Comprehensive Study Notes on Current Electricity, Circuit Analysis, and Electrical Energy

Electrical Energy and Cost Calculation

  • Definition of Kilowatt-Hour (kWh\text{kWh}):

    • A kilowatt-hour (kWh\text{kWh}) represents 1000 W1000\,\text{W} of electrical power consumed or generated continuously over a duration of one hour (1 h1\,\text{h}).

    • It serves as a standard unit of measurement for total electrical energy consumed and total work performed.

    • The kilowatt-hour (kWh\text{kWh}) is the commercial billing unit utilized by electrical utility providers to charge consumers.

  • Step-by-Step Energy and Cost Calculation Procedure:

    • Step 1: Calculate Electrical Power (PP):

    • Multiply electrical potential difference (VV) by current (II):       P=V×IP = V \times I

    • In this relationship, potential difference is measured in volts (V\text{V}), current in amperes (A\text{A}), and resulting power in watts (W\text{W}).

    • Step 2: Convert Power to Kilowatts (kW\text{kW}):

    • Divide power in watts (W\text{W}) by the metric conversion factor of 1000 W/kW1000\,\text{W/kW}:       Power in kW=Power in W1000 W/kW\text{Power in kW} = \frac{\text{Power in W}}{1000\,\text{W/kW}}

    • Step 3: Calculate Consumed Electrical Energy (kWh\text{kWh}):

    • Multiply power in kilowatts (kW\text{kW}) by the total elapsed operational time in hours (h\text{h}):       Energy (kWh)=Power (kW)×Time (h)\text{Energy (kWh)} = \text{Power (kW)} \times \text{Time (h)}

    • Step 4: Compute Monetary Cost:

    • Multiply total energy consumed in kilowatt-hours by the specific energy tariff rate per kilowatt-hour:       Cost=Energy (kWh)×Unit Price per kWh\text{Cost} = \text{Energy (kWh)} \times \text{Unit Price per kWh}

  • Worked Example — Slow Cooker Consumption:

    • Problem: A slow cooker operates on an electric current of 4 A4\,\text{A} drawn from a 110 V110\,\text{V} circuit for a duration of 2 h2\,\text{h}. Calculate the total electrical energy consumed in kilowatt-hours (kWh\text{kWh}).

    • Step 1 — Determine Power:
          P=110 V×4 A=440 WP = 110\,\text{V} \times 4\,\text{A} = 440\,\text{W}

    • Step 2 — Convert Watts to Kilowatts:
          440 W1000 W/kW=0.44 kW\frac{440\,\text{W}}{1000\,\text{W/kW}} = 0.44\,\text{kW}

    • Step 3 — Multiply by Operational Hours:
          0.44 kW×2 h=0.88 kWh0.44\,\text{kW} \times 2\,\text{h} = 0.88\,\text{kWh}

  • Practical Energy and Operational Cost Problems:

    • Problem 1 (Electric Stove Energy): An electric stove draws 20 A20\,\text{A} of current on a 220 V220\,\text{V} circuit for 1 h1\,\text{h}.

    • Power: P=220 V×20 A=4400 W=4.4 kWP = 220\,\text{V} \times 20\,\text{A} = 4400\,\text{W} = 4.4\,\text{kW}

    • Energy consumed: 4.4 kW×1 h=4.4 kWh4.4\,\text{kW} \times 1\,\text{h} = 4.4\,\text{kWh}

    • Problem 2 (Electric Stove Operating Cost): Total cost to run the electric stove in Problem 1 at an energy tariff of R0.08\text{R}0.08 per kWh\text{kWh}:

    • Cost=4.4 kWh×R0.08/kWh=R0.352\text{Cost} = 4.4\,\text{kWh} \times \text{R}0.08/\text{kWh} = \text{R}0.352 (or 35.2 cents35.2\,\text{cents})

    • Problem 3 (Microwave Oven Energy): A microwave oven draws 6 A6\,\text{A} of current on a 110 V110\,\text{V} circuit for 2 h2\,\text{h}.

    • Power: P=110 V×6 A=660 W=0.66 kWP = 110\,\text{V} \times 6\,\text{A} = 660\,\text{W} = 0.66\,\text{kW}

    • Energy consumed: 0.66 kW×2 h=1.32 kWh0.66\,\text{kW} \times 2\,\text{h} = 1.32\,\text{kWh}

    • Problem 4 (Microwave Oven Operating Cost): Total cost to operate the microwave oven in Problem 3 at an energy rate of R0.08\text{R}0.08 per kWh\text{kWh}:

    • Cost=1.32 kWh×R0.08/kWh=R0.1056\text{Cost} = 1.32\,\text{kWh} \times \text{R}0.08/\text{kWh} = \text{R}0.1056 (or 10.56 cents10.56\,\text{cents})

    • Problem 5 (Refrigerator Daily Consumption): A refrigerator operates at 10 A10\,\text{A} on a 220 V220\,\text{V} circuit for an average run time of 18 h18\,\text{h} per day.

    • Power: P=220 V×10 A=2200 W=2.2 kWP = 220\,\text{V} \times 10\,\text{A} = 2200\,\text{W} = 2.2\,\text{kW}

    • Daily energy consumed: 2.2 kW×18 h=39.6 kWh2.2\,\text{kW} \times 18\,\text{h} = 39.6\,\text{kWh}

    • Problem 6 (Refrigerator Daily Running Cost): Daily operational cost of running the refrigerator in Problem 5 at an electricity rate of 14 cents14\,\text{cents} per kWh\text{kWh}:

    • Cost=39.6 kWh×14 cents/kWh=554.4 cents=R5.544\text{Cost} = 39.6\,\text{kWh} \times 14\,\text{cents/kWh} = 554.4\,\text{cents} = \text{R}5.544

    • Problem 7 (Household Monthly Electricity Bill): A residential electricity meter displays a reading of 73602 kWh73602\,\text{kWh} on June 1 and 76167 kWh76167\,\text{kWh} on July 1. The unit cost of electricity is 15 cents15\,\text{cents} per kWh\text{kWh}.

