Electrochemistry, Batteries and Fuel CellsIntroduction and ContextElectrochemistry is the study of chemical reactions involving electron transfer and the relationship between chemical energy and electrical energy. It provides the scientific foundation for batteries, fuel cells, electroplating, corrosion control, sensors, electrolysis, and many mechatronic systems. Autonomous robots, electric vehicles, backup power supplies, medical instruments, and industrial controllers all depend on electrochemical components whose voltage, current, efficiency, lifetime, safety, and environmental impact must be understood. A galvanic or voltaic cell converts a spontaneous chemical reaction into electrical work. An electrolytic cell uses an externally supplied electrical current to drive a non-spontaneous chemical reaction. Batteries contain one or more cells and store energy internally, whereas fuel cells convert continuously supplied fuel and oxidant into electricity. Learning ObjectivesBy the end of this chapter, the reader should be able to: - Explain oxidation, reduction, electrodes, electrolytes, and cell notation.
- Calculate standard and non-standard electrode and cell potentials using the Nernst equation.
- Relate ionic conductivity, resistance, current density, and electrolysis.
- Compare primary batteries, secondary batteries, supercapacitors, and fuel cells.
- Interpret charging behavior, efficiency, degradation, safety risks, and recycling requirements.
- Select an appropriate electrochemical energy technology for a mechatronic application.
1. Electrochemical Foundations1.1 Oxidation and reductionOxidation is the loss of electrons, while reduction is the gain of electrons. They always occur together in a redox reaction. A useful mnemonic is “OIL RIG”: oxidation is loss, reduction is gain. In a galvanic cell, oxidation occurs at the anode and reduction occurs at the cathode. The anode is therefore negative during galvanic operation because it supplies electrons to the external circuit; the cathode is positive. In an electrolytic cell, the signs are reversed by the power supply, but the reaction locations remain unchanged: oxidation is still at the anode and reduction is still at the cathode. For a zinc–copper cell: Zn(s) → Zn²⁺(aq) + 2e⁻ Cu²⁺(aq) + 2e⁻ → Cu(s) The overall reaction is: Zn(s) + Cu²⁺(aq) → Zn²⁺(aq) + Cu(s) Electrons travel through the external conductor from zinc to copper. Ions move through the electrolyte or separator to maintain approximate electrical neutrality. 1.2 Cell notation and salt bridgesThe conventional notation for the zinc–copper cell is: Zn(s) | Zn²⁺(aq) || Cu²⁺(aq) | Cu(s) A single vertical line represents a phase boundary. The double line represents a salt bridge or porous separator. A salt bridge completes the internal ionic circuit, limits direct mixing, and reduces liquid-junction potentials. In practical batteries, a porous separator permits ionic transport while preventing electronic contact between electrodes. 1.3 Electrode potentialAn electrode potential expresses the tendency of a half-cell reaction to undergo reduction. Standard reduction potentials are measured relative to the standard hydrogen electrode, assigned a potential of 0.000 V under standard conditions. A more positive standard reduction potential indicates a greater thermodynamic tendency for reduction. The standard cell potential is: E°cell = E°cathode − E°anode where E°cathode and E°anode are standard reduction potentials in volts. The equation assumes both tabulated values are written as reductions. A positive E°cell indicates that the reaction is thermodynamically spontaneous under standard conditions. Thermodynamic spontaneity is not the same as practical performance. Reaction kinetics, internal resistance, mass transport, polarization, heat generation, and side reactions determine the voltage and power delivered by a real cell. 1.4 Gibbs energy and cell voltageFor a reversible electrochemical reaction: ∆G = −nFE where ∆G is the Gibbs free-energy change in joules per mole of reaction, n is the number of electrons transferred per reaction as written, F is Faraday’s constant, approximately 96 485 C mol⁻¹, and E is the reversible cell potential in volts. Since 1 V = 1 J C⁻¹, nFE has units of joules per mole. Under standard conditions: ∆G° = −nFE°cell A positive cell voltage corresponds to negative Gibbs energy for a spontaneous galvanic reaction. The maximum electrical work is obtained only under reversible conditions; actual devices deliver less energy because of irreversible losses. 