Comprehensive Study Notes for National Certificate in Electrical Power Engineering
National Certificate in Electrical Power Engineering Study Notes
LO2 – Describe Electric Circuits
2.1 SI Units of Charge, Force, Work and Power
The International System of Units (SI) provides standard units for physical quantities in electrical engineering.
Quantity: Current
Symbol: I
SI Unit: Ampere (A)
Formula: I = \frac{Q}{t}Quantity: Charge
Symbol: Q
SI Unit: Coulomb (C)
Formula: Q = I \times tQuantity: Force
Symbol: F
SI Unit: Newton (N)
Formula: F = m \times aQuantity: Work
Symbol: W
SI Unit: Joule (J)
Formula: W = V \times QQuantity: Power
Symbol: P
SI Unit: Watt (W)
Formulas:P = \frac{W}{t}
P = V \times I
Quantity: Potential
Symbol: V
SI Unit: Volt (V)
Formula: V = \frac{W}{Q}Quantity: EMF
Symbol: E
SI Unit: Volt (V)
Formula: E = V + IrQuantity: Resistance
Symbol: R
SI Unit: Ohm (Ω)
Formula: R = \frac{V}{I}Quantity: Conductance
Symbol: G
SI Unit: Siemens (S)
Formula: G = \frac{1}{R}Quantity: Energy
Symbol: E
SI Unit: Joule (J)
Formula: E = P \times t
Charge, Work, and Power Calculations
Charge Calculation: Q = I \times t
Example: If I = 3 \, A and t = 10 \, s, then Q = 3 \times 10 = 30 \, C
Work Calculation: W = V \times Q
Example: If V = 12 \, V and Q = 5 \, C, then W = 12 \times 5 = 60 \, J
Power Calculation:
Formulas:
P = V \times I
P = I^2 R
P = \frac{V^2}{R}
Example:
Given V = 12 \, V, I = 3 \, A, R = 4 \, Ω,
All forms yield same power:
P = 12 \times 3 = 36 \, W
P = 9 \times 4 = 36 \, W
P = \frac{144}{4} = 36 \, W
Electrical Energy Calculation: E = P \times t
Energy in Joules when P is in Watts and t is in seconds.
Example: For a 2 kW heater operating for 3 hours,
E = 2 \times 3 = 6 \, kWh = 21,600,000 \ J
2.2 Resistance vs Conductance
Resistance Calculation:
R = \frac{V}{I}Current Calculation - Ohm's Law:
I = \frac{V}{R}Voltage Calculation - Ohm's Law:
V = I \times RConductance Calculation:
G = \frac{1}{R}Resistance vs Conductance:
Resistance (R): Opposition to current flow, expressed in Ohms (Ω).
Higher R means less current.
Conductance (G): Ease of current flow, expressed in Siemens (S).
Higher G means higher current flow.
2.3 Electrical Power vs Energy
Power: Rate of Energy Use
Unit: Watt (W)
Formula: P = V \times I
Energy: Total Energy Used
Unit: Joule (J) or kWh
Formula: E = P \times t
Linear and Non-Linear Devices
Linear Devices: Obey Ohm's Law; resistance remains constant (e.g., resistors).
Non-Linear Devices: Do not obey Ohm's Law; resistance varies with voltage or temperature (e.g., diodes, thermistors, LDRs).
Resistance and Resistivity
Resistive Formula: R = \frac{\rho L}{A}
Where
\rho (rho) is resistivity (Ω·m),
L is length (m),
A is cross-sectional area (m²).
Factors Affecting Resistance:
Longer wire: Increases R.
Thicker wire (larger A): Decreases R.
High resistivity material: Increases R.
Higher temperature (metals): Increases R.
Example Calculation:
For Copper: \rho = 1.7 \times 10^{-8} \ Ω·m, L = 5 \, m, A = 2 \times 10^{-6} \ m²,
R = \frac{1.7 \times 10^{-8} \times 5}{2 \times 10^{-6}} = 0.0425 \ Ω
Temperature Coefficient of Resistance
Formula: R_T = R_0 (1 + \alpha T)
Where
R_0 = resistance at 0°C,
\alpha = temperature coefficient (per °C),
T = temperature (°C).
