ISC • Class 12 • Physics
Current Electricity
Current flow, resistance, circuits, and potentiometer.
Chapter 2
Verified Curriculum Topic
What is Current Electricity?
Current flow, resistance, circuits, and potentiometer.
Current Electricity matters because it connects theory, equations, and real physical behaviour. At Class 12 level, students are typically expected to explain concepts precisely, apply laws correctly, and interpret numerical or experimental questions with confidence.
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Summary
The One Thing
Current electricity concerns the ordered motion of charge caused by a potential difference. Circuit behaviour is determined by the relationship between potential difference, resistance, current, and the characteristics of real cells, including their internal resistance.
Reactions, Processes and Experiments
| What happens | Equation or process | What you observe | Type |
|---|---|---|---|
| Charge exists in discrete amounts. | q = ne, where n is an integer and e = 1.6 x 10^-19 C. | — | Quantization of charge |
| Electric current is the rate of flow of charge through a cross-section. | I = Q/t; for changing current, I = dQ/dt. | — | Definition and relation |
| Charge carriers drift through a conductor under an applied electric field. | I = neAv_d, where n is carrier concentration, e is charge, A is area, and v_d is drift velocity. | Electron drift is opposite to the direction of conventional current. | Microscopic current relation |
| Current flows per unit cross-sectional area. | J = I/A; in microscopic form, J = ne v_d. | — | Current density |
| A potential difference is associated with work done per unit charge. | V = W/Q. | — | Potential difference |
| For a conductor at constant temperature and physical conditions, current is directly proportional to potential difference. | V = IR. | A graph of potential difference against current is linear for an ohmic conductor under constant conditions. | Ohm’s law |
| Resistance depends on the material and dimensions of a conductor. | R = rho l/A. | Resistance increases with length and decreases with cross-sectional area. | Resistance relation |
| Resistivity characterises the material of a conductor. | rho = RA/l. | — | Resistivity |
| Conductivity is the reciprocal of resistivity. | sigma = 1/rho. | — | Conductivity |
| Resistance changes with temperature for many metals over a limited range. | R_T = R_0[1 + alpha(T - T_0)]. | Resistance generally increases with temperature for metals. | Temperature dependence of resistance |
| Several resistors are connected in series. | R_s = R_1 + R_2 + R_3 + ... . | The same current flows through each resistor. | Series combination |
| Several resistors are connected in parallel. | 1/R_p = 1/R_1 + 1/R_2 + 1/R_3 + ... . | The same potential difference acts across each branch. | Parallel combination |
| Two resistors are connected in parallel. | R_p = R_1R_2/(R_1 + R_2). | — | Parallel combination |
| A cell supplies current through an external resistance while possessing internal resistance. | I = E/(R + r). | The current is less than it would be for an ideal cell with the same emf and external resistance. | Cell circuit |
| A discharging cell delivers energy to an external circuit. | V = E - Ir. | A real battery’s terminal voltage decreases under load because of the potential drop across its internal resistance. | Terminal potential difference |
| A cell is being charged. | V = E + Ir. | The applied terminal voltage exceeds the emf by the internal potential drop. | Charging cell |
| Cells are connected in series in the aiding direction. | E_eq = E_1 + E_2 + ... and r_eq = r_1 + r_2 + ... . | The emfs and internal resistances add. | Cells in series |
| Identical cells are connected in series. | E_eq = nE and r_eq = nr. | — | Cells in series |
| Identical cells are connected in parallel. | E_eq = E and r_eq = r/n. | The emf remains that of one cell, while the equivalent internal resistance is reduced. | Cells in parallel |
| Electrical power is consumed or supplied in a circuit. | P = VI = I^2R = V^2/R. | — | Electrical power |
| A cell supplies power to a circuit. | P = EI; useful external power is P_external = VI = I^2R. | The supplied power is divided between useful external power and internal dissipation. | Power supplied by a cell |
| Maximum power is transferred to the external resistance. | R = r; P_max = E^2/(4r). | Maximum external power occurs when external resistance equals internal resistance. | Maximum power transfer |
| Currents meet at a circuit junction. | The algebraic sum of currents at a junction is zero; total current entering a junction equals total current leaving it. | Current entering equals current leaving. | Kirchhoff’s junction rule |
| Potential changes are considered around a closed circuit loop. | The algebraic sum of potential changes around any closed loop is zero. | The total potential rise equals the total potential drop around the loop. | Kirchhoff’s loop rule |
| Electrical energy is used over a time interval. | W = VIt = I^2Rt. | — | Electrical energy |
| A Wheatstone bridge is adjusted to balance. | P/Q = R/S, with no current through the central galvanometer. | The galvanometer shows no deflection. | Wheatstone bridge |
| A meter bridge, a practical form of the Wheatstone bridge, is balanced using a uniform wire. | X/R = l/(100 - l), for unknown X in the left gap and known R in the right gap. | The galvanometer shows zero deflection at the balance point. | Meter bridge |
| A potentiometer measures potential difference by comparison with the potential drop along a uniform wire. | A uniform resistance wire is connected across a potential difference, and a null point is located using a galvanometer. | At the null point, the galvanometer shows zero deflection. | Potentiometer |
| The potential drop along a potentiometer wire is related to its length. | k = V/L. | A longer potentiometer wire gives a smaller potential gradient and therefore greater sensitivity. | Potential gradient |
| Two emfs are compared using balancing lengths on a potentiometer. | E_1/E_2 = l_1/l_2. | Each emf is associated with a balancing length at which the galvanometer shows zero deflection. | Comparison of emfs |
| The internal resistance of a cell is determined using a potentiometer. | r = R(l_1 - l_2)/l_2. | The balance length decreases when external resistance R is connected across the cell. | Measurement of internal resistance |
| A potentiometer compares an emf under a zero-current condition. | At balance, it draws no current from the source being measured. | Zero galvanometer deflection gives a null measurement. | Null-deflection method |
Key Terms
- Electric current: The rate of flow of electric charge through a cross-section, given by I = Q/t; its SI unit is the ampere.
