Physiology Lab: Transfer Functions

This application is designed to help you understand how the outer and middle ear modify and transfer sound energy before cochlear stimulation.

1. Chart Overview

The graph displays simplified, frequency-dependent transfer functions in decibels (dB) relative to frequency (Hz) on a logarithmic scale from 200 Hz to 16,000 Hz.

The red curve should therefore be interpreted as a relative transfer function, not as a direct measurement of sound pressure inside the cochlea.

2. Interaction & Controls

You can manipulate the acoustic input using the control panel:

3. Reading the Results

As you adjust the sliders, the Results Card updates in real time:

This value is provided only as a teaching index. It should not be interpreted as a measured cochlear SPL, oval-window pressure, or clinically calibrated physiological quantity.

Basilar Membrane Tonotopic Map

Below the graph, a color-coded track represents the tonotopic organization of the cochlea.

The marker moves according to the selected frequency to illustrate approximately where that frequency is represented along the basilar membrane.

Scientific Notes for Students

Outer-ear resonance

Notice that the outer-ear transfer reaches its maximum in the region of approximately 2–4 kHz in this simplified model.

This reflects the frequency-dependent resonances of the pinna, concha, and ear canal and contributes to enhanced sensitivity in a frequency region that is important for speech perception.

Middle-ear transfer

The middle ear does not simply amplify sound by a fixed number of decibels.

Its transfer characteristics vary with frequency because of the combined effects of mass, stiffness, damping, tympanic-membrane mechanics, ossicular coupling, and impedance transformation between air and cochlear fluids.

Model limitations

This application uses simplified log-Gaussian functions to illustrate the general frequency dependence of outer- and middle-ear transfer.

The curves should therefore be interpreted as conceptual teaching models rather than precise physiological measurements.

The combined curve is formed by adding the modeled transfer terms in dB. It illustrates how their frequency-dependent effects may combine, but it does not represent a direct measurement of cochlear input.

Question for Students

How does the combined modeled transfer change as you move from the middle-ear transfer peak near 1.2 kHz toward the outer-ear transfer peak near 3 kHz?

Which of the two components contributes most to the combined response at each frequency?