Behavior:
Metals (\alpha positive): Resistance increases with temperature.
Semiconductors (\alpha negative): Resistance decreases with temperature.
Example Calculation:
For a resistor with R_0 = 50 \, Ω, \alpha = 0.004/°C, T = 75°C,
R_T = 50(1 + 0.004 \times 75) = 50 \times 1.3 = 65 \, Ω
Resistor Colour Coding
4-band Resistor Color Code:
Bands:
Band 1 & 2: Digits
Band 3: Multiplier
Band 4: Tolerance
Example:
Brown, Black, Red, Gold
Values: 1, 0, ×100, ±5% = 1,000 Ω = 1 kΩ ±5%
Multiples and Sub-multiples
Prefix Table:
Mega (M): \times 10^6
Kilo (k): \times 10^3
Milli (m): \times 10^{-3}
Micro (µ): \times 10^{-6}
Nano (n): \times 10^{-9}
Pico (p): \times 10^{-12}
Conversion Examples:
3 MΩ = 3,000,000 Ω
4.7 kΩ = 4,700 Ω
Main Effects of Electric Current
Heating Effect: ext{Heat} = I^2 R t (Joules).
Used in: heaters, toasters, fuses.
Magnetic Effect: Current produces a magnetic field around a conductor.
Basis for: motors, relays, electromagnets.
Chemical Effect: Current through an electrolyte causes electrolysis.
Used in: electroplating, battery charging, metal refining.
Fuses
Fuse Design: A thin wire that melts and breaks the circuit when current exceeds safety level.
Calculation for Fuse Size: I = \frac{P}{V}
Choose the next standard fuse size above this value.
Example:
For a 500 W appliance on 240 V:
I = \frac{500}{240} = 2.08 \, AChoose a 3 A fuse.
LO3 – Batteries and Alternative Sources of Energy
The Simple Cell
Construction: Two different metal electrodes in an electrolyte.
Chemical reaction drives electrons from the negative terminal (zinc) to the positive terminal (copper).
Polarisation Issue: Hydrogen bubbles form on the copper electrode, increasing internal resistance and reducing current.
Solution: Use a depolarizer (e.g., manganese dioxide).
Local Action Issue: Impurities in zinc cause energy wastage even when no current is drawn.
Solution: Amalgamate zinc with mercury.
EMF and Internal Resistance
Formula for EMF:
E = V + IrTerminal Voltage Formula:
V = E - IrCircuit Current Formula: I = \frac{E}{R + r}
Where
E = EMF (V),
V = terminal voltage (V),
I = current (A),
r = internal resistance (Ω),
R = external resistance (Ω).
Analogue: EMF represents salary; internal resistance represents tax; terminal voltage represents take-home pay.
Example:
E = 6 \, V, r = 0.5 \, Ω, R = 2.5 \, Ω
Results: I = \frac{6}{3} = 2 \, A and V = 6 - (2 \times 0.5) = 5 \, V (1 V lost internally).
Cell Capacity
Formula:
ext{Capacity (Ah)} = I \times tDuration Calculation:
t = \frac{ ext{Capacity}}{I}Example:
Capacity = 60 Ah, I = 4 \, A
Time: t = \frac{60}{4} = 15 \, hours
Primary vs Secondary Cells
Features of Primary Cells:
Not rechargeable: No
Reaction: Irreversible
Internal Resistance: Higher
Cost: Cheap
Examples: Zinc-carbon, alkaline
Features of Secondary Cells:
Rechargeable: Yes
Reaction: Reversible
Internal Resistance: Lower
Cost: Expensive
Examples: Lead-acid, Li-ion, NiCd
Applications:
Primary: Torches, remotes
Secondary: Cars, phones, UPS
Lead-Acid Battery (Secondary Cell)
Composition:
Positive Plate: Lead dioxide (PbO2)
Negative Plate: Spongy lead (Pb)
Electrolyte: Dilute sulphuric acid (H₂SO₄)
Nominal Voltage per Cell:
2 V → 12 V battery = 6 cells in series
Charging and Discharging Process:
Discharging: Chemical → Electrical
Charging: Electrical → Chemical
Electrolyte: Weaker during discharging, stronger during charging
Plates: Both convert to lead sulphate during discharge, restored to original form during charge
Safe Disposal of Batteries
Disposal Instructions:
Never throw in ordinary waste bins due to toxic contents.
