CBSE âą Class 12 âą Physics
Current Electricity
Current, drift velocity, Ohm's law, resistivity, Kirchhoff rules and Wheatstone bridge.
Chapter 3
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What is Current Electricity?
Current, drift velocity, Ohm's law, resistivity, Kirchhoff rules and Wheatstone bridge.
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 links the microscopic drift of charge carriers to measurable circuit quantities such as current, potential difference, resistance, and power. Circuit behaviour is analysed using Ohmâs law, resistance relations, Kirchhoffâs rules, and Wheatstone-bridge balance, each subject to specified physical conditions.
Reactions, Processes and Experiments
| What happens | Equation or process | What you observe | Type |
|---|---|---|---|
| Charge flows through a conductor at a steady rate. | I = Q/t | A constant amount of charge passes a cross-section per unit time. | Definition of steady current |
| Charge flow varies with time. | I = dQ/dt | The rate of charge flow changes with time. | Definition of time-varying current |
| Free electrons acquire an average drift under an applied electric field. | I = nAevd | Electrons drift opposite to the electric field; the drift velocity is much smaller than their random thermal velocity. | Microscopic model of current |
| Current density is related to carrier density and drift velocity. | J = I/A = nevd | Current is distributed over the conductorâs cross-sectional area. | Current-density relation |
| Current density is related to the applied electric field. | J = ÏE | Greater conductivity gives greater current density for the same electric field. | Macroscopic conduction relation |
| Potential difference is proportional to current for an ohmic conductor at constant temperature and other physical conditions. | V = IR | A graph of V versus I is a straight line through the origin; its slope gives resistance. | Ohmâs law |
| Resistance is determined from potential difference and current. | R = V/I | A larger potential difference is required to produce the same current in a conductor with greater resistance. | Definition of resistance |
| The resistance of a uniform conductor depends on its material, length, and cross-sectional area. | R = ÏL/A | Resistance increases with length and decreases with cross-sectional area. | Resistance relation |
| Resistivity is determined from the resistance and dimensions of a sample. | Ï = RA/L | Resistivity does not depend on the dimensions of the sample, but depends on material and temperature. | Definition of resistivity |
| Conductivity is the reciprocal of resistivity. | Ï = 1/Ï | A material with low resistivity has high conductivity. | Definition of conductivity |
| Mobility relates drift velocity to electric field. | Ό = vd/E | Greater mobility gives greater drift velocity for the same electric field. | Definition of mobility |
| Conductivity is related to charge-carrier density and mobility. | Ï = neÎŒ | Conductivity increases with carrier density or mobility. | Conductivity relation |
| Resistance changes with temperature over a limited range. | R_T = R_0[1 + α(T - T_0)] | For many metals, resistance increases approximately linearly with temperature. | Temperature dependence of resistance |
| Resistivity changes with temperature. | â | Resistivity generally increases with temperature in metals and generally decreases with temperature in many semiconductors. | Temperature dependence of resistivity |
| Resistors are connected end to end. | R_s = R_1 + R_2 + R_3 + ... | The same current flows through every resistor, and voltage divides among them. | Series combination |
| Resistors are connected across the same two points. | 1/R_p = 1/R_1 + 1/R_2 + 1/R_3 + ... | The same potential difference appears across every resistor, and current divides among the branches. | Parallel combination |
| A source supplies energy per unit charge to the complete circuit. | â | The source is characterised by its electromotive force, measured in volts. | Electromotive force |
| A cell supplies current through an external resistance. | I = Δ/(R + r) | Current is reduced by the cellâs internal resistance. | Cell with internal resistance |
| A discharging cell supplies current to an external circuit. | V = Δ - Ir | Terminal potential difference is less than the emf because of the internal potential drop. | Discharging cell |
