Speaker Impedance Explained (2Ω, 4Ω, 8Ω, 16Ω)
Understand why loudspeaker impedance is not a fixed resistance number, how impedance curves change with frequency, and how load Ohms dictate amplifier wattage.
Mode 1: RMS Voltage + Impedance
P = V² / RCalculate continuous electrical or speaker wattage using known RMS Voltage and load resistance/impedance.
Voltage × Load Impedance Power Matrix
Click standard test voltages and speaker impedances (2Ω, 4Ω, 8Ω, 16Ω) to immediately retrieve real continuous wattage.
DC Resistance vs. AC Impedance ($Z$)
While simple DC resistance ($R$) is the fixed opposition to direct current flow, loudspeaker impedance ($Z$) is a complex, frequency-dependent quantity consisting of real resistance and reactive elements:
Where R_e is voice coil DC resistance, L_e is voice coil inductance causing impedance to rise at high frequencies, and Z_Mechanical creates a massive impedance peak at resonant frequency F_s.
Impedance Tier Comparison Matrix (2Ω vs 4Ω vs 8Ω vs 16Ω)
| Nominal Load | Typical DC Resistance (Re) | Current Draw @ 28.28V | Continuous Power Output | Primary Application |
|---|---|---|---|---|
| 2 Ω Load | 1.5 – 1.8 Ω | 14.14 Amperes | 400 Watts RMS | Car Audio Competition Subwoofers |
| 4 Ω Load | 3.1 – 3.6 Ω | 7.07 Amperes | 200 Watts RMS | Car Audio Coaxials & Pro PA Monitors |
| 8 Ω Load | 5.8 – 6.8 Ω | 3.54 Amperes | 100 Watts RMS | Home Hi-Fi, Studio Monitors & AVRs |
| 16 Ω Load | 11.5 – 13.5 Ω | 1.77 Amperes | 50 Watts RMS | Pro Compression Horns & Multi-Cab Stacks |