🚧 Under construction — VoTechWorks is being built. A free tech program — complimentary, as our commitment to get America working.
voTechWorksGrade 13 · a vocational technology learning center, by urbanicity
newSchoolWorks.com › VoTechWorks › Building & Construction › Electrical › DC/AC Electrical Theory › Lesson 8
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:

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

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.
  1. Convert millihenries to henries: 150 mH = 0.150 H
  2. Write the formula: X_L = 2πfL
  3. Substitute values: X_L = 2 × 3.1416 × 60 × 0.150
  4. 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.
  1. From the previous example, X_L = 56.6 Ω
  2. Apply the impedance formula: Z = √(R² + X_L²) = √(47² + 56.6²)
  3. Calculate squares: 47² = 2209; 56.6² = 3203.6
  4. Add: 2209 + 3203.6 = 5412.6
  5. Take square root: Z = √5412.6 ≈ 73.6 Ω
  6. 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.
  1. Write the formula: X_L = 2πfL
  2. Substitute: X_L = 2 × 3.1416 × 400 × 0.150
  3. Multiply: 6.2832 × 400 = 2513.3; then 2513.3 × 0.150 = 376.99 Ω
  4. 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.
  1. Find current using Ohm's law for AC: I = V_source / Z = 12.0 / 73.6 ≈ 0.163 A
  2. Voltage across resistor: V_R = I × R = 0.163 × 47 ≈ 7.66 V
  3. Voltage across inductor: V_L = I × X_L = 0.163 × 56.6 ≈ 9.23 V
  4. 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
Brush up in the math halls at newSchoolWorks.com:
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.

NCCER Electrical — AC Theory
1. Which formula correctly calculates inductive reactance?
NCCER Electrical — AC Theory
2. A 200 mH inductor is connected to a 60 Hz source. What is its inductive reactance?
NCCER Electrical — AC Theory
3. In a pure inductor connected to an AC source, the relationship between voltage and current is best described as:
NCCER Electrical — AC Theory
4. A series RL circuit has R = 30 Ω and X_L = 40 Ω. What is the impedance?
NCCER Electrical — AC Theory
5. You double the frequency applied to an inductor while keeping inductance and voltage constant. What happens to X_L?
NCCER Electrical — AC Theory
6. During the lab, you measure voltage across the resistor and voltage across the inductor, then add them. The sum is greater than the source voltage. Why?
NCCER Electrical — AC Theory
7. When using a dual-trace oscilloscope to observe phase lag, one probe is placed across the resistor. Why is the resistor chosen rather than the inductor?
OSHA 10 — Electrical Safety
8. Which of the following is the FIRST action a student should take before rewiring a breadboard circuit during a lab session?
Record this lesson on my transcript. Sign in with your key and enrollment email to record lessons (enroll free if you have no key). This page stays open to read and practise.