Tuning a Guitar to the Harmonic Series for Primer Music 150X Winter, 2012

Total Page:16

File Type:pdf, Size:1020Kb

Tuning a Guitar to the Harmonic Series for Primer Music 150X Winter, 2012 Tuning a guitar to the harmonic series For Primer Music 150x Winter, 2012 UCSC, Polansky Tuning is in the D harmonic series. There are several options. This one is a suggested simple method that should be simple to do and go very quickly. VI Tune the VI (E) low string down to D (matching, say, a piano) D = +0¢ from 12TET fundamental V Tune the V (A) string normally, but preferably tune it to the 3rd harmonic on the low D string (node on the 7th fret) A = +2¢ from 12TET 3rd harmonic IV Tune the IV (D) string a ¼-tone high (1/2 a semitone). This will enable you to finger the 11th harmonic on the 5th fret of the IV string (once you’ve tuned). In other words, you’re simply raising the string a ¼-tone, but using a fretted note on that string to get the Ab (11th harmonic). There are two ways to do this: 1) find the 11th harmonic on the low D string (very close to the bridge: good luck!) 2) tune the IV string as a D halfway between the D and the Eb played on the A string. This is an approximation, but a pretty good and fast way to do it. Ab = -49¢ from 12TET 11th harmonic III Tune the III (G) string to a slightly flat F# by tuning it to the 5th harmonic of the VI string, which is now a D. The node for the 5th harmonic is available at four places on the string, but the easiest one to get is probably at the 9th fret. F# = -14¢ from 12TET 5th harmonic II Tune the II (B) string up almost a semitone, to a C that is about 1/6th-tone flat. Use the VI (D) string to get the 7th harmonic. The 7th harmonic is available at six places on the string, all of which should sound clearly, but the easiest one is probably right before the 3rd fret (alternatively, on electrics, it’s usually about halfway between the bridge and neck pickups). C = -31¢ from 12TET 7th harmonic I Tune the high (I) E string to E, but as a P5th to the V string, by sounding the 3rd harmonic (7th fret node) on the V string E = +4 from 12TET 9th harmonic .
Recommended publications
  • A Framework for the Static and Dynamic Analysis of Interaction Graphs
    A Framework for the Static and Dynamic Analysis of Interaction Graphs DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Sitaram Asur, B.E., M.Sc. * * * * * The Ohio State University 2009 Dissertation Committee: Approved by Prof. Srinivasan Parthasarathy, Adviser Prof. Gagan Agrawal Adviser Prof. P. Sadayappan Graduate Program in Computer Science and Engineering c Copyright by Sitaram Asur 2009 ABSTRACT Data originating from many different real-world domains can be represented mean- ingfully as interaction networks. Examples abound, ranging from gene expression networks to social networks, and from the World Wide Web to protein-protein inter- action networks. The study of these complex networks can result in the discovery of meaningful patterns and can potentially afford insight into the structure, properties and behavior of these networks. Hence, there is a need to design suitable algorithms to extract or infer meaningful information from these networks. However, the challenges involved are daunting. First, most of these real-world networks have specific topological constraints that make the task of extracting useful patterns using traditional data mining techniques difficult. Additionally, these networks can be noisy (containing unreliable interac- tions), which makes the process of knowledge discovery difficult. Second, these net- works are usually dynamic in nature. Identifying the portions of the network that are changing, characterizing and modeling the evolution, and inferring or predict- ing future trends are critical challenges that need to be addressed in the context of understanding the evolutionary behavior of such networks. To address these challenges, we propose a framework of algorithms designed to detect, analyze and reason about the structure, behavior and evolution of real-world interaction networks.
