A — Line Maintenance (Aeroplane Turbine)Module 3 · 20 practice questions

Module 3: Electrical Fundamentals

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Semiconductors and Diodes Semiconductors and Diodes PN Junction Structure P-type (holes) majority carriers N-type (electrons) majority carriers depletion Anode (A) Cathode (K) Diode Symbols Standard: K A LED: K A Forward Bias (Conducts) P N V > 0.7V I (conventional current) Reverse Bias (Blocks) P N V < 0 No current flow Half-Wave Rectifier Circuit AC ~ D1 R_L Output: t V_out Input: Rectification Converts AC to pulsating DC. Only positive half-cycles pass. Key Properties • Forward voltage drop: ~0.7V (Si) • Forward voltage drop: ~0.3V (Ge) • Blocks current in reverse direction • Used for rectification in aircraft power supplies (e.g. 28V DC) Aircraft Application Diode bridges in generator control units (GCUs) rectify AC to DC.

Module 3: Electrical Fundamentals – Study Material

1. Module Overview

Module 3 of the EASA Part-66 syllabus provides the foundational knowledge of electrical theory required for aircraft maintenance certifying staff. This module covers the behaviour of DC and AC circuits, the characteristics of essential components (resistors, capacitors, inductors, transformers), and the principles of power generation and distribution within aircraft systems. A thorough understanding of these fundamentals is critical for safe troubleshooting, testing, and certification of electrical work on modern aeroplanes, which increasingly rely on complex electrical and electronic systems.

The module is structured to build from basic atomic theory and units of measurement, through DC circuit analysis, to the more complex concepts of AC theory, magnetism, and finally, the practical application of these principles in aircraft batteries and measurement instruments. The knowledge levels range from a general overview (Level 1) to a detailed theoretical understanding (Level 3) required for complex fault diagnosis and system analysis.


2. Key Concepts Explained in Detail

2.1 Basic Electrical Units and Ohm's Law

The foundation of all electrical work is the relationship between the fundamental units: Voltage (V), Current (I), and Resistance (R). These are defined by the International System of Units (SI).

  • Voltage (V): The electrical potential difference between two points. It is the "pressure" that pushes electrons through a circuit. Unit: Volt (V).
  • Current (I): The rate of flow of electric charge. It is the "flow" of electrons. Unit: Ampere (A).
  • Resistance (R): The opposition to the flow of current. It converts electrical energy into heat. Unit: Ohm (Ω).

Ohm's Law is the fundamental relationship governing these three quantities:

> V = I × R

This law is used to calculate any one of the three values if the other two are known. For example, a navigation light bulb rated at 28 V and drawing 2 A has a filament resistance of R = V / I = 28 V / 2 A = 14 Ω.

Electrical Power (P) is the rate at which electrical energy is converted into another form of energy (e.g., heat, light, or mechanical motion). It is calculated using:

> P = V × I

Using Ohm's Law, this formula can be rearranged to P = I² × R or P = V² / R. For instance, a 28 V DC motor drawing 10 A consumes P = 28 V × 10 A = 240 W of electrical power.

Basic Electrical Circuits Basic Electrical Circuits SERIES CIRCUIT 12 V R₁ 4 Ω R₂ 6 Ω Lamp Key Characteristics: • Current is the SAME through all components • Total resistance: R_total = R₁ + R₂ + ... • Total voltage: V_total = V₁ + V₂ + ... Ohm's Law Application: R_total = R₁ + R₂ = 4 Ω + 6 Ω = 10 Ω I = V / R_total = 12 V / 10 Ω = 1.2 A V₁ = I × R₁ = 1.2 A × 4 Ω = 4.8 V V₂ = I × R₂ = 1.2 A × 6 Ω = 7.2 V Check: V₁ + V₂ = 4.8 V + 7.2 V = 12 V ✓ PARALLEL CIRCUIT 12 V R₁ 4 Ω R₂ 6 Ω Lamp Key Characteristics: • Voltage is the SAME across all branches • Total current: I_total = I₁ + I₂ + ... • Total resistance: 1/R_total = 1/R₁ + 1/R₂ + ... Ohm's Law Application: 1/R_total = 1/4 + 1/6 = 3/12 + 2/12 = 5/12 R_total = 12/5 = 2.4 Ω I₁ = V / R₁ = 12 V / 4 Ω = 3 A I₂ = V / R₂ = 12 V / 6 Ω = 2 A I_total = 3 A + 2 A = 5 A; V = I × R = 5 A × 2.4 Ω = 12 V ✓ Series: I constant Parallel: V constant

2.2 DC Circuits and Circuit Protection

A Direct Current (DC) circuit is one where current flows in a single, constant direction. Aircraft systems commonly use 28 V DC for many services, supplied by batteries and generator-driven rectifiers.

