Reference efficiency.
Calculate one-sided reference efficiency and a stated-condition, mass-controlled sensitivity estimate. A nominal 1 W reference is not the power consumed by a real loudspeaker.
Driver parameters
Sensitivity conditions
Air & conventions
Optional driver overrides
Blank derives mass from fs, Vas, and Sd. A conflicting entered value is flagged.
Blank derives Bl from the moving mass, fs, Re, and Qes.
Read this result with its assumptions.
Efficiency counts one side radiating into an infinite-baffle half-space. A two-sided acoustic-power convention doubles that number.
Sensitivity: 2.830 V RMS, 1 m, ideal half-space, negligible inductance and source resistance.
Sensitivity uses Mms = 99.336 g and Bl = 11.894 T m, derived unless overridden.
Voltage sensitivity is not automatically 1 W sensitivity. Actual loudspeaker power is frequency-dependent.
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The math, in plain sight.
Efficiency is not the same as sensitivity.
One-sided reference efficiency
The convention here counts one side radiating into an ideal infinite-baffle half-space. A convention that counts both sides of an ideal infinite baffle gives twice the acoustic power.
Efficiency is a dimensionless fraction; multiply by 100 for percent. With fs = 30 Hz, Vas = 100 L, and Qes = 0.45, this convention gives approximately 0.59%.
Sensitivity under stated conditions
For a specified RMS voltage in a mass-controlled, approximately flat on-axis range, neglecting voice-coil inductance and source resistance:
The ideal free-space comparison uses 4 pi instead of 2 pi in the pressure denominator. Sensitivity is always labeled with voltage, distance, and radiation condition.
What nominal 1 W means
2.83 V RMS corresponds to 1 W into an 8 ohm resistive reference, not automatically 1 W into a real driver or a 4 ohm nominal load. Reference efficiency does not predict maximum output or thermal compression.