2. The Nernst EquationCell potential changes with temperature, concentration, pressure, and reaction composition. For a general reaction: aA + bB ⇌ cC + dD the reaction quotient is: Q = (aCc aDd) ÷ (aAa aBb) where a represents thermodynamic activity. For dilute solutions, activity is often approximated by concentration divided by a standard concentration. Pure solids and pure liquids have activity approximately equal to one and are omitted from Q. The Nernst equation is: E = E° − (RT ÷ nF) ln Q where E is the reversible potential in volts, E° is the standard potential, R is the gas constant, 8.314 J mol⁻¹ K⁻¹, T is absolute temperature in kelvin, n is the number of transferred electrons, F is Faraday’s constant, and Q is dimensionless. The equation applies to reversible or near-equilibrium conditions and does not include ohmic, kinetic, or mass-transfer overpotentials. At 25 °C, using common logarithms: E = E° − (0.05916 ÷ n) log₁₀ Q Worked Example 1: Concentration effectFor the cell reaction: Zn(s) + Cu²⁺(aq) → Zn²⁺(aq) + Cu(s) let E°cell = 1.10 V, [Zn²⁺] = 0.10 M, [Cu²⁺] = 1.0 M, and n = 2. The reaction quotient is: Q = [Zn²⁺] ÷ [Cu²⁺] = 0.10 Therefore: E = 1.10 − (0.05916 ÷ 2) log₁₀(0.10) Since log₁₀(0.10) = −1: E = 1.10 + 0.02958 = 1.1296 V ≈ 1.13 V The cell voltage is higher than the standard value because the products are relatively dilute compared with the reactant ion. 3. Conductivity and ElectrolytesAn electrolyte contains mobile ions and conducts electricity through ionic motion. Strong electrolytes, such as many soluble salts, strong acids, and strong bases, dissociate extensively. Weak electrolytes dissociate only partially. Solid metals conduct through electrons, whereas electrolytes conduct mainly through ions. Resistance is related to resistivity by: R = ρL ÷ A where R is resistance in ohms, ρ is resistivity in Ω m, L is conductor length in metres, and A is cross-sectional area in m². Conductivity κ is the reciprocal of resistivity: κ = 1 ÷ ρ Thus, for a uniform electrolyte cell: G = κA ÷ L where G is conductance in siemens. Conductivity depends on ion concentration, ion charge, mobility, solvent viscosity, and temperature. Increasing concentration does not always increase conductivity indefinitely: at high concentration, ion–ion interactions can reduce mobility. Molar conductivity is: Λm = κ ÷ c where Λm is molar conductivity, κ is conductivity, and c is molar concentration expressed consistently with the chosen unit system. Conductivity measurements are useful in water-quality monitoring, battery electrolyte evaluation, corrosion studies, and process control. Internal resistance and polarizationA real cell can be represented approximately by an ideal electromotive force E connected to an internal resistance r. Under discharge: Vterminal = E − Ir where Vterminal is terminal voltage, I is current, and r is internal resistance. This simple model assumes constant r and neglects nonlinear electrochemical effects. At high current, additional activation and concentration polarization may be important. The power delivered to an external load resistance Rload is: Pload = I²Rload For the simple Thevenin model, maximum power transfer occurs when Rload = r, but efficiency is then only 50%. Practical batteries are normally operated at lower current than this condition to obtain better efficiency, lower heating, and longer life. 4. Electrolysis and Faraday’s LawsElectrolysis uses electrical energy to force a chemical reaction. Applications include metal refining, electroplating, chlor-alkali production, hydrogen production, and battery manufacturing. Faraday’s first law states that the amount of chemical change is proportional to the charge passed. The mass deposited is: m = (MIt) ÷ (nF) where m is deposited mass in grams or kilograms, M is molar mass, I is current, t is time, n is electrons per ion, and F is Faraday’s constant. Units must be chosen consistently. Worked Example 2: Copper depositionA current of 2.00 A passes through Cu²⁺ solution for 30.0 min. For copper, M = 63.546 g mol⁻¹ and n = 2. t = 30.0 × 60 = 1800 s m = (63.546 × 2.00 × 1800) ÷ (2 × 96485) = 1.185 g Approximately 1.19 g of copper is deposited, assuming 100% current efficiency and negligible side reactions. In industrial systems, current efficiency is less than 100% when competing reactions, such as hydrogen evolution, occur. Electrolysis cells require attention to electrode spacing, current density, electrolyte composition, temperature, gas evolution, ventilation, and electrical isolation. Hydrogen and oxygen generated by water electrolysis form an explosive mixture if poorly separated or ventilated. 5. Batteries: Operating Principles and PerformanceA battery is an electrochemical energy-storage device. Its essential components are anode, cathode, electrolyte, separator, current collectors, casing, and often electronic protection. During discharge, the anode is oxidized and the cathode is reduced. During charging of a rechargeable battery, the reactions are driven in the reverse direction, although side reactions prevent perfect reversibility. Important battery specifications include: | Quantity | Meaning |