    [Show full text]
  • To the New Owner by Emmett Chapman
    To the New Owner by Emmett Chapman contents PLAYING ACTION ADJUSTABLE COMPONENTS FEATURES DESIGN TUNINGS & CONCEPT STRING MAINTENANCE BATTERIES GUARANTEE This new eight-stringed “bass guitar” was co-designed by Ned Steinberger and myself to provide a dual role instrument for those musicians who desire to play all methods on one fretboard - picking, plucking, strumming, and the two-handed tapping Stick method. PLAYING ACTION — As with all Stick models, this instrument is fully adjustable without removal of any components or detuning of strings. String-to-fret action can be set higher at the bridge and nut to provide a heavier touch, allowing bass and guitar players to “dig in” more. Or the action can be set very low for tapping, as on The Stick. The precision fretwork is there (a straight board with an even plane of crowned and leveled fret tips) and will accommodate the same Stick low action and light touch. Best kept secret: With the action set low for two-handed tapping as it comes from my setup table, you get a combined advantage. Not only does the low setup optimize tapping to its SIDE-SADDLE BRIDGE SCREWS maximum ease, it also allows all conventional bass guitar and guitar techniques, as long as your right hand lightens up a bit in its picking/plucking role. In the process, all volumes become equal, regardless of techniques used, and you gain total control of dynamics and expression. This allows seamless transition from tapping to traditional playing methods on this dual role instrument. Some players will want to compromise on low action of the lower bass strings and set the individual bridge heights a bit higher, thereby duplicating the feel of their bass or guitar.
    [Show full text]
  • Pipa by Moshe Denburg.Pdf
    Pipa • Pipa [ Picture of Pipa ] Description A pear shaped lute with 4 strings and 19 to 30 frets, it was introduced into China in the 4th century AD. The Pipa has become a prominent Chinese instrument used for instrumental music as well as accompaniment to a variety of song genres. It has a ringing ('bass-banjo' like) sound which articulates melodies and rhythms wonderfully and is capable of a wide variety of techniques and ornaments. Tuning The pipa is tuned, from highest (string #1) to lowest (string #4): a - e - d - A. In piano notation these notes correspond to: A37 - E 32 - D30 - A25 (where A37 is the A below middle C). Scordatura As with many stringed instruments, scordatura may be possible, but one needs to consult with the musician about it. Use of a capo is not part of the pipa tradition, though one may inquire as to its efficacy. Pipa Notation One can utilize western notation or Chinese. If western notation is utilized, many, if not all, Chinese musicians will annotate the music in Chinese notation, since this is their first choice. It may work well for the composer to notate in the western 5 line staff and add the Chinese numbers to it for them. This may be laborious, and it is not necessary for Chinese musicians, who are quite adept at both systems. In western notation one writes for the Pipa at pitch, utilizing the bass and treble clefs. In Chinese notation one utilizes the French Chevé number system (see entry: Chinese Notation). In traditional pipa notation there are many symbols that are utilized to call for specific techniques.
    [Show full text]
  • EDUCATION GUIDE History and Improvisation: Making American Music “We Play the Same Songs but the Solos Are Different Every Night
    EDUCATION GUIDE History and Improvisation: Making American Music “We play the same songs but the solos are different every night. The form is the same, but the improvisations are what is really what makes that music what it is…Jazz is about being creative, all the time.” – Scotty Barnhart LESSON OVERVIEW In this lesson, students will view the MUSIC episode from the PBS series Craft in America. The episode features the skilled craftwork required to make ukuleles, trumpets, banjos, guitars, and timpani mallets. Students will hear musicians playing each of the instruments. Students will also hear the musicians talk about their personal connection to their instruments. Additionally, the program illustrates how a study of American music is a study of American history. After viewing the episode, students will investigate connections between musicians and their instruments and between American music and American history. The studio portion of the lesson is designed around the idea of creating a maker space in which students experiment with and invent prototype instruments. Instructions are also included for a basic banjo made from a sturdy cardboard box. Note: While this lesson can take place completely within the art department, it is an ideal opportunity to work with music teachers, history teachers, technical education teachers, and physics teachers (for a related study of acoustics.) Grade Level: 9-12 Estimated Time: Six to eight 45-minute class periods of discussion, research, design Craft In America Theme/Episode: MUSIC Background Information MUSIC focuses on finely crafted handmade instruments and the world-renowned artists who play them, demonstrating the perfect blend of form and function.
