BLD-ELEC05-02 · Lesson 8 · 24 clock hours · lab
Inductance, Inductive Reactance, and RL Circuits
Objective. Students will calculate inductive reactance (XL = 2πfL) for a given inductor at two frequencies, measure the resulting impedance with a meter, and explain why voltage leads current by 90° in a pure inductor.
What Is Inductance?
An inductor is a coil of wire that stores energy in a magnetic field when current flows through it. The property that describes how strongly a coil opposes a change in current is called inductance, symbol L, measured in henries (H). A larger coil with more turns and an iron core has higher inductance than a small air-core coil with few turns.
In a DC circuit, an inductor acts like a short piece of wire once current is steady — its only opposition is the small DC resistance of the wire itself. In an AC circuit, everything changes, because AC is constantly reversing, meaning the current is always changing. That changing current constantly collapses and rebuilds the magnetic field, and that changing field induces a voltage that opposes the change. This opposition is called inductive reactance.
Inductive Reactance (X_L)
Inductive reactance is the AC opposition an inductor presents to current flow. It is measured in ohms (Ω), just like resistance, but it behaves differently — no heat is produced by pure reactance. The formula is:
> X_L = 2πfL
Where:
- X_L = inductive reactance in ohms (Ω)
- π ≈ 3.1416
- f = frequency in hertz (Hz)
- L = inductance in henries (H)
Two important conclusions follow directly from this formula:
1. Higher frequency → higher X_L. The current changes faster, so the inductor fights back harder.
2. Larger inductance → higher X_L. More magnetic flux linkage means more opposition.
At the US power-line frequency of 60 Hz, a 100 mH (0.1 H) inductor has X_L = 2π × 60 × 0.1 ≈ 37.7 Ω.
Why Voltage Leads Current by 90°
In a pure inductor, the induced voltage is greatest when the current is changing most rapidly (at the zero crossing), and the induced voltage is zero when the current is at its peak (not changing at that instant). This timing relationship means the voltage waveform reaches its peak one-quarter cycle (90°) before the current waveform. Put another way, current lags voltage by 90° in a pure inductor.
A useful memory aid: ELI — in an inductive (L) circuit, Voltage (E) comes before Current (I).
RL Series Circuits and Impedance
When a resistor and an inductor are connected in series, the total opposition to AC current is called impedance, symbol Z, also in ohms. You cannot simply add R and X_L the way you add two resistances, because they are 90° out of phase with each other. Instead, use the Pythagorean theorem:
> Z = √(R² + X_L²)
The phase angle θ between voltage and current in the RL circuit is:
> θ = arctan(X_L / R)
In a purely resistive circuit θ = 0°; in a purely inductive circuit θ = 90°. A real RL circuit falls somewhere between those extremes.
Reading Your Measurements
In the lab you will use a true-RMS DMM to measure AC voltages. A true-RMS meter correctly reads the effective value of any AC waveform — this is important because standard average-responding meters are calibrated for a perfect sine wave and can read low on distorted signals from function generators.
You will also use a dual-trace oscilloscope to see both the source voltage and the resistor voltage at the same time. The resistor voltage is in phase with the current (Ohm's law — V_R = I × R, no phase shift). By comparing the resistor trace to the source trace you can directly observe how much the current lags the source voltage.
Lab Safety
- Bench transformer and function generator outputs in this lab are low-voltage AC. Even so, treat every energized conductor as a shock hazard. Do not reach into a live circuit.
- Build and check your circuit with power OFF. Have your instructor verify the wiring before you apply power.
- Lockout/tagout awareness: Although bench supplies have simple on/off switches, the professional habit of de-energizing before working on a circuit must be practiced every time — it is the foundation of LOTO procedures you will use on the job under OSHA standards.
- Oscilloscope probes: Keep probe ground clips connected to the same reference point to avoid creating a short circuit through the scope's chassis ground.
- Inspect components: Check for cracked or burned inductors and resistors before use. Do not use damaged components.
- Wear safety glasses in the lab at all times.
Connecting Theory to Your Credentials
NCCER Electrical Levels 1 and 2 cover AC theory and the math behind inductive circuits — material that appears on NCCER written assessments. Understanding impedance also prepares you for motor and transformer topics in Levels 3 and 4. Your state journeyman exam will expect you to analyze AC circuits correctly. OSHA 10 training reinforces the safe work habits practiced in every lab session.
Key terms8
Inductance (L)The property of a coil that opposes any change in current by storing energy in a magnetic field; measured in henries (H).
Inductive Reactance (X_L)The AC opposition of an inductor to current flow, measured in ohms; calculated as X_L = 2πfL. Increases with both frequency and inductance.
Impedance (Z)The total opposition to AC current in a circuit containing both resistance and reactance; measured in ohms and calculated as Z = √(R² + X_L²) for a series RL circuit.