  • Series Circuits: Components are connected end-to-end, forming a single path for current. The current is the same through all components. The total resistance is the sum of individual resistances (R_total = R1 + R2 + ...). The total voltage is the sum of the voltage drops across each component (V_total = V1 + V2 + ...).
  • Parallel Circuits: Components are connected across the same two points, providing multiple paths for current. The voltage is the same across all components. The total current is the sum of the currents through each branch (I_total = I1 + I2 + ...). The total resistance is calculated using the reciprocal formula: 1/R_total = 1/R1 + 1/R2 + ...

Circuit Protection: A short circuit occurs when a live conductor makes direct contact with the return path (e.g., the aircraft structure/ground), bypassing the intended load. This creates a path of almost zero resistance, causing a dangerously high current to flow. This can lead to overheating, fire, and damage to wiring and components. Protective devices like fuses and circuit breakers are designed to detect this excessive current and interrupt the circuit. A chafed wire touching the airframe is a classic example of a short circuit.

Voltage Drop: In a practical circuit, the wiring itself has resistance. When current flows, a voltage drop (V = I × R) occurs across this resistance. If connections are poor or wiring is undersized, the resistance increases, leading to an excessive voltage drop. This results in a lower-than-expected voltage at the load. For example, a dim cockpit light measuring 20 V instead of 28 V is a classic symptom of high resistance in the supply wiring or a poor connection.

2.3 Capacitance and Capacitors

A capacitor is a passive component that stores electrical energy in an electric field. It consists of two conductive plates separated by an insulating material called a dielectric. Its ability to store charge is called capacitance (C), measured in Farads (F). Aircraft systems commonly use capacitors in microfarads (µF) or picofarads (pF).

  • Capacitors in Parallel: The total capacitance is the sum of the individual capacitances.

> C_total = C1 + C2 + C3 + ...

For example, a 20 µF and a 30 µF capacitor in parallel yield a total of 50 µF.

  • Capacitors in Series: The total capacitance is less than the smallest individual capacitance. The reciprocal of the total is the sum of the reciprocals of the individual capacitances.

> 1/C_total = 1/C1 + 1/C2 + ...

Capacitive Reactance (Xc): In an AC circuit, a capacitor offers opposition to the flow of current, known as capacitive reactance. This opposition is frequency-dependent and is calculated using:

> Xc = 1 / (2πfC)

Where:

  • Xc is the capacitive reactance in Ohms (Ω)
  • f is the frequency in Hertz (Hz)
  • C is the capacitance in Farads (F)

For a 50 µF capacitor connected to a 115 V, 400 Hz supply, the reactance is:

Xc = 1 / (2 × π × 400 Hz × 50 × 10⁻⁶ F) ≈ 7.96 Ω.

2.4 AC Circuits and Power

Alternating Current (AC) is an electric current that periodically reverses direction. Aircraft AC systems typically operate at 115 V (phase-to-neutral) and 400 Hz. The higher frequency allows for smaller and lighter transformers and motors.

Three-Phase Systems: Aircraft often use three-phase AC power for heavy loads like pumps and generators. In a balanced star (wye) connection, the relationship between the phase voltage (V_ph, measured between a phase and neutral) and the line voltage (V_L, measured between any two phases) is:

> V_L = √3 × V_ph

For a system with a 115 V phase voltage, the line-to-line voltage is V_L = 1.732 × 115 V ≈ 199.2 V.

Power in AC Circuits: In AC circuits, the voltage and current may not be in phase. The phase difference is denoted by the angle φ (phi). This leads to three types of power:

  • True Power (P): The actual power consumed by the circuit to do work (e.g., produce heat, light, or motion). Measured in Watts (W). P = V × I × cos(φ).
  • Apparent Power (S): The product of the RMS voltage and current. It represents the total power drawn from the source. Measured in Volt-Amperes (VA). S = V × I.
  • Reactive Power (Q): The power that oscillates between the source and the reactive components (inductors and capacitors) without doing work. Measured in Volt-Amperes Reactive (VAR). Q = V × I × sin(φ).