    • Total monthly energy consumption:
            76167 kWh−73602 kWh=2565 kWh76167\,\text{kWh} - 73602\,\text{kWh} = 2565\,\text{kWh}

    • Total electricity bill for June:
            2565 kWh×15 cents/kWh=38475 cents=$384.752565\,\text{kWh} \times 15\,\text{cents/kWh} = 38475\,\text{cents} = \$384.75 (or R384.75\text{R}384.75)

    • Problem 8 (Lighting Efficiency and Cost Savings): An office space is illuminated by three 100 W100\,\text{W} incandescent bulbs for 8 h8\,\text{h} per day. The fixtures are retrofitted with 60 W60\,\text{W} bulbs. Electricity costs 12 cents12\,\text{cents} per kWh\text{kWh}.

    • Initial total power: 3×100 W=300 W=0.3 kW3 \times 100\,\text{W} = 300\,\text{W} = 0.3\,\text{kW}

    • Retrofitted total power: 3×60 W=180 W=0.18 kW3 \times 60\,\text{W} = 180\,\text{W} = 0.18\,\text{kW}

    • Power saved:
            0.3 kW−0.18 kW=0.12 kW0.3\,\text{kW} - 0.18\,\text{kW} = 0.12\,\text{kW}

    • Daily electrical energy saved:
            0.12 kW×8 h=0.96 kWh0.12\,\text{kW} \times 8\,\text{h} = 0.96\,\text{kWh}

    • Monetary savings achieved per day:
            0.96 kWh×12 cents/kWh=11.52 cents0.96\,\text{kWh} \times 12\,\text{cents/kWh} = 11.52\,\text{cents}

Electric Current and Charge

  • Definition of Electric Current:

    • An electric current is defined fundamentally as a flow of charge.

  • Conventional Current vs. Electron Flow:

    • In a conducting circuit, negatively charged electrons physically move away from the negative terminal and toward the positive terminal of a power source.

    • Conventional current (II) is defined as the flow of positive charge from the positive terminal to the negative terminal (represented conceptually as empty positive "spaces" migrating toward the negative terminal).


Electron movement toward the positive terminal and positive space movement toward the negative terminal in a conductor
  • Mathematical Formulation of Current:

    • Conventional current equals the rate of flow of charge past a given cross-sectional boundary:     I=QtI = \frac{Q}{t}

    • Variable definitions:

    • II = conventional current, measured in amperes (A\text{A})

    • QQ = quantity of charge flowing, measured in coulombs (C\text{C})

    • tt = elapsed time, measured in seconds (s\text{s})

  • Unit Definition of the Ampere:

    • One ampere (1 A1\,\text{A}) is the constant current flowing when one coulomb (1 C1\,\text{C}) of charge passes a specific point in an electrical conductor in one second (1 s1\,\text{s}):     1 A=1 C/s1\,\text{A} = 1\,\text{C/s}

  • Unit Definition of the Coulomb:

    • One coulomb (1 C1\,\text{C}) is the quantity of electric charge transported past a point when a steady current of one ampere (1 A1\,\text{A}) flows for a duration of one second (1 s1\,\text{s}):     Q=I×tQ = I \times t     1 C=1 A×1 s1\,\text{C} = 1\,\text{A} \times 1\,\text{s}

Potential Difference (Voltage) and Resistance

  • Potential Difference (Voltage — VV):

    • Potential difference is the work done or energy expended by electrical cells to move charge between two points in an electrical circuit:     V=WQV = \frac{W}{Q}

    • Variable definitions:

    • VV = potential difference, measured in volts (V\text{V})

    • WW = electrical work or energy transferred, measured in joules (J\text{J})

    • QQ = quantity of electrical charge moved, measured in coulombs (C\text{C})

    • One volt (1 V1\,\text{V}) represents the transfer of one joule (1 J1\,\text{J}) of energy per one coulomb (1 C1\,\text{C}) of charge displaced:     1 V=1 J/C1\,\text{V} = 1\,\text{J/C}

  • Electrical Resistance (RR):

    • Resistance is a quantitative measure of the opposition experienced by moving charge carriers passing through a circuit component.

    • Microscopic cause: Electrical resistance arises directly due to collisions between mobile conduction electrons and the vibrating, stationary positive metal ions forming the crystalline lattice of the conductor.

  • Ohm's Law:

    • The resistance of a conductor, maintained at a constant temperature, is measured by the ratio of the potential difference across it to the current flowing through it (the "push-to-flow" ratio):     R=VIR = \frac{V}{I}

    • Variable definitions:

    • RR = resistance, measured in ohms (Ω\Omega)

    • VV = potential difference, measured in volts (V\text{V})

    • II = current, measured in amperes (A\text{A})

    • Definition of the Ohm: One ohm (1 Ω1\,\Omega) is the resistance of an electrical conductor when a potential difference of one volt (1 V1\,\text{V}) applied across its terminals produces a current of one ampere (1 A1\,\text{A}).

  • Physical Determinants of Electrical Resistance:

    • Conductor resistance depends fundamentally upon four physical parameters:

    • Temperature: For metallic conductors, resistance increases as temperature rises due to increased thermal lattice vibrations, leading to more frequent electron-ion collisions.

