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148th ASA Meeting, San Diego, CA


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How to Pitch-Match Drumsticks - 10,000 Times a Day


George Bissinger bissingerg@mail.ecu.edu
Physics Department
East Carolina University
Greenville, NC 27858

Popular version of Paper 4aMU7
Presented Thursday morning, November 18, 2004
148th ASA Meeting
San Diego, CA

 

Theme: How to automate pitch-matching ten thousand drumsticks a day using modal (vibration) analysis techniques.

Sub-theme: a drumstick is a one-dimensional violin. We want to evolve procedures to evaluate and match violin top and back plate vibrational properties on assembly line violin production.


OUTLINE

Pitch is a quintessentially musical term not commonly applied to drumsticks. Yet it is considered a desirable attribute by drummers, enough to make such matching commercially viable. For the tidy harmonic series like those from string vibrations (where the frequencies fn = n x f1, and n is always an integer =1,2,3…) a well-defined pitch generally comes naturally. Although no well-defined sense of pitch is possible for drumsticks since their normal bending modes (which produce the sound we hear) are not harmonic - or even nearly so - there is still some sort of "pitch center" that allows one to achieve approximate matches by ear.

Listen here for a demonstration of drumstick pitching

On the practical side, pitch matching of drumsticks is commonly done by those unversed in any underlying psychoacoustics explanations. Choose one drumstick from a box and then pick out any other drumstick, strike both on a hard surface and listen for a match. This takes a few seconds for each stick match and there is no minimum number of sticks to try. One might expect minutes on average to make a match from a box of sticks that have not been pre-sorted by either weight or pitch. Such rates, however, mean that using individuals to match drumsticks by ear in manufacturing consumes far too much time to be compatible with the many thousands of drumsticks throughput per day in normal manufacture.

There is a sensible modern solution to this problem. Understand the vibrational behavior of the drumstick - this means understanding its dependence on density, stiffness and shape - so well that even when it is held that one can reliably predict the effects of holding. Our understanding of the modes of vibration was achieved through experimental modal analysis, a technique whereby the "atoms" of vibration - the normal modes - can be assembled into the "molecule" of mechanical vibration that results from being set into motion.

Over 100 hickory drumsticks, in all-wood and plastic-tip models, were weighed, examined for material defects, and vibration-analyzed to create a statistical database. This database was then analyzed to find the range of mode frequencies expected to set analysis frequency bands, compute frequency relationships between modes in any one drumstick, check the effect of material defects including knots, grain twists or kinks and on vibrational behaviors. The final conclusion was very simple - only the frequency of the very lowest mode of vibration was necessary to reliably pitch match drumsticks!

On the manufacturing line this knowledge was turned into a brief (~1 s) vibration measurement after the manufacture, analyzed in few milliseconds and the drumstick was then sorted into frequency "bins". (Weights of the drumsticks were determined separately.) The pitch (and weight) matched drumsticks can then be paired and sold. To date millions have been pitched using this procedure since the manufacturer initiated the process last year.

A little side note. The pitch and weight matching also guarantees that the drumsticks are stiffness-matched. This is due to the basic physics behind vibrating objects where if the density(mass), stiffness and shape properties of a material are known the vibration frequencies can be computed. So turning this around a little, if you know the shape, density, and vibration frequencies it is possible to get the stiffness properties.

Violin making tradition
Violin makers have been "pitching" violin top and back plates for centuries using tap tones. These tones are generated by holding the plate between thumb and forefinger at particular places and then striking with a fingertip or knuckle at particular points. The result is not like the well-defined pitch of the plucked string, a sequence of harmonics with all frequencies being some integer multiple of a lowest (fundamental) frequency. Rather it is a summation of all the ways that certain structures like a violin plate (and the violin itself) can vibrate at a certain frequency. These are what we refer to individually as the normal modes - the "atoms" of vibration.

Normal modes
As an analogy think of building a house. You don't just build a house, you assemble the building blocks of a house: concrete blocks, bricks, wall studs, sheet rock, etc. Your choice of building materials and your choice of how/where to assemble the building blocks determines the shape and character of the house. Similarly, to construct a "molecule" of vibration you must assemble its constituent atoms, the normal modes. Each normal mode is characterized by its:

a) frequency of vibration - the number of cycles per second

b) "damping" (our measure of how a vibrating object loses its energy - here part of the energy goes to heat (internal damping), part to sound (radiation damping) and part to whoever is holding the vibrating device (the "support fixture" damping in engineering terms). How many cycles of vibration the vibrator goes through before stopping is a measure of its damping. Damping greatly colors the perceived sound - think of a struck bell suspended by a string vs. being held with the hand.

c) "shape" - this is just a profile of its motion. Simplifying the shape is commonly done by drawing a line through just the points on the object where there is no motion (nodal points) to create a nodal line. For the violin, or a violin plate each nodal line pattern for any mode is completely distinct from every other one, both mathematically and by visual inspection.

To help understand what is meant by mode shape, we will go to a two-dimensional world. Consider what happens when you scatter a powder on a plate and force the plate to vibrate. If you get the plate to vibrate in one of its normal mode shapes the powder will be bounced to the nodal regions, highlighting the regions of no motion. This technique, called Chladni patterns, has been around for centuries. Some visualizations of violin plate motions are shown below.

a) Center graphic is a photo of glitter on a wooden violin top plate that was forced to vibrate at one of its normal mode frequencies by placing it over a loudspeaker and driving the loudspeaker with a sine wave set at the normal mode frequency. The dark glitter traces the nodal lines and serves to give a shape for the motional pattern.

b) Left graphic shows motional pattern presented as a number of little bars that either go up or down at various points over the whole surface. These are the actual measured velocities at each point on the surface. Note that sometimes the bars are above and sometimes below the plate surface. If you trace a line through the places where the plate has no motion again you get a nodal line pattern.

c) Right graphic shows a greatly magnified change/deformation in the plate shape as it goes through its vibratory motions.

These three graphics illustrate some of the ways of illustrating motion in a static presentation. The analysis software that takes the vibrations and turns them into these graphics also has animation capability.

When the plates are glued to the violin ribs the vibration patterns change significantly because the edges have some constraints that do not allow them to flex freely. Modal analysis allows us to visualize these vibration changes exactly like free plates.

Finally, the whole violin vibrations for one of its normal modes is shown below. All the yellow/white (fat line) parts do NOT radiate significant sound.


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