Applied Acoustics Systems Chromaphone 3 Upgrade Acoustic Object Synthesizer Plug-In (Download) User Manual

Page 38

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38

The Editor View

air which will propagate to our ears as sound waves.

Mathematically, a complex vibrational motion can be decomposed into elementary motion pat-

terns called the

normal modes

of the object. Under a normal mode, all the parts of the structure

move in phase and at the same frequency in a sinusoidal motion. In other words, this complex
motion results from the fact that objects naturally oscillate at many different frequencies at once,
each frequency being related to a normal mode of vibration. These frequencies are called

partials

;

the lowest partial is called the

fundamental

and the higher ones are referred to as

overtones

. When

relating to music, the fundamental corresponds to the

note

played and the overtones are called

harmonics

as in most musical instruments their frequency is a multiple integer (or almost) of the

fundamental.

As an example, the vibration motion associated with two normal modes of a rectangular plate is

illustrated in Figures 21 and 22. In the first figure, one can see the vibration motion associated with
two different normal modes of the plate (modes [1,1] and [3,2]). Over one period of oscillation,
all the points go up and down in phase. The principle remains the same for all mode, the motion
pattern only becoming more and more complex as the order of the mode increases. The full motion
of a plate, however complicated, will always correspond to a combination of all its normal modes.
Figure 22 is a top view of the plate and shows contour lines corresponding to the same normal
modes. A contour line groups points that oscillate with the same amplitude. In particular, the
straight lines in the second graph of this figure, corresponds to so-called

nodal lines

where the

amplitude of the motion is zero and therefore where the plate is still.

The relative frequencies or ratio of the frequency of the overtones to the fundamental frequency

is specific to the type of the object and its boundary conditions (whether its boundaries are free to
vibrate or are fixed). In other words this distribution of partials is characteristic of the type of object
and could be viewed as its tonal signature; it allows us to distinguish, for example, a vibrating
plate from a drumhead. The specific frequency of the partials, related to the sensation of pitch, is
determined by the dimensions of the object, for example a small plate will have a higher pitch than
an larger one.

Figure 21: Motion corresponding to normal mode [1,1] and [3,2] of a plate.

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