“…Input to the ME can then be quantified as the pressure incident on the TM, devoid of any standing-wave cancellations. This decomposition of total pressure is achieved by prior determination of the Thevenin-equivalent source impedance and pressure of the transducer ͑Sivian and White, 1933;Rabinowitz, 1981;Allen, 1986;Keefe et al, 1992;Neely and Gorga, 1998;Hudde et al, 1999;Farmer-Fedor and Rabbitt, 2002͒. Knowing the source impedance ͑Z s ͒ and pressure ͑P s ͒, the impedance of any unknown load ͑Z L ͒, whether the ear canal or another cavity, is defined as…”