    • Length: Resistance is directly proportional to conductor length (R∝LR \propto L).

    • Thickness (Cross-Sectional Area): Resistance is inversely proportional to conductor thickness or cross-sectional area (R∝1AR \propto \frac{1}{A}).

    • Type of Metal: Inherent resistivity varies across different materials based on atomic structure and free electron density.

Circuit Symbols and Measuring Instruments

  • Standard Circuit Symbols:

    • Standard graphical representations are utilized for electrical schematic drafting:

    • Cell: Pair of parallel unequal lines (long thin positive line, short thick negative line).

    • Alternating Source: Circle enclosing a sinusoidal wave symbol.

    • Filament Bulb: Circle enclosing an "X".

    • Switch: Two terminal circles connected by a hinged lever (open or closed).

    • Fuse: Rectangular box with an axial connecting wire traversing through its center.

    • Resistor: Hollow elongated rectangle.

    • Variable Resistor (Rheostat): Hollow rectangle crossed diagonally by an arrow indicating adjustability.

    • Voltmeter: Circle enclosing the uppercase letter "V".

    • Ammeter: Circle enclosing the uppercase letter "A".


Standard circuit diagram schematic symbols for electrical components
  • Measurement Instruments (Meters):

    • Ammeters:

    • Function: Measure electric current strength flowing through a circuit.

    • Connection: Always connected strictly in series within the path of interest.

    • Internal Resistance: Designed with almost zero internal resistance (R≈0 ΩR \approx 0\,\Omega) so that insertion of the meter does not appreciably alter or restrict the current flowing through the circuit.

    • Voltmeters:

    • Function: Measure electrical potential difference between two separate points.

    • Connection: Always connected strictly in parallel across the component being measured.

    • Internal Resistance: Designed with extremely high internal resistance (R→∞R \to \infty) so that the meter draws virtually no current from the main circuit.

Resistors in Series and Parallel Networks

  • Resistors Connected in Series:

    • Configuration: Components connected end-to-end along a single continuous conducting loop.

    • Path: There is only one path available for current flow.

    • Current Behavior: Current remains constant throughout all series components:     ITOT=I1=I2=I3=…I_{\text{TOT}} = I_1 = I_2 = I_3 = \dots

    • Potential Difference Distribution: Total source potential difference splits across the individual resistors in direct proportion to their resistances:     VTOT=V1+V2+V3+…V_{\text{TOT}} = V_1 + V_2 + V_3 + \dots

    • Total Equivalent Resistance: Total resistance equals the direct algebraic sum of the individual resistances:     RTOT=R1+R2+R3+…R_{\text{TOT}} = R_1 + R_2 + R_3 + \dots

    • Circuit Reliability: If any single series component fails or burns out, the circuit is broken completely and all current flow ceases instantly.


Schematic circuit diagram of three resistors connected in series with a DC voltage source
  • Worked Example — Resistors in Series:

    • Scenario: A 12 V12\,\text{V} battery is connected across three series resistors with values of 1 Ω1\,\Omega, 2 Ω2\,\Omega, and 3 Ω3\,\Omega.

    • (a) Total Resistance:
          RTOT=R1+R2+R3=1 Ω+2 Ω+3 Ω=6 ΩR_{\text{TOT}} = R_1 + R_2 + R_3 = 1\,\Omega + 2\,\Omega + 3\,\Omega = 6\,\Omega

    • (b) Circuit Current:
          I=VRTOT=12 V6 Ω=2 AI = \frac{V}{R_{\text{TOT}}} = \frac{12\,\text{V}}{6\,\Omega} = 2\,\text{A}

    • (c) Potential Difference Across Each Resistor:
          V1Ω=I×R1=2 A×1 Ω=2 VV_{1\Omega} = I \times R_1 = 2\,\text{A} \times 1\,\Omega = 2\,\text{V}     V2Ω=I×R2=2 A×2 Ω=4 VV_{2\Omega} = I \times R_2 = 2\,\text{A} \times 2\,\Omega = 4\,\text{V}     V3Ω=I×R3=2 A×3 Ω=6 VV_{3\Omega} = I \times R_3 = 2\,\text{A} \times 3\,\Omega = 6\,\text{V}

    • Verification: VTOT=2 V+4 V+6 V=12 VV_{\text{TOT}} = 2\,\text{V} + 4\,\text{V} + 6\,\text{V} = 12\,\text{V}

  • Resistors Connected in Parallel:

    • Configuration: Multiple components connected across common electrical junctions.

    • Path: There is more than one path available for current flow.

    • Potential Difference Behavior: Potential difference across all parallel branches is identical and constant:     Vparallel=V1=V2=V3=…V_{\text{parallel}} = V_1 = V_2 = V_3 = \dots

    • Total Equivalent Resistance (ReqR_{\text{eq}}): The reciprocal of equivalent resistance equals the sum of reciprocals of individual resistances:     1Req=1R1+1R2+1R3+…\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + \dots

    • Resistance Property: The equivalent resistance of a parallel combination is always strictly less than the smallest individual resistor in the combination because parallel branches create additional pathways for charge flow.

    • Current Division: Total main circuit current splits into each parallel branch inversely proportional to branch resistance:     Ibranch=VparallelRbranchI_{\text{branch}} = \frac{V_{\text{parallel}}}{R_{\text{branch}}} or Ibranch=Imain×ReqRbranchI_{\text{branch}} = \frac{I_{\text{main}} \times R_{\text{eq}}}{R_{\text{branch}}}     Imain=I1+I2+I3+…I_{\text{main}} = I_1 + I_2 + I_3 + \dots

    • Circuit Reliability: If one branch component fails or blows, the circuit loop remains intact through all alternate parallel branches, permitting current to continue flowing uninterrupted (e.g., standard domestic household circuits).