Dispose at designated recycling points.
Avoid burning or crushing due to explosion risks and toxic gas release.
Handle leaking batteries with protective gloves.
Renewable Energy Sources
Solar (PV): Converts sunlight to electricity via panels.
Formula: P = \eta \times A \times G
Wind: Wind drives turbines.
Formula: P = \frac{1}{2}\rho A v^3
Hydropower: Flowing water drives turbines.
Formula: P = \rho g Q h
Geothermal: Earth's heat produces steam.
Biomass: Organic material undergoes combustion/processing.
Hydropower Example:
Given: Q = 2 \, m³/s, h = 10 \, m
Calculation: P = 1000 \times 9.81 \times 2 \times 10 = 196200 \, W \approx 196.2 \, kW
LO4 – Series and Parallel Networks
Series Circuits
Rules:
Same current throughout the circuit.
Voltages add up.
Resistances add up.
R_T = R_1 + R_2 + R_3Current Calculation:
I = \frac{V_T}{R_T}Voltage Calculation:
V_1 = I \times R_1,
V_2 = I \times R_2,
V_3 = I \times R_3Total Voltage Calculation:
V_T = V_1 + V_2 + V_3
Example:
For resistors R_1 = 2 \, Ω, R_2 = 3 \, Ω, R_3 = 5 \, Ω, and V = 20 \, V:
R_T = 10 \, Ω
I = 2 \, A
Calculated Voltages:
V_1 = 4 \, V
V_2 = 6 \, V
V_3 = 10 \, V
Verification: 4 + 6 + 10 = 20 \, V ✓
Potential Divider
Formula: V_{out} = V_{in} \times \frac{R_2}{(R_1 + R_2)}
Explanation: The output voltage is taken across R_2. The larger the R_2 relative to R_1, the greater the voltage received by R_2.
Example:
Given: V_{in} = 15 \, V, R_1 = 5 \, Ω, R_2 = 10 \, Ω
Calculation:
V_{out} = 15 \times \frac{10}{15} = 10 \, V
Parallel Circuits
Rules:
Same voltage across each branch.
Currents add up.
Total resistance is less than the smallest branch resistance.
Formula for total resistance:
\frac{1}{R_T} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3}
Shortcut for Two Resistors:
R_T = \frac{R_1 \times R_2}{(R_1 + R_2)}Current Calculations:
I_T = \frac{V}{R_T}
For branch currents: I_1 = \frac{V}{R_1}, I_2 = \frac{V}{R_2}
Verification:
I_T = I_1 + I_2 + I_3
Example:
Given: R_1 = 4 \, Ω, R_2 = 6 \, Ω, R_3 = 12 \, Ω, V = 12 \, V
Calculation:
\frac{1}{R_T} = \frac{3}{12} + \frac{2}{12} + \frac{1}{12} = \frac{6}{12}
Thus R_T = 2 \, Ω
And I_T = 6 \, A
For Branches:
I_1 = 3 \, A, I_2 = 2 \, A, I_3 = 1 \, A
Verification:
Total Currents: 3 + 2 + 1 = 6 \, A ✓
Current Division
Formulas:
For resistors R_1 and R_2:
I_1 = I_T \times \frac{R_2}{(R_1 + R_2)}
I_2 = I_T \times \frac{R_1}{(R_1 + R_2)}Note: Current through smaller resistor increase in comparison to larger resistor.
