Joe Wolfe Created 2026-10-13 Updated 2026-10-18
John William Strutt, 3rd Baron Rayleigh Created 2026-10-18 Updated 2026-10-24
A physicist whose research joined waves, optics, acoustics and precise measurement. He maintained a laboratory at Terling and served as Cavendish professor of experimental physics from 1879 to 1884. At Cambridge he developed laboratory courses; later he donated his Nobel award proceeds toward a Cavendish laboratory extension.[ref]
The Rayleigh-Ramsay argon density experiment, pursued with William Ramsay, connects a small discrepancy in gas weighing to chemical separation. Its lesson is practical: agreement within one preparation method does not ensure that a second method produces the same chemical substance. The gas density model explains how composition and filling conditions both affect the readout.
Milan Červenka 2026-10-18
A physicist whose research includes nonlinear and computational acoustics and who teaches in the physics department at the Czech Technical University in Prague.[ref]
Model the room's decaying acoustic waves as a weakly damped resonator. The quality factor from ringdown is related to stored energy by
where is the pressure wave amplitude and . The measured frequency gives . If the stated is interpreted as an approximate wave amplitude exponential relaxation time,
an estimate of order . Taking as an energy exponential relaxation time instead gives .
There is a real convention ambiguity: “heard to die away” gives neither an initial sound level nor an audibility threshold, so it does not determine either exponential relaxation time. More generally, if the energy falls by a factor in ,
In room acoustics, a reverberation time usually denotes a decibel drop of , or an energy factor . If means , the corresponding estimate is instead . The simple decay-time estimate and the conventional reverberation time estimate should not be silently equated.