Schematic circuit diagram of three resistors connected in parallel across a DC power source
  • Worked Example — Resistors in Parallel:

    • Scenario: A 12 V12\,\text{V} battery is connected across three parallel resistors with ratings of 10 Ω10\,\Omega, 15 Ω15\,\Omega, and 30 Ω30\,\Omega.

    • (a) Equivalent Resistance (ReqR_{\text{eq}}):
          1Req=110+115+130=3+2+130=630\frac{1}{R_{\text{eq}}} = \frac{1}{10} + \frac{1}{15} + \frac{1}{30} = \frac{3 + 2 + 1}{30} = \frac{6}{30}     Req=306=5 ΩR_{\text{eq}} = \frac{30}{6} = 5\,\Omega

    • (b) Total Ammeter Reading (ImainI_{\text{main}}):
          I=VReq=12 V5 Ω=2.4 AI = \frac{V}{R_{\text{eq}}} = \frac{12\,\text{V}}{5\,\Omega} = 2.4\,\text{A}

    • (c) Current Through the 10 Ω10\,\Omega Resistor:
          I10Ω=VparallelR10Ω=12 V10 Ω=1.2 AI_{10\Omega} = \frac{V_{\text{parallel}}}{R_{10\Omega}} = \frac{12\,\text{V}}{10\,\Omega} = 1.2\,\text{A}

    • Branch current check:
            I15Ω=12 V15 Ω=0.8 AI_{15\Omega} = \frac{12\,\text{V}}{15\,\Omega} = 0.8\,\text{A}       I30Ω=12 V30 Ω=0.4 AI_{30\Omega} = \frac{12\,\text{V}}{30\,\Omega} = 0.4\,\text{A}       ITOT=1.2 A+0.8 A+0.4 A=2.4 AI_{\text{TOT}} = 1.2\,\text{A} + 0.8\,\text{A} + 0.4\,\text{A} = 2.4\,\text{A}

  • Combinations of Electrochemical Cells:

    • Cells in Series: Total potential difference equals the sum of potential differences of the individual cells:     VTOT=V1+V2+…V_{\text{TOT}} = V_1 + V_2 + \dots

    • Example: A 2 V2\,\text{V} cell connected in series with a 1 V1\,\text{V} cell provides:       VTOT=2 V+1 V=3 VV_{\text{TOT}} = 2\,\text{V} + 1\,\text{V} = 3\,\text{V}

    • Cells in Parallel: Total potential difference equals the potential difference of the largest cell in the parallel bank:     VTOT=VlargestV_{\text{TOT}} = V_{\text{largest}}

    • Example: A 2 V2\,\text{V} cell connected in parallel with a 1 V1\,\text{V} cell provides:       VTOT=2 VV_{\text{TOT}} = 2\,\text{V}

Direct Current (D.C.) and Alternating Current (A.C.)

  • Direct Current (D.C.):

    • Definition: Electric current in which electrons drift unidirectionally through a conductor, moving from negative to positive.

    • Typical sources: Electrochemical cells, chemical batteries, and direct current power supplies.

    • Waveform: A continuous horizontal line above zero on both voltage-time (VV-tt) and current-time (II-tt) oscilloscope traces.


Oscilloscope voltage-time trace depicting constant unsmoothed direct current
  • Alternating Current (A.C.):

    • Definition: Electric current in which moving charge carriers regularly reverse their direction of flow at fixed temporal intervals.

    • Utility Grid Standards: In South Africa, the national grid frequency supplied by ESKOM operates at 50 Hz50\,\text{Hz} (50 cycles/second50\,\text{cycles/second}).

    • Biological Perception Limit: The human eye can discern a maximum of 44 oscillations/second44\,\text{oscillations/second}; consequently, visual lighting running at 50 Hz50\,\text{Hz} appears perfectly continuous without perceptible flicker.

    • Waveform: A sinusoidal trace displaying periodic oscillation above and below the zero-axis on voltage-time (VV-tt) and current-time (II-tt) traces.


Oscilloscope voltage-time trace depicting a sinusoidal alternating current waveform

Domestic Electrical Installations and Household Circuits

  • Utility Supply Characteristics:

    • The electrical utility (ESKOM) supplies residential properties with a nominal 220 V220\,\text{V} alternating current.

    • Supply enters the home through an external service cable comprising two primary conductors passing through the utility meter to the main distribution box:

    • Live Wire (L): High-potential conductor operating at an alternating potential of 220 V220\,\text{V}.

    • Neutral Wire (N): Return conductor maintained at ground potential (0 V0\,\text{V}).

    • Earth Wire (E): Low-resistance safety conductor connected directly to a buried earth ground electrode.

  • Internal Distribution Box Architecture:

    • Incoming power passes through a paired main switch capable of isolating both Live and Neutral simultaneously.

    • Sub-circuits originate from shared busbars in the distribution box, each governed by dedicated circuit breakers or trip switches tailored to expected load capacities:

    • Stove Circuit: Heavy-duty dedicated branch protected by a 60 A60\,\text{A} breaker.

    • Wall Socket Plugs (Main Circuit): Power circuits protected by a 30 A30\,\text{A} breaker feeding three-pin wall sockets with connected earth conductors.

    • Lighting Circuit: Protected by a 15 A15\,\text{A} breaker supplying ceiling illumination fittings.

    • Main Circuit Breaker: Overall system safety protected by a master 60 A60\,\text{A} trip switch to prevent wiring from overheating and causing structural fires.