Phase Angle (θ)The angular difference in degrees between the voltage and current waveforms in an AC circuit; for a series RL circuit, θ = arctan(X_L / R).
True-RMS DMMA digital multimeter that accurately measures the effective (root-mean-square) value of any AC waveform, not just a pure sine wave.
ELIA memory aid meaning that in an inductive (L) circuit, Voltage (E) leads Current (I) — equivalently, current lags voltage.
Dual-Trace OscilloscopeA test instrument that displays two voltage waveforms simultaneously on screen, allowing phase differences between signals to be observed directly.
Hertz (Hz)The SI unit of frequency; one hertz equals one complete AC cycle per second. US power line frequency is 60 Hz.
Worked examples4
1. Calculate the inductive reactance of a 150 mH inductor at 60 Hz.
- Convert millihenries to henries: 150 mH = 0.150 H
- Write the formula: X_L = 2πfL
- Substitute values: X_L = 2 × 3.1416 × 60 × 0.150
- Multiply: 2 × 3.1416 = 6.2832; then 6.2832 × 60 = 376.99; then 376.99 × 0.150 = 56.55 Ω
Answer: X_L ≈ 56.6 Ω at 60 Hz
2. A series RL circuit has R = 47 Ω and L = 150 mH at 60 Hz. Calculate the impedance Z and the phase angle θ.
- From the previous example, X_L = 56.6 Ω
- Apply the impedance formula: Z = √(R² + X_L²) = √(47² + 56.6²)
- Calculate squares: 47² = 2209; 56.6² = 3203.6
- Add: 2209 + 3203.6 = 5412.6
- Take square root: Z = √5412.6 ≈ 73.6 Ω
- Calculate phase angle: θ = arctan(X_L / R) = arctan(56.6 / 47) = arctan(1.2043) ≈ 50.3°
Answer: Z ≈ 73.6 Ω; θ ≈ 50.3° (current lags voltage by 50.3°)
3. The same 150 mH inductor is now driven at 400 Hz (common in aircraft and some industrial systems). Calculate X_L at 400 Hz and compare it to the 60 Hz value.
- Write the formula: X_L = 2πfL
- Substitute: X_L = 2 × 3.1416 × 400 × 0.150
- Multiply: 6.2832 × 400 = 2513.3; then 2513.3 × 0.150 = 376.99 Ω
- Compare: at 60 Hz X_L ≈ 56.6 Ω; at 400 Hz X_L ≈ 377 Ω — about 6.67 times higher, matching the frequency ratio (400/60 ≈ 6.67)
Answer: X_L ≈ 377 Ω at 400 Hz — nearly 6.7× higher than at 60 Hz, confirming that X_L is directly proportional to frequency.
4. In the 60 Hz RL lab circuit (R = 47 Ω, Z ≈ 73.6 Ω), the source voltage is measured at 12.0 V RMS. Calculate the expected circuit current and the voltage drop across R and across L.
- Find current using Ohm's law for AC: I = V_source / Z = 12.0 / 73.6 ≈ 0.163 A
- Voltage across resistor: V_R = I × R = 0.163 × 47 ≈ 7.66 V
- Voltage across inductor: V_L = I × X_L = 0.163 × 56.6 ≈ 9.23 V
- Verify using phasor addition (not arithmetic addition): V_source = √(V_R² + V_L²) = √(7.66² + 9.23²) = √(58.7 + 85.2) = √143.9 ≈ 12.0 V ✓
Answer: I ≈ 0.163 A; V_R ≈ 7.66 V; V_L ≈ 9.23 V. Note that V_R + V_L (7.66 + 9.23 = 16.89 V) does not equal V_source — phasor addition must be used, not simple arithmetic addition.
The math in this lesson2
Learners compute X_L = 2πfL, RL impedance and phase angle, and current and voltage drops at 12 V RMS.
A-SSE.1G-SRT.8
In class: Worked-example lecture: instructor solves XL and total impedance for three RL series circuits at 60 Hz, then students solve three similar problems independently. · Lab measurement: students build an RL series circuit using a known inductor value, apply 60 Hz AC from a bench transformer, measure voltage across R and across L with a true-RMS DMM, and calculate impedance; they repeat at a second frequency using the function generator. · Phase-lag demonstration: using the dual-trace oscilloscope, students connect one probe across the resistor (proportional to current) and one across the source; they sketch both waveforms, label phase difference, and confirm current lags voltage in the lab log.
Materials: Known-value air-core inductors; resistors; AC bench power supply and/or function generator; dual-trace oscilloscope; true-RMS DMM; breadboard or terminal-strip trainer; lab log; NCCER Level 1 and Level 2 textbooks
Check: Calculated XL vs. measured impedance within ±10% (inductor tolerance is wider than resistor); phase-lag sketch present and labeled correctly; lab log signed by instructor. Students with errors >10% must repeat the measurement with instructor guidance.
Practice check8
Answer each question, then check it. Nothing is recorded; this is your own practice.
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