| A cell is being charged. | V = Δ + Ir | The applied terminal potential difference exceeds the emf. | Charging cell |
| Currents meet at a circuit junction. | ÎŁI = 0 | The total current entering a junction equals the total current leaving it. | Kirchhoffâs junction rule |
| Potential changes are followed around a closed circuit loop. | ÎŁÎV = 0 | The algebraic sum of potential changes around the loop is zero. | Kirchhoffâs loop rule |
| Current directions are assigned when applying Kirchhoffâs rules. | Choose current directions arbitrarily. | A negative calculated current indicates that the actual direction is opposite to the assumed direction. | Circuit-analysis procedure |
| Four resistances are arranged in a bridge circuit to determine an unknown resistance. | â | The unknown resistance is determined by comparison with known resistances. | Wheatstone bridge |
| A Wheatstone bridge is balanced. | P/Q = R/S | No current flows through the galvanometer because the galvanometer junctions are at equal potential. | Balanced Wheatstone bridge |
| A bridge is adjusted for greatest sensitivity. | â | The Wheatstone bridge is most sensitive when the resistances in the two ratio arms are of comparable magnitude. | Wheatstone-bridge condition |
| A uniform one-metre resistance wire is used as a practical Wheatstone bridge. | X/R = l/(100 - l) | At balance, the galvanometer current is zero; l is the balance length in centimetres. | Metre bridge |
| Electrical energy is supplied or consumed over time. | W = VIt | Energy increases with potential difference, current, and time. | Electrical energy |
| Electrical power is calculated from circuit quantities. | P = VI = I^2R = V^2/R | Power is measured in watts. | Electrical power |
| Electrical energy is measured commercially. | 1 kWh = 3.6 Ă 10^6 J | One kilowatt-hour corresponds to 3.6 Ă 10^6 J. | Commercial electrical-energy unit |
Key Terms
- Electric current: The rate of flow of electric charge through a cross-section of a conductor. It is given by
I = dQ/dtand measured in amperes (A). - Conventional current: The assumed direction of current from higher potential to lower potential, opposite to electron drift in a metallic conductor.
- Drift velocity: The average velocity acquired by free electrons because of an applied electric field; for electrons, it is opposite to the electric-field direction.
- Current and drift velocity relation: For a metallic conductor,
I = nAevd, wherenis charge-carrier number density,Ais cross-sectional area,eis electronic charge, andvdis drift velocity. - Current density: Current per unit cross-sectional area, given by
J = I/A = nevd. - Ohmâs law: At constant temperature and other physical conditions, potential difference is directly proportional to current:
V = IR. - Ohmic conductor: A conductor that obeys Ohmâs law under specified constant physical conditions.
- Resistance: The opposition offered by a conductor to current flow, defined by
R = V/I; its SI unit is the ohm (Ω). - Resistivity: The resistance of a material sample of unit length and unit cross-sectional area, given by
Ï = RA/L; its SI unit is ohm metre (Ω m). - Conductivity: The ability of a material to conduct current, given by
Ï = 1/Ï. - Mobility: Drift velocity acquired per unit electric field, given by
ÎŒ = vd/E; conductivity is related to mobility byÏ = neÎŒ. - Temperature dependence of resistance: For many metallic conductors over a limited range, resistance varies approximately as
R_T = R_0[1 + α(T - T_0)]. - Temperature coefficient of resistance: The quantity
αin the temperature relation for resistance. - Series combination of resistors: A connection in which resistors carry the same current;
R_s = R_1 + R_2 + R_3 + .... - Parallel combination of resistors: A connection in which resistors have the same potential difference;
1/R_p = 1/R_1 + 1/R_2 + 1/R_3 + .... - Electromotive force: Energy supplied by a source per unit charge in moving charge through the complete circuit; it is denoted by
Δand measured in volts. - Internal resistance: Resistance within a cell or source that causes a potential drop when current flows.
- Terminal potential difference: The potential difference across a cellâs terminals; for a discharging cell,
V = Δ - Ir, and for a charging cell,V = Δ + Ir. - Kirchhoffâs junction rule: The algebraic sum of currents at a junction is zero, expressing conservation of charge.