The relationship between these three types of power is described by the Power Triangle:

> S² = P² + Q²

The Power Factor (PF) is the ratio of true power to apparent power: PF = P / S = cos(φ). A purely resistive circuit has a PF of 1 (φ = 0°). An inductive circuit has a lagging PF (current lags voltage), while a capacitive circuit has a leading PF (current leads voltage).

For example, if a circuit has a phase angle of 60° and a true power of 500 W, the apparent power is S = P / cos(φ) = 500 W / 0.5 = 1000 VA. Similarly, if the apparent power is 200 VA and the true power is 173.2 W, the reactive power is Q = √(S² - P²) = √(200² - 173.2²) ≈ 100 VAR.

2.5 Transformers

A transformer is a static device that transfers electrical energy between two or more circuits through electromagnetic induction. It consists of a primary winding and a secondary winding wound around a common magnetic core. Transformers can only operate on AC.

The relationship between the voltages and the number of turns in the primary (Np) and secondary (Ns) windings is:

> V_s / V_p = N_s / N_p

This is known as the turns ratio. A transformer with more turns on the secondary than the primary is a step-up transformer (increases voltage). A transformer with fewer turns on the secondary is a step-down transformer (decreases voltage).

For example, a transformer with 200 turns on the primary and 400 turns on the secondary, connected to a 115 V supply, will produce a secondary voltage of:

V_s = V_p × (N_s / N_p) = 115 V × (400 / 200) = 230 V.

Conversely, a transformer with 1000 turns on the primary and 250 turns on the secondary will step down the voltage to V_s = 115 V × (250 / 1000) = 28.75 V.

2.6 Batteries and Internal Resistance

Aircraft batteries, typically 24 V lead-acid types, are critical for starting engines and providing backup power. A battery is not a perfect voltage source; it has an internal resistance (r) due to the resistance of the electrolyte and plates.

  • Discharging: The terminal voltage (V) is lower than the battery's EMF (electromotive force, E) due to the voltage drop across the internal resistance.

> V = E - (I × r)

  • Charging: The terminal voltage is higher than the EMF because the charger must overcome the internal resistance.

> V = E + (I × r)

For example, a 24 V battery with an internal resistance of 0.05 Ω being charged with 10 A will have a terminal voltage of V = 24 V + (10 A × 0.05 Ω) = 24.5 V.

Battery Condition: A fully charged 24 V lead-acid battery has an open-circuit (no load) terminal voltage of approximately 25.2 to 27.6 V. This is due to the electrochemical potential of the cells (about 2.1–2.3 V per cell). A reading of 27.5 V with the generator off indicates a fully charged battery, not a fault.

2.7 Temperature Coefficient of Resistance

The resistance of a conductor changes with temperature. For most metals (like copper), resistance increases as temperature increases. This is quantified by the temperature coefficient of resistance (α).

The resistance at a new temperature (R_t) can be calculated using:

> R_t = R_0 [1 + α (t - t_0)]

Where:

  • R_0 is the resistance at the reference temperature (t_0), typically 20 °C.
  • α is the temperature coefficient of resistance (per °C).
  • t is the new temperature.

For example, a sensor coil with a resistance of 120 Ω at 20 °C, made of copper (α = 0.004/°C), will have a resistance of R_t = 120 Ω × [1 + 0.004 × (30 °C - 20 °C)] = 120 Ω × 1.04 = 124.8 Ω at 30 °C.

2.8 Electrical Measurement and Instruments

Accurate measurement is essential for troubleshooting. The correct use of a Digital Multimeter (DMM) is a key skill.

  • Measuring Voltage: A voltmeter is connected in parallel with the component or supply. This is because it must measure the potential difference across the two points without significantly affecting the circuit. A DMM in voltage mode has a very high internal resistance.
  • Measuring Current: An ammeter is connected in series with the load. This forces all the current in the circuit to flow through the meter. A DMM in current mode has a very low internal resistance. Connecting an ammeter in parallel creates a short circuit, potentially damaging the meter and the circuit.
  • Measuring Resistance: An ohmmeter is connected in parallel with the component, but only when the circuit is de-energised (power off). The meter applies a small current and measures the resulting voltage to calculate resistance.
  • Measuring Frequency: A DMM can measure frequency by connecting it in parallel with the AC supply, just like a voltage measurement. This is a common task when verifying 400 Hz power quality.

