A method to transform the impedance measured in the ear canal, Z EC , to the plane of the eardrum, Z ED , is described. The portion of the canal between the probe and eardrum was modeled as a concatenated series of conical segments, allowing for spatial variations in its cross-sectional area. A model of the middle ear (ME) and cochlea terminated the ear-canal model, which permitted estimation of ME efficiency. Acoustic measurements of Z EC were made at two probe locations in 15 normal-hearing subjects. Z EC was sensitive to measurement location, especially near frequencies of canal resonances and anti-resonances. Transforming Z EC to Z ED reduced the influence of the canal, decreasing insertion-depth sensitivity of Z ED between 1 and 12 kHz compared to Z EC . Absorbance, A, was less sensitive to probe placement than Z EC , but more sensitive than Z ED above 5 kHz. Z ED and A were similarly insensitive to probe placement between 1 and 5 kHz. The probe-placement sensitivity of Z ED below 1 kHz was not reduced from that of either A or Z EC . ME efficiency had a bandpass shape with greatest efficiency between 1 and 4 kHz. Estimates of Z ED and ME efficiency could extend the diagnostic capability of wideband-acoustic immittance measurements.