) can be modeled electrically as resistances
16. ECEN 4517 16
A basic battery model
+
āV(SOC)
Ideal diodes
Rcharge(SOC)
Rdischarge(SOC)
+
Vbatt
ā
Ibatt
SOC0% 100%
V(SOC)
Rcharge(SOC)
Rdischarge(SOC)
Basic model Dependence of model parameters
on battery state of charge (SOC)
17. ECEN 4517 17
Types of lead-acid batteries
1. Car battery
āSLIā - starter lighting ignition
Designed to provide short burst of high current
Maybe 500 A to crank engine
Cannot handle ādeep dischargeā applications
Typical lifetime of 500 cycles at 20% depth of discharge
2. Deep discharge battery
We have these in power lab carts
More rugged construction
Bigger, thicker electrodes
Calcium (and others) alloy: stronger plates while maintaining low leakage current
More space below electrodes for accumulation of debris before plates are shorted
Ours are
Sealed, valve regulated, absorbent glass mat
Rated 56 A-hr at 2.33A (24 hr) discharge rate
18. ECEN 4517 18
Types of lead-acid batteries
3. āGolf cartā or āforkliftā batteries
Similar to #2
Bigger, very rugged
Low cost ā established industry
Antimony alloy
Strong big electrodes
But more leakage current than #2
Can last 10-20 years
Nominal capacity: A-hrs @ 25ĖC to 1.75 V/cell
36 A-hr
1 hr
56 A-hr49 A-hr46 A-hr45 A-hr
24 hr8 hr4 hr2 hr
Manufacturerās specifications for our power lab batteries:
19. ECEN 4517 19
Battery capacity
The quantity C is defined as the current that discharges the battery in 1 hour,
so that the battery capacity can be said to be C Ampere-hours (units confusion)
If we discharge the battery more slowly, say at a current of C/10, then we might
expect that the battery would run longer (10 hours) before becoming
discharged. In practice, the relationship between battery capacity and
discharge current is not linear, and less energy is recovered at faster discharge
rates.
Peukertās Law relates battery capacity to discharge rate:
Cp = Ik t
where Cp is the amp-hour capacity at a 1 A discharge rate
I is the discharge current in Amperes
t is the discharge time, in hours
k is the Peukert coefficient, typically 1.1 to 1.3
20. ECEN 4517 20
Example
Our lab batteries
k = 1.15
C = 36 A
Cp = 63 A-hr
Prediction of Peukert
equation is plotted at left
Nominal capacity: A-hrs @ 25ĖC to 1.75 V/cell
36 A-hr
1 hr
56 A-hr49 A-hr46 A-hr45 A-hr
24 hr8 hr4 hr2 hr
What the manufacturerās
data sheet specified:
21. ECEN 4517 21
Energy efļ¬ciency
Efļ¬ciency = ED/EC
EC = Total energy during charging = vbatt (-ibatt) dt VCICTC
ED = Total energy during discharging = vbatt ibatt dt VDIDTD
Energy efficiency =
VD
VC
IDTD
ICTC
= voltage efficiency coulomb efficiency
+
āV(SOC)
Ideal diodes
Rcharge(SOC)
Rdischarge(SOC)
+
Vbatt
ā
Ibatt
Coulomb efļ¬ciency = (discharge A-hrs)/(charge A-hrs)
Voltage efļ¬ciency = (discharge voltage)/(charge voltage)
22. ECEN 4517 22
Energy efļ¬ciency
Energy is lost during charging when reactions other than reversal of
sulfation occur
At beginning of charge cycle, coulomb efļ¬ciency is
near 100%
Near end of charge cycle, electrolysis of water
reduces coulomb efļ¬ciency. Can improve this
efļ¬ciency by reducing charge rate (taper charging)
Typical net coulomb efļ¬ciency: 90%
Approximate voltage efļ¬ciency: (2V)/(2.3V) = 87%
Energy efļ¬ciency = (87%)(90%) = 78%
Commonly quoted estimate: 75%
24. ECEN 4517 24
Charge management
Over-discharge leads to āsulfationā and the battery is ruined. The reaction becomes
irreversible when the size of the lead-sulfate formations become too large
Overcharging causes other undesirable reactions to occur
Electrolysis of water and generation of hydrogen gas
Electrolysis of other compounds in electrodes and electrolyte, which can generate
poisonous gasses
Bulging and deformation of cases of sealed batteries
Battery charge management to extend life of battery:
Limit depth of discharge
When charged but not used, employ āļ¬oatā mode to prevent leakage currents from
discharging battery
Pulsing to break up chunks of lead sulfate
Trickle charging to equalize charges of series-connected cells
25. ECEN 4517 25
Charge proļ¬le
A typical good charge proļ¬le:
Bulk charging at maximum power
Terminate when battery is 80% charged
(when a voltage set point is reached)
Charging at constant voltage
The current will decrease
This reduces gassing and improves
charge efļ¬ciency
āAbsorptionā or ātaper chargingā
Trickle charging / ļ¬oat mode
Equalizes the charge on series-connected
cells without signiļ¬cant gassing
Prevents discharging of battery by
leakage currents
Occasional pulsing helps reverse sulfation
of electrodes
The three-step charge profile used
by the chargers in our power lab
26. ECEN 4517 26
Charge and ļ¬oat voltages
Good chargers can:
ā¢ Program charge/ļ¬oat
voltages to needs of
speciļ¬c battery type
ā¢ Temperature-compensate
the voltage set points
ā¢ Maintain battery in fully
charged state (ļ¬oat mode)
when in storage
ā¢ Avoid overcharging
battery (charge voltage set
point)
ā¢ Taper back charging
current to improve charge
efļ¬ciency and reduce
outgassing
27. ECEN 4517 27
Battery charge controller
PV
array
Charge
controller
Inverter AC
loads
ā¢ Prevent sulfation of battery
ā¢ Low SOC disconnect
ā¢ Float or trickle charge mode
ā¢ Control charge profile
ā¢ Multi-mode charging, set points
ā¢ Nightime disconnect of PV panel
Direct energy transfer
Charge battery by direct connection
to PV array
MPPT
Connect dc-dc converter between
PV array and battery; control this
converter with a maximum power
point tracker