Example:
Given: I_T = 12 \, A, R_1 = 8 \, Ω, R_2 = 4 \, Ω:
Calculation:
I_1 = 12 \times \frac{4}{12} = 4 \, A
I_2 = 12 \times \frac{8}{12} = 8 \, A
Verification:
Total: 4 + 8 = 12 \, A ✓
Relative and Absolute Voltages
Definitions:
Absolute Voltage: Measured from earth (0 V reference).
Relative Voltage: Voltage difference between two points — can be positive or negative.
Example:
If Point A = 10 V, Point B = 4 V:
V_A relative to B = 10 - 4 = +6 \, V
V_B relative to A = 4 - 10 = -6 \, V
Wiring Lamps – Series vs Parallel
Comparison:
Series:
Brightness: Dimmer (voltage is shared)
One lamp failure: All go out
Voltage per lamp: \frac{V_{supply}}{n}
Total resistance: Increases with each lamp
Applications: Decorative/fairy lights
Parallel:
Brightness: Full brightness
One lamp failure: Others stay on
Voltage per lamp: Full supply voltage
Total resistance: Decreases with each lamp
Applications: Home & commercial lighting.
LO5 – Capacitors and Capacitance
What is a Capacitor?
A capacitor is a device that stores electrical charge. It consists of two conducting plates separated by an insulating material known as a dielectric. It allows AC signals to pass through but blocks DC once fully charged.
Capacitance
Formula for Capacitance: C = \frac{Q}{V}
Rearranged:
Q = C \times V
V = \frac{Q}{C}
Units: Capacitance is measured in Farads (F), charge in Coulombs (C), and voltage in Volts (V).
Example Calculation:
For a 100 µF capacitor charged to 50 V:
Q = 100 \times 10^{-6} \times 50 = 0.005 C = 5 \, mC
Electric Field Strength
Formula for Electric Field Strength: E = \frac{V}{d}
Where V = voltage across plates (V) and d = distance between plates (m).
Example Calculation:
For V = 500 \, V and d = 0.005 \, m,
E = \frac{500}{0.005} = 100000 \, V/m = 100 \, kV/m
Electric Flux Density
Formula for Electric Flux Density: D = \frac{Q}{A}
Where D = flux density (C/m²), Q = charge on plate (C), and A = plate area (m²).
Example Calculation:
For Q = 0.002 \, C and A = 0.01 \, m²,
D = \frac{0.002}{0.01} = 0.2 \, C/m²
Permittivity
Formula for Permittivity: \epsilon = \epsilon_0 \times \epsilon_r
Where \epsilon_0 = 8.85 \times 10^{-12} \, F/m (constant) and \epsilon_r is the relative permittivity of the dielectric (given).
Approximate Values for Common Materials:
Air/vacuum: \epsilon_r = 1
Paper: \epsilon_r = 2 - 2.5
Polyester: \epsilon_r = 3 - 4
Mica: \epsilon_r = 5 - 7
Ceramic: \epsilon_r = 10 - 1000+
Parallel Plate Capacitor
Capacitance Formula for Parallel Plates: C = \frac{\epsilon_0 \epsilon_r A}{d}
Influence on Capacitance:
Increase plate area A → C increases
Decrease plate separation d → C increases
Use dielectric with higher \epsilon_r → C increases
Example Calculation:
For \epsilon_r = 4, A = 0.02 \, m², d = 0.002 \, m,
C = \frac{8.85 \times 10^{-12} \times 4 \times 0.02}{0.002} = 354 \ pF
Capacitors in Parallel and Series
Capacitors in Parallel:
Total Capacitance:
C_T = C_1 + C_2 + C_3Same voltage across all capacitors.
Example:
For C_1 = 4 \, µF, C_2 = 6 \, µF, C_3 = 10 \, µF,
C_T = 20 \, µF
Capacitors in Series:
Total Capacitance:
\frac{1}{C_T} = \frac{1}{C_1} + \frac{1}{C_2} + \frac{1}{C_3}Shortcut for Two Capacitors:
C_T = \frac{C_1 \times C_2}{(C_1 + C_2)}Same charge on each capacitor.