  • Safety and Structural Wiring Rules:

    • Parallel Arrangement: All wall plugs, sockets, and lighting fixtures are wired in parallel across the Live and Neutral rails. This ensures that every individual appliance receives the full operational potential difference of 220 V220\,\text{V} and can operate independently.

    • Switch Placement: All control switches must be situated on the Live wire. This guarantees that opening a switch fully de-energizes the appliance from the 220 V220\,\text{V} supply, mitigating electrocution risks during servicing.


Comprehensive structural wiring diagram of a residential building distribution box, lighting, and socket circuits

Summary of Physical Quantities, Units, and Triangle Relations

  • Physical Quantities and SI Units:

    • Charge: Symbol QQ, Unit name coulomb, Unit symbol C\text{C}

    • Current strength: Symbol II, Unit name ampere, Unit symbol A\text{A}

    • Time: Symbol tt, Unit name second, Unit symbol s\text{s}

    • Potential difference: Symbol VV, Unit name volt, Unit symbol V\text{V}

    • Resistance: Symbol RR, Unit name ohm, Unit symbol Ω\Omega

    • Work: Symbol WW, Unit name joule, Unit symbol J\text{J}

    • Energy: Symbol WW, Unit name joule, Unit symbol J\text{J}

  • Fundamental Electrical Formula Triangles:

    • Charge-Current-Time Triangle (Q=I⋅tQ = I \cdot t):     Q=I×tQ = I \times t     I=QtI = \frac{Q}{t}     t=QIt = \frac{Q}{I}

    • Work-Charge-Voltage Triangle (W=Q⋅VW = Q \cdot V):     W=Q×VW = Q \times V     V=WQV = \frac{W}{Q}     Q=WVQ = \frac{W}{V}

    • Ohm's Law Triangle (V=I⋅RV = I \cdot R):     V=I×RV = I \times R     I=VRI = \frac{V}{R}     R=VIR = \frac{V}{I}

Comprehensive Practice Problems and Worked Solutions

  • Theoretical Review Questions:

    • Question 1: What is the function of a cell in an electric circuit?

    • Answer: A cell acts as an electrical energy source; it performs work on charges to create and maintain an electrical potential difference, driving charge through the circuit.

    • Question 2: What is an electric current?

    • Answer: An electric current is a continuous flow of electrical charge.

    • Question 3: In what unit is an electric current measured?

    • Answer: The ampere (A\text{A}).

    • Question 4: How would you connect an ammeter in a circuit?

    • Answer: An ammeter is connected strictly in series with the component whose current is to be measured.

    • Question 5: Does an ammeter have a high or low resistance? Explain why this must be so.

    • Answer: An ammeter has an extremely low resistance (approaching zero). This ensures it introduces negligible total resistance into the branch, preventing it from reducing the current it is intended to measure.

    • Question 6: Which current direction do we use?

    • Answer: Conventional current direction (from the positive terminal to the negative terminal).

    • Question 7: Define a coulomb charge.

    • Answer: One coulomb is the quantity of electric charge that flows past a given cross-section of a conductor when a steady current of one ampere is sustained for one second (1 C=1 A×1 s1\,\text{C} = 1\,\text{A} \times 1\,\text{s}).

  • Charge, Current, and Time Calculations (Question 8):

    • Row a: Given I=2.5 AI = 2.5\,\text{A}, t=6 st = 6\,\text{s}.     Q=I×t=2.5 A×6 s=15 CQ = I \times t = 2.5\,\text{A} \times 6\,\text{s} = 15\,\text{C}

    • Row b: Given I=0.6 AI = 0.6\,\text{A}, t=30 st = 30\,\text{s}.     Q=I×t=0.6 A×30 s=18 CQ = I \times t = 0.6\,\text{A} \times 30\,\text{s} = 18\,\text{C}

    • Row c: Given Q=250 CQ = 250\,\text{C}, t=200 st = 200\,\text{s}.     I=Qt=250 C200 s=1.25 AI = \frac{Q}{t} = \frac{250\,\text{C}}{200\,\text{s}} = 1.25\,\text{A}

    • Row d: Given Q=300 CQ = 300\,\text{C}, t=1 minute=60 st = 1\,\text{minute} = 60\,\text{s}.     I=Qt=300 C60 s=5 AI = \frac{Q}{t} = \frac{300\,\text{C}}{60\,\text{s}} = 5\,\text{A}

    • Row e: Given Q=18 CQ = 18\,\text{C}, I=0.2 AI = 0.2\,\text{A}.     t=QI=18 C0.2 A=90 st = \frac{Q}{I} = \frac{18\,\text{C}}{0.2\,\text{A}} = 90\,\text{s}

    • Row f: Given Q=0.8 CQ = 0.8\,\text{C}, I=16 mA=0.016 AI = 16\,\text{mA} = 0.016\,\text{A}.     t=QI=0.8 C0.016 A=50 st = \frac{Q}{I} = \frac{0.8\,\text{C}}{0.016\,\text{A}} = 50\,\text{s}

  • Single-Variable Circuit Current Calculations:

    • Question 9: A current of 15 A15\,\text{A} flows in an electric heater for 12 s12\,\text{s}. Calculate the charge passing a point in the circuit:     Q=I×t=15 A×12 s=180 CQ = I \times t = 15\,\text{A} \times 12\,\text{s} = 180\,\text{C}

    • Question 10: A tape recorder draws 0.01 A0.01\,\text{A} for 5 minutes5\,\text{minutes} (5×60=300 s5 \times 60 = 300\,\text{s}). Calculate the charge drawn from the battery:     Q=I×t=0.01 A×300 s=3 CQ = I \times t = 0.01\,\text{A} \times 300\,\text{s} = 3\,\text{C}

