Editing Loudspeaker (section)

===Efficiency vs. sensitivity===
Loudspeaker efficiency is defined as the [[sound power]] output divided by the electrical power input. Most loudspeakers are inefficient transducers; only about 1% of the electrical energy sent by an amplifier to a typical home loudspeaker is converted to acoustic energy. The remainder is converted to heat, mostly in the voice coil and magnet assembly. The main reason for this is the difficulty of achieving proper [[impedance matching]] between the [[acoustic impedance]] of the drive unit and the air it radiates into.{{efn|At low frequencies, improving this match is the main purpose of speaker enclosure designs.}} The efficiency of loudspeaker drivers varies with frequency as well. For instance, the output of a woofer driver decreases as the input frequency decreases because of the increasingly poor impedance match between air and the driver.

Driver ratings based on the SPL for a given input are called ''sensitivity ratings'' and are notionally similar to efficiency. Sensitivity is usually expressed as the SPL (''dB<sub>SPL</sub>'' by common usage meaning ''dB relative to {{val|20|ul=μPa}}'') at 1&nbsp;W electrical input, measured at 1 meter,{{efn|A different measurement technique{{specify|date=July 2024}} is used for headphones.}} often at a single frequency. The voltage used is often 2.83&nbsp;V<sub>RMS</sub>, which results in 1&nbsp;watt into a nominal 8&nbsp;Ω speaker impedance. Measurements taken with this reference are typically quoted as dB<sub>SPL</sub> with 2.83&nbsp;V @ 1&nbsp;m.{{Citation needed|date=August 2024}}

The sound pressure output is measured at (or mathematically scaled to be equivalent to a measurement taken at) one meter from the loudspeaker and on-axis (directly in front of it), under the condition that the loudspeaker is radiating into an infinitely large space and mounted on an [[infinite baffle]]. Clearly then, sensitivity does not correlate precisely with efficiency, as it also depends on the directivity of the driver being tested and the acoustic environment in front of the actual loudspeaker. For example, a cheerleader's horn produces more sound output in the direction it is pointed by concentrating sound waves from the cheerleader in one direction, thus ''focusing'' them. The horn also improves impedance matching between the voice and the air, which produces more acoustic power for a given speaker power. In some cases, improved impedance matching (via careful enclosure design) lets the speaker produce more acoustic power.

Typical home loudspeakers have sensitivities of about 85 to 95&nbsp;dB<sub>SPL</sub> for 1&nbsp;W @ 1&nbsp;m—an efficiency of 0.5–4%. Sound reinforcement and public address loudspeakers have sensitivities of perhaps 95 to 102&nbsp; dB<sub>SPL</sub> for 1&nbsp;W @ 1&nbsp;m—an efficiency of 4–10%. Rock concert, stadium PA, marine hailing, etc. speakers generally have higher sensitivities of 103 to 110&nbsp; dB<sub>SPL</sub> for 1&nbsp;W @ 1&nbsp;m—an efficiency of 10–20%.{{Citation needed|date=July 2024}}

Since sensitivity and power handling are largely independent properties, a driver with a higher maximum power rating cannot necessarily be driven to louder levels than a lower-rated one. In the example that follows, assume (for simplicity) that the drivers being compared have the same electrical impedance, are operated at the same frequency within both driver's respective passbands, and that power compression and distortion are insignificant. A speaker 3&nbsp;dB more sensitive than another produces very nearly double the sound power (is 3&nbsp;dB louder) for the same electrical power input. Thus, a 100&nbsp;W driver (A) rated at 92&nbsp; dB<sub>SPL</sub> for 1&nbsp;W&nbsp;@ 1&nbsp;m sensitivity puts out twice as much acoustic power as a 200&nbsp;W driver (B) rated at 89&nbsp; dB<sub>SPL</sub> for 1&nbsp;W&nbsp;@ 1&nbsp;m when both are driven with 100&nbsp;W of electrical power. In this example, when driven at 100&nbsp;W, speaker A produces the same SPL, or [[loudness]] as speaker B would produce with 200&nbsp;W input. Thus, a 3&nbsp;dB increase in the sensitivity of the speaker means that it needs half the amplifier power to achieve a given SPL. This translates into a smaller, less complex power amplifier—and often, to reduced overall system cost.

{{Anchor|Hofmann}}<!--"Hofmann's Iron Law" redirects here.-->
It is typically not possible to combine high efficiency (especially at low frequencies) with compact enclosure size and adequate low-frequency response. One can, for the most part, choose only two of the three parameters when designing a speaker system. So, for example, if extended low-frequency performance and small box size are important, one must accept low efficiency. This [[rule of thumb]] is sometimes called '''Hofmann's Iron Law''' (after [[J. Anton Hofmann|J.A. Hofmann]], the H in [[KLH (company)|KLH]]).<ref>{{Cite web |url=http://ldsg.snippets.org/appdx-a.php |archive-url=https://web.archive.org/web/20080305171316/http://ldsg.snippets.org/appdx-a.php |title=Hofmann's Iron Law |archive-date=March 5, 2008 }}</ref><ref>{{cite web |url=http://www.salksound.com/wp/?p=56 |title=Sensitivity and Hoffman's Iron Law, or 'Why You Can't Have Hour Cake and Eat It Too' – Audioblog |website=SalkSound.com |access-date=April 14, 2018 }}</ref>