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Conical Fretboard Radiusing Jig

Conical Fretboard Radiusing Jig

by Mike Nealon

Originally published in American Lutherie #66, 2001



How flat does the top surface of a fretboard need to be? A good working estimate would be to equate the tolerance to the gap between the top of the 2nd fret and the bottom of a string fretted at the 1st fret. The tolerance must be less than this gap or the 2nd fret will come into contact with the string. With the bottom of the open string about .01" above the top of the 1st fret and about 1/16" from the top of the 20th fret, the gap between the fretted string and the top of the second fret is about .005".

Making a hardwood board flat to within .005" is not too difficult using ordinary woodworking tools. The router table and movable plate described here will produce a machine-carved surface smooth enough to require only a minimal amount of sanding or leveling.

Photo 1 shows the jig fully assembled, with the router. Photo 2 shows the jig partially disasembled to show the function of the parts. The conical fretboard made with this jig has a 10" radius at the nut, flattening to a radius of 16" at the last fret. The fretboard blank is 3/8" × 2 1/2" × 21", and is flat on one side. The finished fretboards are 7/32" thick at the crown, and taper from 1 11/16" at the nut to 2 3/16" at the 12th fret (12.670" from the nut).

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Violin Free Plate Mode Tuning Reprised

Violin Free Plate Mode Tuning Reprised

by Edgar B. Singleton

Originally published in American Lutherie #103, 2010



In the early stages of violin building, the outline of the top and back plates are established, as is the contour of the outside surfaces. Wood is removed from the underside of each plate until the thickness of the plate is a millimeter or so thicker than expected to be in the final form. The f-holes are cut; the bass bar and purfling are installed. The time has then come to graduate the plates, i.e., regulate the thickness of the plates in an attempt to assure that the finished violin will have all of the desired characteristics. Some builders “graduate to thickness” by carefully copying thickness measurements from important old violins. They listen to the pitches of tap tones and have learned ways to adjust these pitches. They have also learned to bend and twist the plates in their hands with the goal of assessing elastic properties, using experience to relate these “felt” properties to the finished violin.1 These processes involve as much art as science and require many years of carefully evaluated experience. This experience is very difficult to articulate to the novice builder.

One process associated with graduating the plates that is related to tap tones is referred to as “free plate mode tuning.”2 3 4 5 The following exposition is intended to help instrument builders, familiar with the material contained in the above references, understand the basis of free plate mode tuning as it is based on some simple physics and to provide a technique to fine tune each mode (tap tone) individually. The purpose of this paper is to give the builder a new basis on which to visualize where, and to understand why, to remove wood if one wishes to tune the free plates of a violin.

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Violin Ribs/Latent Tension

Violin Ribs/Latent Tension

by John Meng

Originally published in Guild of American Luthiers Data Sheet #287, 1984 and Big Red Book of American Lutherie Volume One, 2000



Bending Ribs

When wood is bent, the length of the outer surface increases or the length of the inner surface decreases; or most likely some combination of the two occurs. In soft woods, the fibers stretch and compress more easily than they do in hard woods, so soft woods can successfully be bent to smaller radii than can hard woods before the wood fractures.

Thin maple strips used to form violin ribs must be bent to small radii at the corners. Maple being a hard wood, there is a tendency for fibers along the inner surface to strongly resist compression.

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Finite Element Simulation of Guitar Top Vibration

Finite Element Simulation of Guitar Top Vibration

by Phil Banks

Originally published in American Lutherie #18, 1989



The use of engineering finite element analysis software to determine modes and natural resonant frequencies of a guitar top can be a useful (albeit lengthy) process which, if used judiciously, can yield useful information to the guitar maker.

As a graduate mechanical engineer and a guitar maker, I’ve always been interested in marrying the discipline of the luthier’s craft with that of science. I got that chance last year at the University of Sydney. While working as a programmer developing a Finite Element package, I was asked to produce a demonstration of the program’s capabilities. I decided to analyze a guitar top.

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Tuning the Guitar

Tuning the Guitar

by Ian Noyce

Originally published Guild of American Luthiers Data Sheet #56, 1977 and Big Red Book of American Lutherie Volume One, 2000



Because the guitar has fixed frets set to an even temperament, tuning it properly is not the cut-and-dried process that many people believe. And due to various factors that we’ll get to shortly, if the guitar’s bridge is placed exactly where the nominal scale length says it should be, the instrument may not play in tune at all.

The two most common methods of tuning are: (1) the 4th- and 5th-fret method and (2) the harmonic method. Both of these methods are often misunderstood through confusion regarding perfect (or Pythagorean) intervals and even-tempered intervals.

The 4th- and 5th-fret method. Theoretically, this is the simplest method as it simply involves tuning unison intervals. The A string can be tuned to an A tuning fork, then the bass E is fretted at the 5th fret and tuned in unison with the open A. The D string is tuned in unison with the 5th fret of the A, the G string is tuned to the 5th fret of the D, the B string is tuned to the fourth fret of the G, and the high E is tuned to the 5th fret of the B. In practice this can be difficult because any errors are cumulative. It’s also true that many guitars tuned this way will not play in tune in all keys.

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