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| Nominal voltage | Approximate operating voltage under specified conditions | | Capacity | Charge deliverable under specified current, temperature, and cutoff voltage | | Energy | Approximate voltage–charge product, usually in Wh | | Power capability | Maximum useful rate of energy delivery | | C-rate | Current normalized to rated capacity | | Cycle life | Number of cycles before capacity or power reaches a specified limit | | Coulombic efficiency | Discharge charge divided by charge input | | Energy efficiency | Discharge energy divided by charge energy |
Capacity is commonly expressed in ampere-hours: QAh = ∫ I dt ÷ 3600 where I is in amperes and t is in seconds. If current is constant, QAh = It ÷ 3600. Approximate stored energy is: EWh ≈ Vaverage QAh This estimate is valid when average discharge voltage is known; using nominal voltage is only an approximation. The C-rate is: C-rate = I ÷ Qrated where I is current in amperes and Qrated is rated capacity in ampere-hours. A 2 Ah cell discharged at 4 A is operating at 2C. 5.1 Primary batteriesPrimary batteries are designed for one-way use. Alkaline, zinc–carbon, lithium primary, and silver-oxide cells are common examples. They generally offer long shelf life and simple operation, but recharging can cause leakage, rupture, or fire because the chemical reaction is not designed to reverse safely. 5.2 Secondary batteriesSecondary batteries can be recharged. Lead–acid batteries are inexpensive and capable of high surge current but are heavy and contain corrosive electrolyte and toxic lead. Nickel–metal hydride batteries tolerate abuse relatively well but have lower energy density than many lithium-ion systems. Lithium-ion batteries provide high energy and power density but require careful voltage, temperature, and current control. Lithium-ion chemistry is not a single chemistry. Lithium cobalt oxide offers high energy density but has greater thermal-risk concerns. Lithium iron phosphate generally provides improved thermal stability and cycle life, with lower cell voltage and often lower energy density. Nickel–manganese–cobalt and nickel-rich chemistries offer high energy density but require careful thermal and charging management. 5.3 Battery management systemsA battery management system (BMS) measures cell voltage, current, and temperature; estimates state of charge (SoC) and state of health (SoH); balances cells; controls contactors; and disconnects the pack during unsafe conditions. Coulomb counting estimates SoC by integrating current: SoC(t) = SoC(t₀) − (1 ÷ Qusable) ∫ I(τ) dτ with sign conventions defined explicitly. Here Qusable is usable charge capacity. Coulomb counting accumulates sensor and model errors, so it is normally corrected using voltage, current, temperature, and electrochemical or data-driven models. 6. Charging, Degradation and SafetyLithium-ion cells are commonly charged using a constant-current/constant-voltage profile. First, current is held approximately constant until the cell reaches its upper voltage limit. Then voltage is held constant while current decreases to a termination threshold. Charging must remain within manufacturer-specified voltage, current, and temperature limits. Overcharging can cause lithium plating, electrolyte oxidation, gas generation, internal short circuits, and thermal runaway. Excessive discharge may cause copper dissolution from the current collector and permanent damage. Low-temperature charging is particularly hazardous for many lithium-ion chemistries because metallic lithium can plate on the anode. Degradation has several causes: - Calendar ageing: capacity loss while stored, accelerated by high temperature and high state of charge.
- Cycle ageing: damage caused by repeated charge–discharge cycling.
- SEI growth: formation and thickening of the solid-electrolyte interphase, consuming active lithium and increasing resistance.
- Lithium plating: metallic lithium deposition during fast or cold charging.
- Mechanical damage: particle cracking, electrode swelling, separator damage, and loss of electrical contact.
- Thermal abuse: self-heating and possible thermal runaway.