- Kirchhoffâs loop rule: The algebraic sum of potential changes around a closed loop is zero, expressing conservation of energy.
- Wheatstone bridge: A four-resistance network used to determine an unknown resistance by comparison with known resistances.
- Balanced Wheatstone bridge: A bridge in which no current flows through the galvanometer; for arms
P,Q,R, andS, balance requiresP/Q = R/S. - Metre bridge: A practical Wheatstone bridge using a uniform one-metre resistance wire; at balance,
X/R = l/(100 - l). - Electrical energy: Energy supplied or consumed in a circuit, given by
W = VIt. - Electrical power: The rate of electrical energy transfer, given by
P = VI = I^2R = V^2/R; its SI unit is the watt. - Kilowatt-hour: A commercial unit of electrical energy equal to
3.6 Ă 10^6 J.
Easily Confused
- Conventional current and electron drift: Conventional current is taken from higher to lower potential, whereas electrons drift in the opposite direction.
- Resistance and resistivity: Resistance depends on a particular conductorâs material, length, cross-sectional area, and temperature; resistivity is an intrinsic material property at a specified temperature.
- Ohmic and non-ohmic conductors: An ohmic conductor gives a straight-line VâI graph through the origin under constant conditions; diodes and filament lamps may be non-ohmic.
- Series and parallel combinations: Series resistors carry the same current and have voltage division; parallel resistors have the same potential difference and current division.
- Emf and terminal potential difference: Emf is the energy supplied per unit charge by the source, whereas terminal voltage is affected by internal resistance and current.
- Kirchhoffâs junction and loop rules: The junction rule expresses conservation of charge; the loop rule expresses conservation of energy.
- Wheatstone bridge and metre bridge: A metre bridge is a practical Wheatstone bridge using a uniform one-metre resistance wire.
- Resistance and conductance: Resistance opposes current and is measured in ohms; conductivity describes a materialâs ability to conduct and is the reciprocal of resistivity.
What Gets Asked
- Define electric current and use
I = Q/torI = dQ/dt; marks are lost by confusing steady-current and time-varying-current expressions. - Explain metallic conduction using drift velocity and apply
I = nAevdorJ = I/A = nevd; marks are lost by treating electron drift as occurring in the conventional-current direction. - Apply Ohmâs law, identify an ohmic conductor from a straight-line VâI graph through the origin, and interpret the slope as resistance; marks are lost by treating Ohmâs law as universal for devices such as diodes and filament lamps.
- Calculate resistance, resistivity, conductivity, mobility, or temperature-dependent resistance using
R = ÏL/A,Ï = RA/L,Ï = 1/Ï,ÎŒ = vd/E,Ï = neÎŒ, andR_T = R_0[1 + α(T - T_0)]; marks are lost by treating resistance and resistivity as interchangeable. - Determine currents, terminal voltage, and power in series, parallel, or source circuits; marks are lost by omitting internal resistance or using
V = Δ - Irfor a charging cell, whereV = Δ + Irapplies. - Apply Kirchhoffâs rules or calculate an unknown resistance using a balanced Wheatstone bridge or metre bridge; marks are lost by using the wrong conservation principle, omitting the zero galvanometer current at balance, or misusing
X/R = l/(100 - l).
Flashcards
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- Explain the core principle behind Current Electricity in clear scientific language.
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- Interpret diagrams, graphs, or experiments linked to the topic.
- Connect conceptual understanding with the final answer instead of memorising formulas alone.
Common exam prompts
- State the law, principle, or definition behind Current Electricity precisely.
- Apply the relevant equation to a short numerical problem with correct units.
- Explain a diagram, graph, or experiment related to Current Electricity.
- Distinguish between conceptual understanding and memorised formula use in this chapter.
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Quick answers students usually need
What is Current Electricity in CBSE Class 12 Physics?
Current, drift velocity, Ohm's law, resistivity, Kirchhoff rules and Wheatstone bridge.
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