    • Question 11: If 150 C150\,\text{C} passes through a circuit cross-section in 50 s50\,\text{s}, calculate the current:     I=Qt=150 C50 s=3 AI = \frac{Q}{t} = \frac{150\,\text{C}}{50\,\text{s}} = 3\,\text{A}

    • Question 12: A radio operates for 120 s120\,\text{s} with 60 C60\,\text{C} passing a point. Calculate current:     I=Qt=60 C120 s=0.5 AI = \frac{Q}{t} = \frac{60\,\text{C}}{120\,\text{s}} = 0.5\,\text{A}

    • Question 13: A resistor carries a current of 0.8 A0.8\,\text{A}. Calculate the time required for 200 C200\,\text{C} to pass through:     t=QI=200 C0.8 A=250 st = \frac{Q}{I} = \frac{200\,\text{C}}{0.8\,\text{A}} = 250\,\text{s}

  • Potential Difference and Work Concepts:

    • Question 14: What is meant by the electrical potential difference between two points on a conductor?

    • Answer: It is the amount of work done or energy transformed per unit electric charge as it moves between those two specified points (V=WQV = \frac{W}{Q}).

    • Question 15: What unit is used to measure electrical potential difference?

    • Answer: The volt (V\text{V}).

    • Question 16: Which apparatus is used to measure potential difference, and how must it be connected?

    • Answer: A voltmeter, connected in parallel across the two points or components of interest.

    • Question 17: Calculate the potential difference between points XX and YY if 120 J120\,\text{J} of work is required to move 40 C40\,\text{C} between them:     V=WQ=120 J40 C=3 VV = \frac{W}{Q} = \frac{120\,\text{J}}{40\,\text{C}} = 3\,\text{V}

  • Potential Difference, Work, and Charge Calculations (Question 18):

    • Row a: Given W=88 JW = 88\,\text{J}, Q=4 CQ = 4\,\text{C}.     V=WQ=88 J4 C=22 VV = \frac{W}{Q} = \frac{88\,\text{J}}{4\,\text{C}} = 22\,\text{V}

    • Row b: Given V=6 VV = 6\,\text{V}, Q=25 CQ = 25\,\text{C}.     W=V×Q=6 V×25 C=150 JW = V \times Q = 6\,\text{V} \times 25\,\text{C} = 150\,\text{J}

    • Row c: Given V=9 VV = 9\,\text{V}, W=54 JW = 54\,\text{J}.     Q=WV=54 J9 V=6 CQ = \frac{W}{V} = \frac{54\,\text{J}}{9\,\text{V}} = 6\,\text{C}

    • Row d: Given V=4.5 VV = 4.5\,\text{V}, W=2.5 JW = 2.5\,\text{J}.     Q=WV=2.5 J4.5 V=59≈0.56 CQ = \frac{W}{V} = \frac{2.5\,\text{J}}{4.5\,\text{V}} = \frac{5}{9} \approx 0.56\,\text{C}

  • Work and Energy Applications:

    • Question 19: Calculate the potential difference across a resistor requiring 20 J20\,\text{J} of work to move 8 C8\,\text{C} through it:     V=WQ=20 J8 C=2.5 VV = \frac{W}{Q} = \frac{20\,\text{J}}{8\,\text{C}} = 2.5\,\text{V}

    • Question 20: Calculate work done when moving 1.5 C1.5\,\text{C} through a potential difference of 220 V220\,\text{V}:     W=Q×V=1.5 C×220 V=330 JW = Q \times V = 1.5\,\text{C} \times 220\,\text{V} = 330\,\text{J}

    • Question 21: If 60 J60\,\text{J} of work is performed to move charge through a potential difference of 10 V10\,\text{V}, calculate the charge moved:     Q=WV=60 J10 V=6 CQ = \frac{W}{V} = \frac{60\,\text{J}}{10\,\text{V}} = 6\,\text{C}

  • Resistance, Current, and Potential Difference Calculations (Question 22):

    • Row a: Given I=6 AI = 6\,\text{A}, V=24 VV = 24\,\text{V}.     R=VI=24 V6 A=4 ΩR = \frac{V}{I} = \frac{24\,\text{V}}{6\,\text{A}} = 4\,\Omega

    • Row b: Given R=25 ΩR = 25\,\Omega, I=3.2 AI = 3.2\,\text{A}.     V=I×R=3.2 A×25 Ω=80 VV = I \times R = 3.2\,\text{A} \times 25\,\Omega = 80\,\text{V}

    • Row c: Given I=0.2 AI = 0.2\,\text{A}, V=16 VV = 16\,\text{V}.     R=VI=16 V0.2 A=80 ΩR = \frac{V}{I} = \frac{16\,\text{V}}{0.2\,\text{A}} = 80\,\Omega

    • Row d: Given R=4.5 ΩR = 4.5\,\Omega, V=0.9 VV = 0.9\,\text{V}.     I=VR=0.9 V4.5 Ω=0.2 AI = \frac{V}{R} = \frac{0.9\,\text{V}}{4.5\,\Omega} = 0.2\,\text{A}

  • Ohm's Law Applications:

    • Question 23: When the potential difference across a resistor is 6 V6\,\text{V}, current is 2 A2\,\text{A}. Determine resistance:     R=VI=6 V2 A=3 ΩR = \frac{V}{I} = \frac{6\,\text{V}}{2\,\text{A}} = 3\,\Omega

    • Question 24: Calculate potential difference required to drive 6 A6\,\text{A} through a 12 Ω12\,\Omega resistor:     V=I×R=6 A×12 Ω=72 VV = I \times R = 6\,\text{A} \times 12\,\Omega = 72\,\text{V}

    • Question 25: A potential difference of 200 V200\,\text{V} is applied to an 80 Ω80\,\Omega conductor. Calculate current:     I=VR=200 V80 Ω=2.5 AI = \frac{V}{R} = \frac{200\,\text{V}}{80\,\Omega} = 2.5\,\text{A}

    • Question 26: Across a resistor with potential difference 30 V30\,\text{V}, a charge of 120 C120\,\text{C} flows in 15 s15\,\text{s}.