- Conventional current: The direction in which positive charge would move, from higher potential to lower potential in an external circuit.
- Drift velocity: The small average velocity acquired by free electrons in a conductor because of an applied electric field.
- Current density: Current flowing per unit area perpendicular to the flow, given by J = I/A.
- Potential difference: The work done per unit charge in moving a test charge between two points, V = W/Q.
- Ohm’s law: For a conductor at constant temperature and physical conditions, current is directly proportional to potential difference: V = IR.
- Resistance: The opposition offered by a conductor to the flow of current; R = V/I and its SI unit is the ohm.
- Resistivity: A material property defined by rho = RA/l, where R is resistance, A is cross-sectional area, and l is length.
- Conductivity: The reciprocal of resistivity, sigma = 1/rho, indicating how easily a material conducts electricity.
- Temperature dependence of resistance: For many metals over a limited range, R_T = R_0[1 + alpha(T - T_0)], where alpha is the temperature coefficient of resistance.
- EMF: The energy supplied by a source per unit charge when no current is drawn; it is denoted by E and measured in volts.
- Internal resistance: The resistance inside a cell or battery that causes energy loss when current flows; it is denoted by r.
- Terminal potential difference: The voltage available across the terminals of a cell while supplying current; for a discharging cell, V = E - Ir.
- Kirchhoff’s junction rule: The algebraic sum of currents at a junction is zero; total current entering a junction equals total current leaving it.
- Kirchhoff’s loop rule: The algebraic sum of potential changes around any closed loop is zero, expressing conservation of energy.
- Resistors in series: The same current flows through each resistor and the equivalent resistance is R_s = R_1 + R_2 + ... .
- Resistors in parallel: The same potential difference acts across each branch and 1/R_p = 1/R_1 + 1/R_2 + ... .
- Electrical power: The rate of electrical energy consumption, P = VI = I^2R = V^2/R.
- Electrical energy: Energy used in time t, W = VIt = I^2Rt; the commercial unit is the kilowatt-hour.
- Wheatstone bridge: A bridge circuit used to measure an unknown resistance; at balance, P/Q = R/S and no current flows through the galvanometer.
- Meter bridge: A practical form of the Wheatstone bridge using a uniform wire; at balance, X/R = l/(100 - l), subject to the chosen arm arrangement.
- Potentiometer: An instrument that measures potential difference by comparing it with the potential drop along a uniform resistance wire.
- Potential gradient: Potential drop per unit length of potentiometer wire, k = V/L.
- Null point: The position on a potentiometer wire where the galvanometer shows zero deflection, indicating no current through it.
Easily Confused
- EMF and terminal potential difference: EMF is the energy supplied per unit charge when no current is drawn, whereas terminal potential difference is the voltage available while the cell supplies current; for a discharging cell, V = E - Ir.
- Electron drift and conventional current: Electrons drift opposite to conventional current, which is defined as the direction of positive charge motion.
- Resistance and resistivity: Resistance depends on a conductor’s material and dimensions, whereas resistivity is a material property defined by rho = RA/l.
- Series and parallel resistors: In series, the same current flows through every resistor; in parallel, the same potential difference acts across every branch.
- Kirchhoff’s junction rule and loop rule: The junction rule follows conservation of charge, whereas the loop rule follows conservation of energy.
- Wheatstone bridge and meter bridge: The meter bridge is a practical Wheatstone bridge using a uniform wire and a balance length.
- Potentiometer and voltmeter: A potentiometer uses a null point and draws no current from the source being measured at balance, making it more accurate for comparing emfs.
- Power supplied by a cell and useful external power: P = EI is the power supplied by the cell, whereas P_external = VI = I^2R is the useful power delivered to the external resistance.
- Potential gradient and sensitivity: A smaller potential gradient gives a greater potentiometer sensitivity; therefore, a longer wire generally increases sensitivity.
What Gets Asked
- Define electric current, potential difference, resistance, resistivity, conductivity, emf, internal resistance, and terminal potential difference, including their equations and SI units. A common mark-losing error is confusing emf with terminal potential difference under load.
- Derive or apply microscopic current relations, especially I = neAv_d and J = ne v_d. The direction of electron drift must not be identified with the direction of conventional current.
- Calculate equivalent resistance for series and parallel combinations, including R_p = R_1R_2/(R_1 + R_2) for two parallel resistors. The key distinction is same current in series and same potential difference in parallel.
- Solve cell and circuit problems using I = E/(R + r), V = E - Ir, V = E + Ir, and the maximum-power condition R = r. Marks are lost when internal resistance is omitted or when charging and discharging equations are interchanged.
- Apply Kirchhoff’s junction and loop rules to complex circuits. The junction rule expresses conservation of charge, while the loop rule expresses conservation of energy.
- Determine unknown resistance or emf using Wheatstone bridges, meter bridges, and potentiometers. The balance condition must be matched to the stated arm arrangement, and the null point must be interpreted as zero galvanometer deflection.
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What is Current Electricity in ISC Class 12 Physics?
Current flow, resistance, circuits, and potentiometer.
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