    [Show full text]
  • History Special Tools Hardware Dulcimer Wood Onlineextra
    onlineEXTRA Issue #80 (Dec/Jan 2018) Make a Mountain Dulcimer More Dulcimer Info History Mountain dulcimers are attributed to the Scotch-Irish who settled in Appalachia, with drone strings reminiscent of bag pipes. Part of the appeal of the dulcimer is that it could be built from locally available wood with basic hand tools. Traditional designs range from a rough rectangular box held together with nails, bailing wire frets, and ‘possum gut strings—to beautifully crafted instruments with graceful curves, inlay, intricate carving, and satin finish. Special tools A look through a luthier’s catalog will present you with a dizzying array of special saws, clamps, jigs, and other instrument-making tools. A modestly equipped shop has just about all the tools needed. The one exception is the fret saw. It is a fine-tooth narrow kerf back saw designed for cutting slots for frets. It is also a great saw for making fine cuts on other projects, so it is well worth the investment. A special clamp for holding the back and soundboard to the sides can easily be made from 11/2" schedule 40 PVC. These are about 1/4" wide with a 1/2" gap. You can make a couple dozen in just a few minutes and, like the fret saw, they will prove useful in other woodworking projects (and make decent shower curtain rings, too). Hardware There are a few “store bought” parts (fret wire, tuning pins, and strings) that make the assembly much easier and the playing more user friendly. You might want to order these now, so you won’t have to wait when you’re ready for them.
    [Show full text]
  • Experiment 12
    Experiment 12 Velocity and Propagation of Waves 12.1 Objective To use the phenomenon of resonance to determine the velocity of the propagation of waves in taut strings and wires. 12.2 Discussion Any medium under tension or stress has the following property: disturbances, motions of the matter of which the medium consists, are propagated through the medium. When the disturbances are periodic, they are called waves, and when the disturbances are simple harmonic, the waves are sinusoidal and are characterized by a common wavelength and frequency. The velocity of propagation of a disturbance, whether or not it is periodic, depends generally upon the tension or stress in the medium and on the density of the medium. The greater the stress: the greater the velocity; and the greater the density: the smaller the velocity. In the case of a taut string or wire, the velocity v depends upon the tension T in the string or wire and the mass per unit length µ of the string or wire. Theory predicts that the relation should be T v2 = (12.1) µ Most disturbances travel so rapidly that a direct determination of their velocity is not possible. However, when the disturbance is simple harmonic, the sinusoidal character of the waves provides a simple method by which the velocity of the waves can be indirectly determined. This determination involves the frequency f and wavelength λ of the wave. Here f is the frequency of the simple harmonic motion of the medium and λ is from any point of the wave to the next point of the same phase.
    [Show full text]
  • Following the Trail of the Snake: a Life History of Cobra Mansa “Cobrinha” Mestre of Capoeira
    ABSTRACT Title of Document: FOLLOWING THE TRAIL OF THE SNAKE: A LIFE HISTORY OF COBRA MANSA “COBRINHA” MESTRE OF CAPOEIRA Isabel Angulo, Doctor of Philosophy, 2008 Directed By: Dr. Jonathan Dueck Division of Musicology and Ethnomusicology, School of Music, University of Maryland Professor John Caughey American Studies Department, University of Maryland This dissertation is a cultural biography of Mestre Cobra Mansa, a mestre of the Afro-Brazilian martial art of capoeira angola. The intention of this work is to track Mestre Cobrinha’s life history and accomplishments from his beginning as an impoverished child in Rio to becoming a mestre of the tradition—its movements, music, history, ritual and philosophy. A highly skilled performer and researcher, he has become a cultural ambassador of the tradition in Brazil and abroad. Following the Trail of the Snake is an interdisciplinary work that integrates the research methods of ethnomusicology (oral history, interview, participant observation, musical and performance analysis and transcription) with a revised life history methodology to uncover the multiple cultures that inform the life of a mestre of capoeira. A reflexive auto-ethnography of the author opens a dialog between the experiences and developmental steps of both research partners’ lives. Written in the intersection of ethnomusicology, studies of capoeira, social studies and music education, the academic dissertation format is performed as a roda of capoeira aiming to be respectful of the original context of performance. The result is a provocative ethnographic narrative that includes visual texts from the performative aspects of the tradition (music and movement), aural transcriptions of Mestre Cobra Mansa’s storytelling and a myriad of writing techniques to accompany the reader in a multi-dimensional journey of multicultural understanding.