Total Voltage Calculation:
V_T = V_1 + V_2 + V_3Example:
For C_1 = 6 \, µF, C_2 = 3 \, µF, C_3 = 2 \, µF, \frac{1}{C_T} = \frac{1}{6} + \frac{1}{3} + \frac{1}{2} = 1
Thus, C_T = 1 \, µF
Dielectric Strength
Formula for Maximum Voltage: ext{Max V} = ext{Dielectric Strength} \times d
Where d is the plate separation (m).
Example Calculation:
For dielectric strength of 20 kV/mm and d = 0.5 mm,
ext{Max V} = 20 \times 0.5 = 10 kVNote: Exceeding this voltage permanently damages the capacitor.
Energy Stored in a Capacitor
Energy Formula: E = \frac{1}{2} C V^2 = \frac{Q^2}{2C} = \frac{QV}{2}
Example Calculation:
For C = 200 \, µF and V = 100 \, V:
E = \frac{1}{2} \times 200 \times 10^{-6} \times 10,000 = 1 \, J
RC Time Constant
Formula for Time Constant:
\tau = R \times CInterpretation: Time constant \tau indicates how fast a capacitor charges/discharges through a resistor.
Charging/Discharging Characteristics:
1\tau → 63.2% charge
2\tau → 86.5% charge
3\tau → 95.0% charge
4\tau → 98.2% charge
5\tau → ≈ 100% charge (fully charged)
1\tau → 36.8% remaining
2\tau → 13.5% remaining
3\tau → 5.0% remaining
4\tau → 1.8% remaining
5\tau → ≈ 0% (fully discharged)
Example Calculation:
For R = 22 \, kΩ and C = 47 \, µF:
\tau = 22000 \times 47 \times 10^{-6} = 1.034 \, sFully charged after 5\tau ≈ 5.17 \, s
Practical Types of Capacitors
Types and Applications:
Electrolytic: Uses aluminum oxide dielectric; suitable for large capacitance in power supplies.
Ceramic: Uses ceramic dielectric; suitable for high-frequency circuits.
Polyester (film): Uses plastic film dielectric; general-purpose applications.
Mica: Uses mica dielectric; suitable for precision and high frequency.
LO6 – Magnetism
6.1 Electromagnetism
Magnetic Field Due to Electric Current
Principle: When current flows through a conductor, a circular magnetic field is generated around it.
Right-Hand Grip Rule: Grip the conductor with your right hand; the thumb points in the direction of current, and the fingers curl in the direction of the magnetic field.
Magnetic Field Strength Formula: H = \frac{NI}{l}
Where
N = number of turns,
I = current (A),
l = length of coil (m).
Example Calculation:
For N = 500, I = 2 \, A, l = 0.1 \, m:
H = \frac{500 \times 2}{0.1} = 10,000 \, A/m
Magnetic Flux Density
Formula: B = \mu_0 \mu_r H
Units: Tesla (T)
Where:
\mu_0 = 4 \pi \times 10^{-7} H/m,
\mu_r = relative permeability of core material.
Force on a Current-Carrying Conductor
Formula: F = BIL
Where:
B = magnetic flux density (T)
I = current (A)
L = length in field (m)
Example Calculation:
For B = 0.8 \, T, I = 5 \, A, L = 0.3 \, m:
F = 0.8 \times 5 \times 0.3 = 1.2 \, N
Fleming's Left-Hand Rule (for Motors)
Rule Summary:
First Finger = Field Direction
Second Finger = Current Direction
Thumb = Motion/Force Direction
Force on a Moving Charge
Formula: F = q v B
Where:
q = charge (C)
v = velocity (m/s)
B = flux density (T)
Example Calculation:
For q = 1.6 \times 10^{-19} \, C, v = 2 \times 10^{6} \, m/s, B = 0.3 \, T:
F = 1.6 \times 10^{-19} \times 2 \times 10^{6} \times 0.3 = 9.6 \times 10^{-14} \, N
DC Motor – Torque
Torque Formula: T = B I N A
Where:
T = torque (Nm)
N = number of coil turns
A = area of coil (m²)
Example Calculation:
For B = 0.5 \, T, I = 2 \, A, N = 50, A = 0.01 \, m²:
T = 0.5 \times 2 \times 50 \times 0.01 = 0.5 \, Nm
Function of Commutator: It reverses current direction every half turn, keeping rotation continuous.