    • (a) Current:
            I=Qt=120 C15 s=8 AI = \frac{Q}{t} = \frac{120\,\text{C}}{15\,\text{s}} = 8\,\text{A}

    • (b) Resistance:
            R=VI=30 V8 A=3.75 ΩR = \frac{V}{I} = \frac{30\,\text{V}}{8\,\text{A}} = 3.75\,\Omega

    • Question 27: A potential difference of 20 V20\,\text{V} yields a current of 0.4 A0.4\,\text{A}.

    • (a) Charge flowing per minute (t=60 st = 60\,\text{s}):
            Q=I×t=0.4 A×60 s=24 CQ = I \times t = 0.4\,\text{A} \times 60\,\text{s} = 24\,\text{C}

    • (b) Value of the resistor:
            R=VI=20 V0.4 A=50 ΩR = \frac{V}{I} = \frac{20\,\text{V}}{0.4\,\text{A}} = 50\,\Omega

    • Question 28: A potential difference of 24 V24\,\text{V} is applied across a 60 Ω60\,\Omega resistor.

    • (a) Charge passing through in 10 s10\,\text{s}:
            I=VR=24 V60 Ω=0.4 AI = \frac{V}{R} = \frac{24\,\text{V}}{60\,\Omega} = 0.4\,\text{A}       Q=I×t=0.4 A×10 s=4 CQ = I \times t = 0.4\,\text{A} \times 10\,\text{s} = 4\,\text{C}

    • (b) Work done in this time:
            W=Q×V=4 C×24 V=96 JW = Q \times V = 4\,\text{C} \times 24\,\text{V} = 96\,\text{J}

    • Question 29: A potential difference of 6 V6\,\text{V} is maintained across a 20 Ω20\,\Omega resistor.

    • (a) Charge passing per minute (t=60 st = 60\,\text{s}):
            I=VR=6 V20 Ω=0.3 AI = \frac{V}{R} = \frac{6\,\text{V}}{20\,\Omega} = 0.3\,\text{A}       Q=I×t=0.3 A×60 s=18 CQ = I \times t = 0.3\,\text{A} \times 60\,\text{s} = 18\,\text{C}

    • (b) Work done in this time:
            W=Q×V=18 C×6 V=108 JW = Q \times V = 18\,\text{C} \times 6\,\text{V} = 108\,\text{J}

Complex Circuit Network Analysis

  • Series Circuit Analysis (Question 30):

    • Three resistors (R1=6 ΩR_1 = 6\,\Omega, R2=1 ΩR_2 = 1\,\Omega, and R3=3 ΩR_3 = 3\,\Omega) are wired in series across a 20 V20\,\text{V} DC source.


Series circuit schematic with a 20V battery driving three resistors: 6 ohms, 1 ohm, and 3 ohms
  • (a) Total Effective Resistance:
        RTOT=R1+R2+R3=6 Ω+1 Ω+3 Ω=10 ΩR_{\text{TOT}} = R_1 + R_2 + R_3 = 6\,\Omega + 1\,\Omega + 3\,\Omega = 10\,\Omega

  • (b) Circuit Current:
        I=VRTOT=20 V10 Ω=2 AI = \frac{V}{R_{\text{TOT}}} = \frac{20\,\text{V}}{10\,\Omega} = 2\,\text{A}

  • (c) Potential Difference Across the 3 Ω3\,\Omega Resistor:
        V3Ω=I×R3=2 A×3 Ω=6 VV_{3\Omega} = I \times R_3 = 2\,\text{A} \times 3\,\Omega = 6\,\text{V}

    • Parallel Resistor Network Analysis (Question 32):


Three parallel resistor configurations for equivalent resistance determination
  • Network (a): Resistors of 6 Ω6\,\Omega and 24 Ω24\,\Omega in parallel:     1Req=16+124=4+124=524\frac{1}{R_{\text{eq}}} = \frac{1}{6} + \frac{1}{24} = \frac{4 + 1}{24} = \frac{5}{24}     Req=245=4.8 ΩR_{\text{eq}} = \frac{24}{5} = 4.8\,\Omega

  • Network (b): Resistors of 12 Ω12\,\Omega, 6 Ω6\,\Omega, and 4 Ω4\,\Omega in parallel:     1Req=112+16+14=1+2+312=612=12\frac{1}{R_{\text{eq}}} = \frac{1}{12} + \frac{1}{6} + \frac{1}{4} = \frac{1 + 2 + 3}{12} = \frac{6}{12} = \frac{1}{2}     Req=2 ΩR_{\text{eq}} = 2\,\Omega

  • Network (c): Resistors of 20 Ω20\,\Omega, 5 Ω5\,\Omega, and 4 Ω4\,\Omega in parallel:     1Req=120+15+14=1+4+520=1020=12\frac{1}{R_{\text{eq}}} = \frac{1}{20} + \frac{1}{5} + \frac{1}{4} = \frac{1 + 4 + 5}{20} = \frac{10}{20} = \frac{1}{2}     Req=2 ΩR_{\text{eq}} = 2\,\Omega

    • Compound and Geometric Resistor Combinations (Question 33):


Compound bridge, loop, and delta resistor configurations
  • Combination (d): Top parallel branch comprises a series combination of 6 Ω6\,\Omega and 4 Ω4\,\Omega; bottom branch comprises a 30 Ω30\,\Omega resistor.

