Skip to main content
\(\require{cancel}\)
Physics LibreTexts

9.2.1: Other Combination Tones

  • Page ID
    26229
  • The ear-brain system can be easily fooled in many ways giving rise to what are known collectively as phantom tones. The missing fundamental, described above, is one example of a phantom tone. As another example, under the right circumstances listeners will perceive a frequency which is the difference between two frequencies: \(f=f_{1}-f_{2}\), instead of the two individual frequencies. A similar effect can sometimes occur when the sum of two frequencies is heard instead of the two individual frequencies: \(f=f_{1}+f_{2}\). Since most musical instruments have harmonics and overtones, these combination tones (sometimes called Tartini tones) can have an effect on the timbre of a musical note, both for an individual instrument and for two or more instruments playing together.

    The phenomenon of beats, discussed previously, occurs when two notes are close together in frequencies and we perceive one note which varies in loudness. A guitar string can be tuned by comparing a note with a known pitch and tuning the string until the beats disappear. What happens if the two frequencies get further and further apart? If the notes are a little further apart we still hear a single note but it sounds rough or wavering. Eventually we hear two separate notes instead of beats. The range of frequencies where the two frequencies are close enough to cause us to hear a single sound is called a critical band. Notice this is not the same thing as just noticeable difference in frequency. We may still be able to tell one note from another if they played one after the other but when played at the same time our hearing mechanism combines them into a single note.

    The following diagram shows the phenomena of critical bands. For a given frequency \(f_{1}\) a second frequency is played at the same time but its frequency is changed to be first below and then above the frequency \(f_{1}\).

    Figure \(\PageIndex{1}\)

    The critical band width is different at different chosen frequencies, \(f_{1}\). It is about \(100\text{ Hz}\) for frequencies below \(1000\text{ Hz}\) and then steadily increases to about \(3000\text{ Hz}\) at \(10,000\text{ Hz}\). If you start with a frequency, \(f_{1}\), of \(10,000\text{ Hz}\) you will hear beats if a second frequency is introduced that is between \(7,000\text{ Hz}\) and \(13,000\text{ Hz}\). But if you start with a frequency, \(f_{1}\), at \(800\text{ Hz}\) you will only hear beats if the second frequency is between 700 Hz and 900 Hz.

    The critical band also determines how well a tone is masked by noise (a random spread of frequencies). If there is one (or several) background frequencies (noise) but the frequency you are tying to hear is outside the critical band surrounding the noise then it is less difficult to hear the signal. If the signal frequency falls in the critical band, however, it is more difficult to perceive. Effectively this is because the ear mechanisms are already responding to that range of frequencies and the signal doesn't cause additional changes to the hearing system.

    Dissonance is the musical term that is used to describe musical notes that have harmonics close enough to fall in the roughness regime but not close enough to form beats. When two notes are played on a piano an octave apart (the second note has a fundamental exactly twice the fundamental of the first or a \(1\) to \(2\) ratio) all of the harmonics line up and fall on top of each other and there is no dissonance. (For example a \(200\text{ Hz}\) fundamental has harmonics at \(400\text{ Hz}, 600\text{ Hz}, 800\text{ Hz}\), etc. and the note an octave above has frequencies at \(400\text{ Hz}, 800\text{ Hz}\), etc.). However, when a perfect fifth is played (the fundamentals have a \(2\) to \(3\) ratio) the harmonics do not exactly line up. The match of harmonics is worse for harmonics of a minor third (ratio of \(4\) to \(5\)) and progressively worse for a perfect fourth (\(3\) to \(4\) ratio) and minor seventh (\(9\) to \(16\) ratio). If the harmonics fall close enough together there may be beating or roughness which changes the timbre of the combination. This is the primary reason a minor seventh chord does not sound as pleasant to the ears as an octave chord or a perfect fifth; the harmonics produce more roughness in the minor seventh case. The effect is stronger when the harmonics of the instrument are stronger and weaker for instruments with fewer or weaker harmonics.

    A more subtle from of beats, called waveform beats, can occur for a slight difference between two frequencies about an octave apart (one frequency is twice the other). So for example, a \(201\text{ Hz}\) sound and a \(400\text{ Hz}\) sound together will have a \(2\text{ Hz}\) oscillation in volume. This is because the octave above \(201\text{ Hz}\) would have a \(402\text{ Hz}\) frequency which is \(2\text{ Hz}\) from the \(400\text{ Hz}\) signal. Interestingly, a \(200\text{ Hz}\) plus a \(401\text{ Hz}\) signal is heard with a beat frequency of \(1\text{ Hz}\) because the octave above \(200\text{ Hz}\) is \(400\text{ Hz}\) which is only \(1\text{ Hz}\) difference from \(401\text{ Hz}\). The difference between the two cases has to do with the actual shape of the waveform and indicates that our ear-brain system does detect some information about the shape of the wave being heard, in addition to the frequencies (and is best explained by the place theory of hearing). This phenomena can have a slight effect on the timbre of a musical note.

    • Was this article helpful?