    [Show full text]
  • Guitar Anatomy Glossary
    GUITAR ANATOMY GLOSSARY abalone: an iridescent lining found in the inner shell of the abalone mollusk that is often used alongside mother of pearl; commonly used as an inlay material. action: the distance between the strings and the fretboard; the open space between strings and frets. back: the part of the guitar body held against the player’s chest; it is reflective and resonant, and usually made of a hardwood. backstrip: a decorative inlay that runs the length of the center back of a stringed instrument. binding: the inlaid corner trim at the very edges of an instrument’s body or neck, used to provide aesthetic appeal, seal open wood and to protect the edge of the face and back, as well as the glue joint. bout: the upper or lower outside curve of a guitar or other instrument body. body: an acoustic guitar body; the sound-producing chamber to which the neck and bridge are attached. body depth: the measurement of the guitar body at the headblock and tailblock after the top and back have been assembled to the rim. bracing: the bracing on the inside of the instrument that supports the top and back to prevent warping and breaking, and creates and controls the voice of the guitar. The back of the instrument is braced to help distribute the force exerted by the neck on the body, to reflect sound from the top and act sympathetically to the vibrations of the top. bracing, profile: the contour of the brace, which is designed to control strength and tone. bracing, scalloped: used to describe the crests and troughs of the braces where mass has been removed to accentuate certain nodes.
    [Show full text]
  • Homelab 2 [Solutions]
    Homelab 2 [Solutions] In this homelab we will build a monochord and measure the fundamental and harmonic frequencies of a steel string. The materials you will need will be handed out in class. They are: a piece of wood with two holes in it, two bent nails, and a steel guitar string. The string we will give you has a diameter of 0.010 inch. You will also find it helpful to have some kind of adhesive tape handy when you put the string on the monochord. As soon as you can, you should put a piece of tape on the end of the string. The end is sharp and the tape will keep you from hurting your fingers. Step 1 Push the nails into the holes as shown above. They should go almost, but not quite, all the way through the board. If you push them too far in they will stick out the bottom, the board will not rest flat, and you might scratch yourself on them. You won't need a hammer to put the nails in because the holes are already big enough. You might need to use a book or some other solid object to push them in, or it might help to twist them while you push. The nails we are using are called 'coated sinkers.' They have a sticky coating that will keep them from turning in the holes when you don't want them to. It cannot be iterated enough to be careful with the nails. Refer to the diagram above if you are unsure about how the final product of this step looks like.
