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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 efficiency, battery life, and charge profiles
Coulomb efficiency, voltage drops, and round-trip efficiency
Battery life vs. depth of discharge
Charging strategies and battery charge controllers
ECEN 4517 2
Lead-acid battery: construction
Pb PbO2
H2O
H2SO4
Positive
electrode:
Lead-dioxide
Negative
electrode:
Porous
lead
Electrolyte: Sulfuric acid, 6 molar • How it works
• Characteristics and
models
• Charge controllers
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?
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
–
–
Lead atom becomes ionized and forms
ionic bond with sulfate ion. Two electrons
are released into lead electrode
ECEN 4517 5
The chemical reaction (“half reaction”)
at the lead electrode
Pb + SO4
–2 PbSO4 + 2e–
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
–
–This reaction releases net energy
E0 = 0.356 eV
— the “Gibbs free energy”, under standard
conditions (T = 298˚K, 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.
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
–2
O
–2
Pb
+4
O
–2
O
–2
Pb
+4
O
–2
O
–2
–
–
SO4
-2
SO4
-2
H2O
Lead-
dioxide
electrode
Sulfuric acid electrolyte
Pb
+2
Pb
+4
O
–2
O
–2
Pb
+4
O
–2
O
–2
H2O
H2O
• Lead changes oxidation state from +4 to +2
• Two electrons are removed from conduction band in electrode
ECEN 4517 7
The chemical reaction (“half reaction”)
at the lead-dioxide electrode
PbO2 + SO4
–2 + 4H+ + 2e–
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
–2
O
–2
Pb
+4
O
–2
O
–2
Pb
+4
O
–2
O
–2
–
–
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
–2
O–2
Pb
+4
O–2
O–2
Pb
+4
O–2
O
–2
–
–
–
–
• The reactions start to occur
• They use up aqueous ions near
electrodes
• Diffusion within electrolyte
replenishes ions near electrodes
• Excess electrons are created in
lead electrode, and electron
deficit is created in lead-dioxide
electrode
• Electric field is generated at
electrode surfaces. This electric
field opposes the flow of ions.
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 = 298˚K 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
Vbatt– +
Ibatt
Eo
/qe = 0.356 V
Eo
/qe = 1.685 V
Diffusion
Drift
Diffusion
Drift
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
– +
Ibatt
< 0.356 V
< 1.685 V
Pb PbO2
PbSO4
Diffusion
Drift
Diffusion
Drift
R
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 V– +
Ibatt
> 0.356 V
> 1.685 V
Pb PbO2
PbSO4
External source of electrical power
Diffusion
Drift
Diffusion
Drift
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 specific gravity: ~1.3 ~1.1
No-load voltage: 12.7 V 11.7 V
(specific battery types may vary)
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 ˚K
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
ECEN 4517 14
Voltage vs. electrolyte concentration
R. S. Treptow, “The lead-acid battery: its voltage in theory and practice,” 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
ECEN 4517 15
Mechanisms that affect terminal voltage
1. Equilibrium voltage changes with electrolyte concentration (as
described above – Nernst equation)
2. With current flow, there are resistive drops in electrodes, especially in
surface lead-sulfate
3. With current flow, 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
ECEN 4517 16
A basic battery model
+
–V(SOC)
Ideal diodes
Rcharge(SOC)
Rdischarge(SOC)
+
Vbatt
–
Ibatt
SOC0% 100%
V(SOC)
Rcharge(SOC)
Rdischarge(SOC)
Basic model Dependence of model parameters
on battery state of charge (SOC)
ECEN 4517 17
Types of lead-acid batteries
1. Car battery
“SLI” - starter lighting ignition
Designed to provide short burst of high current
Maybe 500 A to crank engine
Cannot handle “deep discharge” 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
ECEN 4517 18
Types of lead-acid batteries
3. “Golf cart” or “forklift” batteries
Similar to #2
Bigger, very rugged
Low cost — established industry
Antimony alloy
Strong big electrodes
But more leakage current than #2
Can last 10-20 years
Nominal capacity: A-hrs @ 25˚C to 1.75 V/cell
36 A-hr
1 hr
56 A-hr49 A-hr46 A-hr45 A-hr
24 hr8 hr4 hr2 hr
Manufacturer’s specifications for our power lab batteries:
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.