6.2 Electromagnetic Induction
Faraday's Law:
Formula: E = N \times \frac{\Delta \Phi}{\Delta t}
Where:
N = number of turns,
\Delta \Phi = change in magnetic flux (Webers or Wb),
\Delta t = time (s).
Lenz's Law: The induced current flows in a direction that opposes the change causing it, hence the negative sign in the full formula.
Fleming's Right-Hand Rule (for Generators):
First Finger = Field
Second Finger = Induced Current
Thumb = Motion
Example Calculation:
For N = 200, \Delta \Phi = 0.05 \, Wb, \Delta t = 0.1 \, s:
E = 200 \times \frac{0.05}{0.1} = 100 \, V
Inductance of a Coil:
Formula:
L = \frac{N^2 \mu A}{l}Where:
L = inductance (Henrys, H)
N = number of turns
\mu = permeability of core material (H/m)
A = cross-sectional area (m²)
l = length of coil (m)
Example Calculation:
For N = 100, \mu = 4\pi \times 10^{-7} \ H/m, A = 0.01 \, m², l = 0.2 \, m:
L \approx 0.63 \, mH
Energy Stored in an Inductor:
Formula:
E = \frac{1}{2} L I^2Example Calculation:
For L = 2 \, H and I = 3 \, A:
E = \frac{1}{2} \times 2 \times 3^2 = 9 \, J
Mutual Inductance:
Formula for induced EMF: E_2 = M \times \frac{\Delta I_1}{\Delta t}
Where M = mutual inductance (H). The changing field of coil 1 induces an EMF in coil 2, applied in transformers.
Example Calculation:
For M = 0.5 \, H, \Delta I = 4 \, A, \Delta t = 0.2 \, s:
E = 0.5 \times \frac{4}{0.2} = 10 \, V
LO7 – Electrical Measuring Instruments and Measurements
Introduction: Forces in Analogue Instruments
Deflecting Force: Causes pointer movement proportional to the quantity measured.
Controlling Force: A hairspring returning the pointer to zero when current stops.
Damping Force: Prevents pointer oscillation, ensuring steady readings.
Moving-Coil Instrument
Mechanism: A permanent magnet provides a fixed field; current through a coil creates a force (F = BIL) that deflects the pointer against the hairspring.
Characteristics:
Measures DC only
Uniform (linear) scale
High accuracy and sensitivity
Not suitable for AC without a rectifier
Moving-Iron Instrument
Mechanism: Current through a coil magnetizes iron pieces inside; they either attract or repel, deflecting the pointer.
Characteristics:
Measures both AC and DC
Non-uniform (cramped lower end) scale
Robust and cheap
Less accurate than moving-coil
Affected by external magnetic fields.
Moving-Coil Rectifier Instrument
Mechanism: Can only read DC; adding a rectifier (diode bridge) converts AC to pulsating DC.