A simplified heat-generation model is: Pheat ≈ I²Rinternal This expression describes irreversible ohmic heating only. A more complete electrochemical heat model also includes reversible entropic heat and polarization losses. Cooling systems must account for peak current, ambient conditions, cell-to-cell variation, and fault conditions. Safety engineering uses containment, fuses, current interruption devices, thermal sensors, pressure relief, spacing, flame-resistant materials, and control software. Standards and regulations vary by application and jurisdiction; designers should consult applicable battery transport, electrical safety, machinery, vehicle, and recycling requirements rather than relying on nominal voltage alone. 7. SupercapacitorsSupercapacitors store energy electrostatically or through fast surface redox reactions. Electric double-layer capacitors use ion adsorption at high-surface-area electrodes. Pseudocapacitors use rapid, reversible faradaic reactions. The stored energy is: E = ½CV² where E is energy in joules, C is capacitance in farads, and V is voltage in volts. Because energy depends on the square of voltage, operating voltage and series-cell balancing are important. For a capacitor discharged through a constant-power load, the available energy between Vmax and Vmin is: Eusable = ½C(Vmax² − Vmin²) Supercapacitors have high power density, rapid charging, very long cycle life, and excellent low-temperature performance. Their disadvantages include low energy density, substantial self-discharge, and a voltage that decreases continuously during discharge. They are useful for regenerative braking, actuator bursts, peak-power support, and smoothing power from intermittent sources. Hybrid systems often combine a battery for energy and a supercapacitor for power transients. 8. Fuel CellsA fuel cell is an electrochemical generator that converts the chemical energy of a continuously supplied fuel and oxidant into electricity, heat, and reaction products. Unlike a battery, it does not store a substantial quantity of reactants internally. For a hydrogen–oxygen proton-exchange membrane fuel cell (PEMFC), the half-reactions are: Anode: H₂ → 2H⁺ + 2e⁻ Cathode: ½O₂ + 2H⁺ + 2e⁻ → H₂O Overall: H₂ + ½O₂ → H₂O The membrane conducts protons but blocks electrons and separates the gases. Electrons travel through the external circuit, while protons cross the membrane. A catalyst accelerates the electrode reactions. The reversible voltage is related to reaction free energy by Erev = −∆G ÷ nF. The actual cell voltage is lower: Vactual = Erev − ηactivation − ηohmic − ηconcentration where the η terms are activation, ohmic, and concentration overpotentials, each measured in volts. Activation losses arise from finite reaction kinetics, ohmic losses from ionic and electronic resistance, and concentration losses from reactant depletion or product accumulation. Fuel-cell systems require fuel processing or purification, air supply, humidification, cooling, water management, power conditioning, leak detection, and control. Hydrogen is not intrinsically more dangerous than all conventional fuels, but its low ignition energy, wide flammability range, and rapid diffusion require appropriate ventilation, sensors, compatible materials, and regulated storage. Other fuel cells include alkaline, phosphoric-acid, molten-carbonate, and solid-oxide types. They differ in electrolyte, operating temperature, fuel flexibility, efficiency, start-up time, and suitable applications. High-temperature cells can use hydrocarbon-derived fuels more readily but impose demanding thermal and materials requirements. 9. Applied Case: Power System for an Autonomous Inspection RobotBackgroundConsider an illustrative inspection robot operating in a factory. It must travel for several hours, accelerate repeatedly, climb short ramps, and survive occasional wireless charging interruptions. The robot requires an average electrical load of 120 W and peak power of 500 W for 10 s during acceleration. ProblemA battery alone sized for the peak power would experience high current pulses, causing voltage sag and heating. A supercapacitor alone would require excessive mass because its energy decreases substantially as voltage falls. AnalysisSuppose a 48 V battery pack has an effective internal resistance of 0.08 Ω. At 500 W, the approximate current is: I = P ÷ V = 500 ÷ 48 = 10.42 A The instantaneous resistive voltage drop is: ∆V = Ir = 10.42 × 0.08 = 0.83 V and heat generation is: Pheat = I²r = 10.42² × 0.08 ≈ 8.7 W A supercapacitor bank can supply the short acceleration pulse, reducing battery current. If C = 100 F and its voltage falls from 48 V to 40 V, its usable energy is: Eusable = ½ × 100 × (48² − 40²) = 35 200 J This equals approximately 9.78 Wh, sufficient in energy terms for a 500 W pulse lasting 10 s, which requires 5 000 J, provided converter and control losses are acceptable. Approach and outcomeThe recommended architecture is a lithium-ion battery for sustained energy, a supercapacitor module connected through a bidirectional DC–DC converter for acceleration and regenerative braking, and a BMS supervising cell limits. The converter controls power sharing: the battery supplies average load while the supercapacitor handles rapid transients. Thermal sensors, current limits, isolation monitoring, and a physically protected enclosure are required. Learning pointsThe case demonstrates that energy and power are separate design requirements. It also shows why nominal voltage is insufficient for design: internal resistance, allowable voltage range, thermal limits, converter efficiency, duty cycle, and ageing must be included. Mechatronics engineers must integrate electrochemistry with sensing, power electronics, mechanical packaging, control software, and safety engineering. 