Peukert’s 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
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 @ 25˚C 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 manufacturer’s
data sheet specified:
ECEN 4517 21
Energy efficiency
Efficiency = 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
+
–V(SOC)
Ideal diodes
Rcharge(SOC)
Rdischarge(SOC)
+
Vbatt
–
Ibatt
Coulomb efficiency = (discharge A-hrs)/(charge A-hrs)
Voltage efficiency = (discharge voltage)/(charge voltage)
ECEN 4517 22
Energy efficiency
Energy is lost during charging when reactions other than reversal of
sulfation occur
At beginning of charge cycle, coulomb efficiency is
near 100%
Near end of charge cycle, electrolysis of water
reduces coulomb efficiency. Can improve this
efficiency by reducing charge rate (taper charging)
Typical net coulomb efficiency: 90%
Approximate voltage efficiency: (2V)/(2.3V) = 87%
Energy efficiency = (87%)(90%) = 78%
Commonly quoted estimate: 75%
ECEN 4517 23
Battery life
ECEN 4517 24
Charge management
Over-discharge leads to “sulfation” 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 “float” 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
ECEN 4517 25
Charge profile
A typical good charge profile:
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 efficiency
“Absorption” or “taper charging”
Trickle charging / float mode
Equalizes the charge on series-connected
cells without significant 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
ECEN 4517 26
Charge and float voltages
Good chargers can:
• Program charge/float
voltages to needs of
specific battery type
• Temperature-compensate
the voltage set points
• Maintain battery in fully
charged state (float mode)
when in storage
• Avoid overcharging
battery (charge voltage set
point)
• Taper back charging
current to improve charge
efficiency and reduce
outgassing
ECEN 4517 27
Battery charge controller
PV
array
Charge
controller
Inverter AC
loads
• Prevent sulfation of battery
• Low SOC disconnect
• Float or trickle charge mode
• Control charge profile
• Multi-mode charging, set points
• 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

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Lead-acid battery guide: construction, charging, capacity & models

  • 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 efficiency, battery life, and charge profiles Coulomb efficiency, voltage drops, and round-trip efficiency 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 • How it works • Characteristics and models • 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 – – 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 (“half reaction”) at the lead electrode Pb + SO4 –2 PbSO4 + 2e– 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 – –This reaction releases net energy E0 = 0.356 eV — the “Gibbs free energy”, under standard conditions (T = 298˚K, 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 –2 O –2 Pb +4 O –2 O –2 Pb +4 O –2 O –2 – – SO4 -2 SO4 -2 H2O Lead- dioxide electrode Sulfuric acid electrolyte Pb +2 Pb +4 O –2 O –2 Pb +4 O –2 O –2 H2O H2O • Lead changes oxidation state from +4 to +2 • Two electrons are removed from conduction band in electrode
  • 7. ECEN 4517 7 The chemical reaction (“half reaction”) at the lead-dioxide electrode PbO2 + SO4 –2 + 4H+ + 2e– 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 –2 O –2 Pb +4 O –2 O –2 Pb +4 O –2 O –2 – –
  • 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 –2 O–2 Pb +4 O–2 O–2 Pb +4 O–2 O –2 – – – – • The reactions start to occur • They use up aqueous ions near electrodes • Diffusion within electrolyte replenishes ions near electrodes • Excess electrons are created in lead electrode, and electron deficit is created in lead-dioxide electrode • Electric field is generated at electrode surfaces. This electric field opposes the flow 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 = 298˚K 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 Vbatt– + 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 – + 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 V– + 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 specific gravity: ~1.3 ~1.1 No-load voltage: 12.7 V 11.7 V (specific 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 ˚K 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, “The lead-acid battery: its voltage in theory and practice,” 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 – Nernst equation) 2. With current flow, there are resistive drops in electrodes, especially in surface lead-sulfate 3. With current flow, 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 + –V(SOC) Ideal diodes Rcharge(SOC) Rdischarge(SOC) + Vbatt – 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 “SLI” - starter lighting ignition Designed to provide short burst of high current Maybe 500 A to crank engine Cannot handle “deep discharge” 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. “Golf cart” or “forklift” batteries Similar to #2 Bigger, very rugged Low cost — established industry Antimony alloy Strong big electrodes But more leakage current than #2 Can last 10-20 years Nominal capacity: A-hrs @ 25˚C to 1.75 V/cell 36 A-hr 1 hr 56 A-hr49 A-hr46 A-hr45 A-hr 24 hr8 hr4 hr2 hr Manufacturer’s 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. Peukert’s 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 @ 25˚C 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 manufacturer’s data sheet specified:
  • 21. ECEN 4517 21 Energy efficiency Efficiency = 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 + –V(SOC) Ideal diodes Rcharge(SOC) Rdischarge(SOC) + Vbatt – Ibatt Coulomb efficiency = (discharge A-hrs)/(charge A-hrs) Voltage efficiency = (discharge voltage)/(charge voltage)
  • 22. ECEN 4517 22 Energy efficiency Energy is lost during charging when reactions other than reversal of sulfation occur At beginning of charge cycle, coulomb efficiency is near 100% Near end of charge cycle, electrolysis of water reduces coulomb efficiency. Can improve this efficiency by reducing charge rate (taper charging) Typical net coulomb efficiency: 90% Approximate voltage efficiency: (2V)/(2.3V) = 87% Energy efficiency = (87%)(90%) = 78% Commonly quoted estimate: 75%
  • 24. ECEN 4517 24 Charge management Over-discharge leads to “sulfation” 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 “float” 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 profile A typical good charge profile: 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 efficiency “Absorption” or “taper charging” Trickle charging / float mode Equalizes the charge on series-connected cells without significant 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 float voltages Good chargers can: • Program charge/float voltages to needs of specific battery type • Temperature-compensate the voltage set points • Maintain battery in fully charged state (float mode) when in storage • Avoid overcharging battery (charge voltage set point) • Taper back charging current to improve charge efficiency and reduce outgassing
  • 27. ECEN 4517 27 Battery charge controller PV array Charge controller Inverter AC loads • Prevent sulfation of battery • Low SOC disconnect • Float or trickle charge mode • Control charge profile • Multi-mode charging, set points • 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