    [Show full text]
  • Guitar Harmonics - Wikipedia, the Free Encyclopedia Guitar Harmonics from Wikipedia, the Free Encyclopedia
    3/14/2016 Guitar harmonics - Wikipedia, the free encyclopedia Guitar harmonics From Wikipedia, the free encyclopedia A guitar harmonic is a musical note played by preventing or amplifying vibration of certain overtones of a guitar string. Music using harmonics can contain very high pitch notes difficult or impossible to reach by fretting. Guitar harmonics also produce a different sound quality than fretted notes, and are one of many techniques used to create musical variety. Contents Basic and harmonic oscillations of a 1 Technique string 2 Overtones 3 Nodes 4 Intervals 5 Advanced techniques 5.1 Pinch harmonics 5.2 Tapped harmonics 5.3 String harmonics driven by a magnetic field 6 See also 7 References Technique Harmonics are primarily generated manually, using a variety of techniques such as the pinch harmonic. Another method utilizes sound wave feedback from a guitar amplifier at high volume, which allows for indefinite vibration of certain string harmonics. Magnetic string drivers, such as the EBow, also use string harmonics to create sounds that are generally not playable via traditional picking or fretting techniques. Harmonics are most often played by lightly placing a finger on a string at a nodal point of one of the overtones at the moment when the string is driven. The finger immediately damps all overtones that do not have a node near the location touched. The lowest-pitch overtone dominates the resulting sound. https://en.wikipedia.org/wiki/Guitar_harmonics 1/6 3/14/2016 Guitar harmonics - Wikipedia, the free encyclopedia Overtones When a guitar string is plucked normally, the ear tends to hear the fundamental frequency most prominently, but the overall sound is also 0:00 MENU colored by the presence of various overtones (integer multiples of the Tuning a guitar using overtones fundamental frequency).
    [Show full text]
  • LCC for Guitar - Introduction
    LCC for Guitar - Introduction In order for guitarists to understand the significance of the Lydian Chromatic Concept of Tonal Organization and the concept of Tonal Gravity, one must first look at the nature of string vibration and what happens when a string vibrates. The Lydian Chromatic concept is based in the science of natural acoustics, so it is important to understand exactly what happens acoustically to a note and the harmonic overtones that nature creates. A guitar string (or any string from any stringed instrument) vibrates when plucked or struck, producing a tone. The vibrating string creates a natural resonant series of vibration patterns which are called Harmonics. When you strike the string by itself, it vibrates back and forth and moves air molecules, producing sound. This is called a FUNDAMENTAL. (See fig 1.01a) Fig 1.01a – FUNADAMENTAL/OPEN STRING = A 440hz/440cps The fundamental vibration pattern on a single string. This is the FUNDAMENTAL vibration or tone and can be equated to a fixed amount of vibrations or cycles per second (cps) For example, consider this to be the open ‘A’ string producing the note A which in turn a universally considered to vibrate at 440cps or the equivalent of 440hz. If you loosen a guitar string you can visually see the result of the vibrations; the string makes a wide arc near the center and it narrows towards each end. When you touch the string exactly in the center (exactly between both ends or on the guitar the physical location is at the 12 th fret) it divides the vibration exactly in half and produces a note or tone exactly one octave higher in pitch.
    [Show full text]
  • The Physics of a Longitudinally Vibrating “Singing” Metal Rod
    UIUC Physics 193/406 Physics of Music/Musical Instruments The Physics of a Longitudinally Vibrating Metal Rod The Physics of a Longitudinally Vibrating “Singing” Metal Rod: A metal rod (e.g. aluminum rod) a few feet in length can be made to vibrate along its length – make it “sing” at a characteristic, resonance frequency by holding it precisely at its mid-point with thumb and index finger of one hand, and then pulling the rod along its length, toward one of its ends with the thumb and index finger of the other hand, which have been dusted with crushed violin rosin, so as to obtain a good grip on the rod as it is pulled. L L L L/2 L/2 Pull on rod here along its length Hold rod here with thumb with violin rosin powdered thumb and index finger of one hand and index finger of other hand, stretching the rod The pulling motion of the thumb and index finger actually stretches the rod slightly, giving it potential energy – analogous to the potential energy associated with stretching a spring along its length, or a rubber band. The metal rod is actually an elastic solid – elongating slightly when pulled! Pulling on the rod in this manner excites the rod, causing both of its ends to simultaneously vibrate longitudinally, back and forth along its length at a characteristic resonance frequency known as its fundamental frequency, f1. For an excited aluminum rod of length, L ~ 2 meters, it is thus possible that at one instant in time both ends of the rod will be extended a small distance, L ~ 1 mm beyond the normal, (i.e.
    [Show full text]