3. Important Formulas and Regulations

3.1 Key Formulas Summary

QuantityFormulaUnits
Ohm's LawV = I × RV, A, Ω
Electrical Power (DC)P = V × IW
Electrical Power (AC)P = V × I × cos(φ)W
Apparent PowerS = V × IVA
Reactive PowerQ = V × I × sin(φ)VAR
Power TriangleS² = P² + Q²VA, W, VAR
Capacitors in ParallelC_total = C1 + C2 + ...F
Capacitors in Series1/C_total = 1/C1 + 1/C2 + ...F
Capacitive ReactanceXc = 1 / (2πfC)Ω
Transformer Turns RatioV_s / V_p = N_s / N_pV, turns
Three-Phase (Star)V_L = √3 × V_phV
Battery Terminal Voltage (Charging)V = E + (I × r)V
Battery Terminal Voltage (Discharging)V = E - (I × r)V
Temperature CoefficientR_t = R_0 [1 + α (t - t_0)]Ω

3.2 Regulatory References

This study material is aligned with the requirements of:

  • Regulation (EU) No 1321/2014, Annex III (Part-66): This regulation establishes the licensing requirements for aircraft maintenance certifying staff.
  • Part-66 Appendix I: This appendix details the basic knowledge syllabus for the aircraft maintenance licence. The specific modules referenced in this material are:
  • Module 3.2: Resistance/Resistor
  • Module 3.3: Electrical Units
  • Module 3.4: Ohm's Law
  • Module 3.5: Electrical Power
  • Module 3.8: Batteries
  • Module 3.9: DC Sources
  • Module 3.11: Capacitance/Capacitors
  • Module 3.12: Alternating Current
  • Module 3.13: AC Circuits
  • Module 3.14: Transformers
  • Module 3.15: AC Motors/Generators
  • Module 3.16: Electrical Measuring Instruments
  • Module 3.17: Wiring Practices

4. Common Relationships Between Concepts

  • Ohm's Law and Power: The power formula (P = V × I) is intrinsically linked to Ohm's Law. By substituting V = I × R, you get P = I² × R. By substituting I = V / R, you get P = V² / R. This allows power to be calculated if any two of the three base quantities are known.
  • Reactance and Frequency: Capacitive reactance (Xc) is inversely proportional to frequency. As frequency increases, Xc decreases. This is why capacitors are used in filtering circuits to block low-frequency signals and pass high-frequency signals.
  • AC Power and Phase Angle: The power factor (cos φ) is the bridge between true, apparent, and reactive power. A purely resistive load has a PF of 1, meaning all power is true power. Inductive loads (motors, ballasts) have a lagging PF, while capacitive loads have a leading PF. Understanding this is crucial for sizing generators and analysing power quality.
  • Transformer Action and Turns Ratio: The turns ratio directly dictates the voltage transformation. A step-down transformer (N_s < N_p) reduces voltage and increases current (to maintain power balance, ignoring losses). A step-up transformer (N_s > N_p) increases voltage and decreases current.
  • Internal Resistance and Battery State: The internal resistance of a battery causes the terminal voltage to sag under load and rise during charging. This is why a battery's voltage cannot be accurately assessed while it is under a heavy load or being charged.

5. Typical Exam Focus Points

Based on the syllabus and typical exam questions, candidates should focus on the following areas:

  • Calculations: Be proficient in applying Ohm's Law (V = IR) and the power formulas (P = VI, P = I²R, P = V²/R) to solve for unknown quantities.
  • Series and Parallel Circuits: Be able to calculate total resistance, current, and voltage for both series and parallel configurations.
  • Capacitors: Understand the difference between series and parallel connections and be able to calculate total capacitance. Be able to calculate capacitive reactance (Xc) at a given frequency.
  • AC Power: Understand the power triangle and be able to calculate true power, apparent power, reactive power, and power factor given a phase angle or other parameters.
  • Three-Phase Systems: Know the relationship between phase and line voltage in a star connection (V_L = √3 × V_ph).
  • Transformers: Be able to use the turns ratio to calculate primary or secondary voltages.
  • Batteries: Understand the concept of internal resistance and be able to calculate terminal voltage during charging and discharging.
  • Temperature Effects: Be able to calculate the change in resistance of a conductor due to temperature changes using the temperature coefficient of resistance.
  • Measurement Techniques: Know the correct way to connect a DMM for voltage (parallel), current (series), and resistance (parallel, power off) measurements.
  • Fault Diagnosis: Apply theoretical knowledge to practical scenarios, such as identifying the cause of a voltage drop (excessive resistance) or the effect of a short circuit (excessive current).

Practice this module

Reinforce Module 3: Electrical Fundamentals with 20 EASA-style practice questions, matched to your weak areas.