    • Resistance of top branch:
            Rtop=6 Ω+4 Ω=10 ΩR_{\text{top}} = 6\,\Omega + 4\,\Omega = 10\,\Omega

    • Total equivalent resistance of the parallel combination:
            1Req=110+130=3+130=430\frac{1}{R_{\text{eq}}} = \frac{1}{10} + \frac{1}{30} = \frac{3 + 1}{30} = \frac{4}{30}       Req=304=7.5 ΩR_{\text{eq}} = \frac{30}{4} = 7.5\,\Omega

  • Combination (e): Square closed-loop network with terminal leads connected across opposite diagonal vertices. The perimeter consists of resistors of 4 Ω4\,\Omega, 2 Ω2\,\Omega, 2 Ω2\,\Omega, and 4 Ω4\,\Omega.

    • Current entering the node splits into two parallel paths:

      • Path 1: 4 Ω+2 Ω=6 Ω4\,\Omega + 2\,\Omega = 6\,\Omega

      • Path 2: 4 Ω+2 Ω=6 Ω4\,\Omega + 2\,\Omega = 6\,\Omega

    • Total equivalent resistance:
            Req=6 Ω×6 Ω6 Ω+6 Ω=3612=3 ΩR_{\text{eq}} = \frac{6\,\Omega \times 6\,\Omega}{6\,\Omega + 6\,\Omega} = \frac{36}{12} = 3\,\Omega

  • Combination (f): Triangular (delta) network connected across the bottom base terminals. The base is a 3 Ω3\,\Omega resistor; the upper apex path consists of a 2 Ω2\,\Omega and a 4 Ω4\,\Omega resistor in series.

    • Upper path series resistance:
            Rupper=2 Ω+4 Ω=6 ΩR_{\text{upper}} = 2\,\Omega + 4\,\Omega = 6\,\Omega

    • Base path resistance:
            Rbase=3 ΩR_{\text{base}} = 3\,\Omega

    • Total equivalent resistance:
            Req=6 Ω×3 Ω6 Ω+3 Ω=189=2 ΩR_{\text{eq}} = \frac{6\,\Omega \times 3\,\Omega}{6\,\Omega + 3\,\Omega} = \frac{18}{9} = 2\,\Omega

    • Series-Parallel Network Analysis (Question 34):

  • A circuit consists of a 10 Ω10\,\Omega resistor connected in series with a parallel combination of a 6 Ω6\,\Omega and a 3 Ω3\,\Omega resistor.


Series-parallel combination circuit with a 10 ohm resistor in series with parallel 6 ohm and 3 ohm resistors
  • (a) Total Resistance of the Circuit:

    • Calculate parallel bank equivalent resistance:
            Rparallel=6 Ω×3 Ω6 Ω+3 Ω=189=2 ΩR_{\text{parallel}} = \frac{6\,\Omega \times 3\,\Omega}{6\,\Omega + 3\,\Omega} = \frac{18}{9} = 2\,\Omega

    • Add the series resistor:
            RTOT=10 Ω+Rparallel=10 Ω+2 Ω=12 ΩR_{\text{TOT}} = 10\,\Omega + R_{\text{parallel}} = 10\,\Omega + 2\,\Omega = 12\,\Omega

  • (b) Readings on Main Ammeters (A1A_1 and A2A_2):

    • Located on the main branch, both ammeters record total circuit current:
            Imain=VsupplyRTOT=Vsupply12 ΩI_{\text{main}} = \frac{V_{\text{supply}}}{R_{\text{TOT}}} = \frac{V_{\text{supply}}}{12\,\Omega}

  • (c) Reading on Voltmeter V2V_2:

    • Measures potential difference across the 10 Ω10\,\Omega series resistor:
            V2=Imain×10 ΩV_2 = I_{\text{main}} \times 10\,\Omega

  • (d) Reading on Voltmeters V3V_3 and V4V_4:

    • Connected across the parallel network; both register the identical potential drop across the parallel combination:
            V3=V4=Imain×2 Ω=VparallelV_3 = V_4 = I_{\text{main}} \times 2\,\Omega = V_{\text{parallel}}

  • (e) Readings on Branch Ammeters (A3A_3 and A4A_4):

    • Current divides through the parallel branches inversely according to branch resistance:
            IA3=Vparallel6 ΩI_{A3} = \frac{V_{\text{parallel}}}{6\,\Omega}       IA4=Vparallel3 ΩI_{A4} = \frac{V_{\text{parallel}}}{3\,\Omega}

    • Ratio check: Current through A4A_4 is twice that through A3A_3 (IA4=2×IA3I_{A4} = 2 \times I_{A3}), and IA3+IA4=ImainI_{A3} + I_{A4} = I_{\text{main}}.

    • Dual-Control Doorbell Circuit Design (Question 35):

  • Design goal: Connect a single audible doorbell unit, a common DC electrical power source, and two push-button switches (front door and back door) so that each switch can independently activate the doorbell.

  • Circuit configuration:

    • The front door push-button switch and back door push-button switch are wired in parallel with each other.

    • This parallel switch sub-assembly is wired in series with the single doorbell unit and the DC power source.

    • Functional operation: Closing the front door switch completes the conducting circuit loop independently of the back door switch; similarly, closing the back door switch completes the loop independently. If both switches are closed simultaneously, the circuit remains closed and the bell rings normally.