10. Selection, Sustainability and Emerging DevelopmentsTechnology selection should consider required energy, peak power, duty cycle, mass, volume, temperature, recharge time, service life, maintenance, cost, safety, and end-of-life treatment. A high-energy battery is not automatically the best solution if the application demands frequent high-power pulses or rapid charging. Life-cycle assessment should include raw-material extraction, manufacturing energy, transport, use-phase efficiency, repair, second-life use, and recycling. Batteries should not be placed in general waste. Damaged lithium batteries require special handling because residual energy can cause fires. Recycling processes recover valuable metals and reduce environmental burdens, but collection, chemistry identification, safe discharge, and economic recovery remain challenges. Responsible design includes modular packs, accessible diagnostics, replaceable components where feasible, documented chemistry and hazard information, secure software updates, and transparent state-of-health reporting. AI and machine learning can improve SoC and SoH estimation, detect abnormal thermal behavior, and optimize charging. However, data-driven models require representative data, validation across temperature and ageing conditions, explainable fault thresholds, and fail-safe behavior. AI must supplement—not replace—physical protection systems. Contemporary developments include silicon-rich anodes, solid-state electrolytes, sodium-ion batteries, metal–air systems, redox-flow batteries, advanced fuel-cell catalysts, and hybrid battery–supercapacitor architectures. Each involves trade-offs in manufacturing maturity, energy density, cycle life, cost, safety, and resource availability. Engineering decisions should therefore be based on verified performance under the actual operating profile rather than on a single headline specification. Best-Practice Design Checklist- Define energy, power, voltage, duty cycle, environment, and service-life requirements.
- Distinguish reversible voltage from terminal voltage under load.
- Use consistent signs for anode, cathode, current, and state-of-charge calculations.
- Include internal resistance, polarization, temperature, and ageing in sizing.
- Use cell balancing and independent protection for multi-cell packs.
- Prevent overcharge, deep discharge, excessive current, and unsafe temperature operation.
- Validate models experimentally over the complete operating envelope.
- Design for inspection, repair, safe transport, and end-of-life recycling.
- Follow applicable technical standards and regulatory requirements.
- Treat safety as a system property involving chemistry, hardware, software, enclosure, and human procedures.
Chapter SummaryElectrochemical systems convert chemical and electrical energy through coupled oxidation and reduction reactions. Oxidation occurs at the anode and reduction at the cathode, independent of whether the cell is galvanic or electrolytic. Standard cell potential is obtained from the difference between cathode and anode reduction potentials, while the Nernst equation accounts for concentration, pressure, and temperature. Electrolyte conductivity governs internal losses and depends on ion concentration and mobility. Faraday’s law connects charge passed during electrolysis with chemical mass transferred. Battery performance involves voltage, capacity, energy, power, C-rate, efficiency, internal resistance, temperature, and ageing. Primary batteries are generally non-rechargeable; secondary batteries are rechargeable but require controlled charging and protection. Supercapacitors provide high power and long cycle life but relatively little energy. Fuel cells generate electricity continuously from supplied reactants and experience activation, ohmic, and concentration losses. Practical mechatronic systems commonly combine batteries, supercapacitors, converters, sensors, and management software. Safe and sustainable design requires thermal control, fault protection, responsible material use, regulatory compliance, and recycling planning. Key TermsOxidation: Loss of electrons in a redox reaction. Reduction: Gain of electrons in a redox reaction. Anode: Electrode where oxidation occurs. Cathode: Electrode where reduction occurs. Electrolyte: Material containing mobile ions that conducts ionic current. Electrode potential: Potential associated with a half-cell reduction tendency. Standard cell potential: Cell voltage under defined standard conditions. Nernst equation: Relation between reversible potential and reaction quotient. Conductivity: Ability of a material to conduct electric current; reciprocal of resistivity. Electrolysis: Use of electrical energy to drive a chemical reaction. Primary battery: Battery intended for one-way discharge. Secondary battery: Rechargeable electrochemical battery. C-rate: Charge or discharge current normalized to rated capacity. State of charge: Remaining usable charge expressed relative to a reference capacity. State of health: Measure of remaining performance relative to a new or reference condition. Supercapacitor: High-capacitance device designed for rapid energy storage and release. Fuel cell: Generator that converts continuously supplied fuel and oxidant into electricity. Overpotential: Difference between actual and reversible electrode potential associated with losses. Thermal runaway: Self-accelerating temperature rise caused by exothermic internal reactions. Coulombic efficiency: Discharge charge divided by charge supplied. Review QuestionsShort Answer Questions- Define oxidation and reduction, and identify where each occurs in an electrochemical cell.