Characteristics:
Measures AC (via rectifier)
More accurate than moving-iron for AC
Uniform scale
Comparison Table: Measuring Instruments
Feature | Moving-Coil | Moving-Iron | Moving-Coil Rectifier |
|---|---|---|---|
Measures | DC only | AC and DC | AC (via rectifier) |
Accuracy | High | Moderate | Good |
Scale | Uniform | Non-uniform | Uniform |
Cost | Higher | Lower | Moderate |
Sensitivity | High | Lower | High |
External field effect | Low | High | Low |
Construction | Permanent magnet + coil | Coil + iron pieces | Moving-coil + rectifier |
Connection of Meters in Circuits
Instrument | Measures | Connected | Internal Resistance
Ammeter | Current (A) | In SERIES | Very LOW
Voltmeter | Voltage (V) | In PARALLEL | Very HIGH
Ohmmeter | Resistance (Ω) | Directly across component | —
Wattmeter | Power (W) | Current coil in series; voltage coil in parallel | —
Connection Notes:
Ammeter: Should have very low resistance so it does not affect circuit current.
Voltmeter: Should have very high resistance to draw negligible current.
Master Formula Reference – All Learning Outcomes
Formula Table:
| Quantity Found | Formula | Learning Outcome |
|----------------|-------------|------------------|
| Charge (C) | Q = I \times t | LO2 |
| Work / Energy (J) | W = V \times Q | LO2 |
| Power (W) | P = V \times I, P = I^2R, P = \frac{V^2}{R} | LO2 |
| Electrical energy (J / kWh) | E = P \times t | LO2 |
| Voltage (V) − Ohm's Law | V = I \times R | LO2 |
| Current (A) − Ohm's Law | I = \frac{V}{R} | LO2 |
| Resistance (Ω) − Ohm's Law | R = \frac{V}{I} | LO2 |
| Conductance (S) | G = \frac{1}{R} | LO2 |
| Resistance from material properties | R = \frac{\rho L}{A} | LO2 |
| Resistance at temperature T | R_T = R_0(1 + \alpha T) | LO2 |
| Fuse current rating | I = \frac{P}{V} | LO2 |
| Terminal voltage (V) | V = E − Ir | LO3 |
| Circuit current with internal resistance | I = \frac{E}{(R + r)} | LO3 |
| Cell capacity (Ah) | Capacity = I \times t | LO3 |
| Hydropower (W) | P = \rho g Q h | LO3 |
| Total series resistance | R_T = R_1 + R_2 + R_3 | LO4 |
| Total parallel resistance | \frac{1}{R_T} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} | LO4 |
| Parallel resistance (2 resistors) | R_T = \frac{R_1 \times R_2}{(R_1 + R_2)} | LO4 |
| Potential divider output | V_{out} = V_{in} \times \frac{R_2}{(R_1 + R_2)} | LO4 |
| Current division (branch 1) | I_1 = I_T \times \frac{R_2}{(R_1 + R_2)} | LO4 |
| Capacitance (F) | C = \frac{Q}{V} | LO5 |
| Electric field strength (V/m) | E = \frac{V}{d} | LO5 |
| Electric flux density (C/m²) | D = \frac{Q}{A} | LO5 |
| Parallel plate capacitance | C = \frac{\epsilon \epsilon_r A}{d} | LO5 |
| Total parallel capacitance | C_T = C_1 + C_2 + C_3 | LO5 |
| Total series capacitance | \frac{1}{C_T} = \frac{1}{C_1} + \frac{1}{C_2} + \frac{1}{C_3} | LO5 |
| Energy in capacitor (J) | E = \frac{1}{2} C V^2 | LO5 |
| RC time constant (s) | \tau = R \times C | LO5 |
| Magnetic field strength (A/m) | H = \frac{NI}{l} | LO6 |
| Magnetic flux density (T) | B = \mu \mu_r H | LO6 |
| Force on conductor (N) | F = BIL | LO6 |
| Force on charge (N) | F = qvB | LO6 |
| Torque on motor coil (Nm) | T = BINA | LO6 |
| Induced EMF — Faraday's Law | E = N \times \frac{\Delta \Phi}{\Delta t} | LO6 |
| Inductance of coil (H) | L = \frac{N^2 \mu A}{l} | LO6 |
| Energy in inductor (J) | E = \frac{1}{2} LI^2 | LO6 |
| Mutual inductance EMF (V) | E = M \times \frac{\Delta I}{\Delta t} | LO6 |