- Why is a separator used in a practical battery?
- State the Nernst equation and define its variables.
- Distinguish battery energy density from power density.
- Name three major sources of battery degradation.
Long Answer Questions- Explain the operation of a zinc–copper galvanic cell, including electron flow, ion movement, cell notation, and electrode polarity.
- Discuss how internal resistance, polarization, and temperature affect the terminal voltage and efficiency of a battery.
- Compare primary batteries, lithium-ion secondary batteries, lead–acid batteries, and supercapacitors for mechatronic applications.
- Explain the construction and operation of a PEM hydrogen fuel cell and identify its principal voltage losses.
- Describe the safety, environmental, and regulatory considerations involved in designing a rechargeable battery pack.
Analytical / Application Questions- A cell has E°cell = 1.20 V, n = 2, and Q = 100 at 25 °C. Calculate its reversible potential using the Nernst equation and interpret the result.
- Design a preliminary energy-storage architecture for a robot requiring 1 kWh average energy and 1 kW peak power. Justify whether a battery, supercapacitor, or hybrid system is most appropriate.
- A battery-powered actuator shows increasing voltage sag and heating after many cycles. Propose a diagnostic plan using current, voltage, temperature, capacity, and internal-resistance measurements, and explain possible degradation mechanisms.
Multiple Choice Questions with AnswersQuestion 1In a galvanic cell, oxidation occurs at the: A. Cathode B. Anode C. Salt bridge D. External load Correct Answer: B. Anode Question 2For a cell reaction with n = 2, E°cell = 1.10 V, and Q = 0.10 at 25 °C, the reversible cell potential is approximately: A. 0.97 V B. 1.07 V C. 1.13 V D. 1.20 V Correct Answer: C. 1.13 V Question 3Which quantity is the reciprocal of resistivity? A. Resistance B. Conductivity C. Capacitance D. Voltage Correct Answer: B. Conductivity Question 4According to Faraday’s law, deposited mass is directly proportional to: A. Electrode area only B. Cell voltage only C. Charge passed D. Electrolyte volume only Correct Answer: C. Charge passed Question 5A 2 Ah battery discharged at 4 A is operating at: A. 0.5C B. 1C C. 2C D. 8C Correct Answer: C. 2C Question 6The approximate energy stored in a capacitor is: A. CV B. ½CV² C. C²V D. V² ÷ C Correct Answer: B. ½CV² Question 7A major advantage of a supercapacitor compared with a battery is: A. Higher energy density in all applications B. Longer cycle life and higher power capability C. Constant voltage throughout discharge D. Zero self-discharge Correct Answer: B. Longer cycle life and higher power capability Question 8In a PEM hydrogen fuel cell, protons primarily pass through the: A. External metallic circuit B. Separator membrane C. Load resistance D. Current collector only Correct Answer: B. Separator membrane Question 9Which condition is especially hazardous for charging many lithium-ion cells? A. Moderate temperature within specification B. Low-temperature charging C. Use of a current sensor D. Cell balancing Correct Answer: B. Low-temperature charging Question 10For a simple cell model, if E = 12 V, I = 2 A, and internal resistance r = 0.5 Ω, the terminal voltage during discharge is: A. 10 V B. 11 V C. 12.5 V D. 13 V Correct Answer: B. 11 V
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