1aMU4 – In search of huge sound… or huge strings, at least

Pawel Bielski – pawbiels@pg.edu.pl
Hanna Pruszko – hanprus1@pg.edu.pl
Tomasz Mikulski – tomi@pg.edu.pl
Gdansk University of Technology
Narutowicza 11/12, 80-233 Gdansk
Poland

Popular version of paper 1aMU4 Numerical and experimental assessment of string gauge influence on guitar tone
Presented Tuesday morning, June 08, 2021
180th ASA Meeting, Acoustics in Focus

Meet Adam. Adam loves the nines (that is, 0.09-inch gauge, or 9’s, named by the diameter of the high E string). When he touches a guitar stringed with the 9’s, it seems soft and responsive under his fingers. This phenomenon is called “feel”. Adam picks a guitar with a proper feel and unites with the instrument. Suddenly physical bounds disappear. Adam believes in supernatural traits of the 9’s and no research can change his mind.

But we can still try.

Guitar players are obsessed with string gauges. From the super slinky 7’s of Billy Gibbons, through the agile 8’s and 9’s of Jimi Hendrix and Jimmy Page, massive sound of Joe Bonamassa (11) and Stevie Ray Vaughan (13), to Pat Martino’s super fat 15’s and extreme twang of Dick Dale (16’s). A wide selection of string gauges covers a variety of guitar playing styles.

Thicker strings are harder to bend but carry more force. Vibration is essentially very fast bending in different modes (shapes) – 1st harmonic (fundamental) and upper harmonics (overtones). Harmonic composition is called the brightness of the string. Higher harmonics create a sharp and open sound. Lower harmonics help to beef up the tone. Definition of chords also benefits from profound fundamentals.

strings

Fundamental mode and upper harmonics of a vibrating string [Source image: Harmonics.png]

Depending on the gauge, the total force carried by electric guitar strings ranges from the weight equivalent of a ten-year-old child to an adult man. It makes nearly triple the difference. Acoustic guitars offer a more humble selection of 10’s – 13’s string gauges, but the choice might be even more critical. The acoustic sound is raw and less processed. It depends on the physical features of the instrument. Fiddling with the pulling force and vibrating mass on a resonant guitar body must make a difference. The body gets tenser and stiffer. It is driven hard and significantly deformed. Will it be able to breathe freely?

Imagine borrowing your general practitioner’s stethoscope and listening to the acoustic guitar’s soundboard while it plays. This is roughly how we used accelerometers. Low E strings of different gauges were repeatedly tested for their volume, sustain (duration of sound), and harmonic composition. The samples were recorded with a microphone too. We analyzed the sound spectrum during different stages of the sound.

Setup of accelerometers [Source image: AccSetup.png]

Most findings agree with the general beliefs regarding string gauges besides one major exception. The weak sustain of heavy strings might be a surprise to many guitar players. Thick strings have a rich and loud attack yet immediately lose their superb qualities. They seem to excel at quick, punchy notes, but struggle with slow-paced singing solos. In the long run, light strings were more sustainable, retaining their harmonics in time.

[Recording of 13’s string: E6nr13.mp3]

[Recording of 10’s string: E6nr10.mp3]

Recordings of heavy and light strings (flanger effect caused by averaging from multiple samples

Advantages of the different gauges shown at two scales [Source image: Signals.png]

Other than that, heavy strings are generally louder and more substantial, while light strings seem brighter and more open. Thick strings excite the body modes (structural vibration) more, while light ones favor air resonance.

Adam will probably not readjust his beliefs, but maybe you will?

Summary of the findings

2pMU3 – Why do harpists still prefer gut strings?

Jim Woodhouse — jw12@cam.ac.uk
Cambridge University Engineering Department
Trumpington St
Cambridge CB2 1PZ, U.K.

Nicolas Lynch-Aird — lynchaird@yahoo.co.uk
The Old Forge
Burnt House Lane
Battisford
Suffolk IP14 2ND, U.K.

Popular version of paper ‘2pMU3’ String choice: Why do harpists still prefer gut?
Presented Wednesday afternoon, June 9, 2021
180th ASA Meeting, Acoustics in Focus

Classical guitarists have all abandoned traditional gut strings in favour of nylon, but harpists still prefer gut.  Why is this? A study of the various limits on string choice for musical instruments has shown that the answer lies in a difference of “damping” in the strings, which is responsible for a difference in brightness of the sound.

When choosing a string for an instrument, the player knows the string length and the frequency it will be tuned to: their task is to choose the material and the diameter. The various different constraints on that choice can be summarised in a chart: a schematic version is shown here.

strings

Schematic chart for choosing strings for musical instruments

The length and the frequency multiplied together defines the position on the horizontal axis. The player’s choice then consists of moving along a vertical line through that point, to choose a string diameter. They need to make a choice within the blue region, otherwise something will go wrong.  The exact shape and position of this blue region depends on the choice of string material.

Obviously the string must not break. There are also upper and lower limits on the tension: if a string is too slack or too tight, it feels wrong to the player.  Less obviously, the choice must lie beneath the dashed line labelled “damping too high”, otherwise the sound will become a dull thud rather than a ringing musical tone. This is where the harp differs from the guitar.  Guitar strings stay well clear of the dashed line, but for the longer, lower-pitched strings of a harp, players want to use strings with very high tension so that the “feel” is right. But that pushes them towards the dashed line, and it is this damping limit that defines the practical limit on string choice. When the detailed charts are compared for nylon and  gut strings, the dashed line is higher for gut. That gives a bit more “headroom” for the player’s choice, and allows them to choose a string that feels good under the fingers, while still having a satisfyingly bright and ringing tone.

4aMUa3 – Musical Notes translate to Emotions? A neuro-acoustical endeavor with Indian Classical music

Shankha Sanyal
Samir Karmakar
Dipak Ghosh
Jadavpur University
Kolkata: 700032, INDIA

Archi Banerjee
Rekhi Centre of Excellence for the Science of Happiness
IIT Kharagpur, 721301, INDIA

Popular version of paper 4aMUa3 Emotions from musical notes? A psycho-acoustic exploration with Indian classical music
Presented Thursday morning, December 10, 2020
179th ASA Meeting, Acoustics Virtually Everywhere
Read the article in Proceedings of Meetings on Acoustics

The Indian classical music (ICM) system is based on the note system which consists of 12 notes, each having a definite frequency. The main feature of this music form is the existence of ‘Ragas’, which are unique, having a definite combination of these 12 notes, though the presence of 12 notes is not essential in each of the Raga; some can have only 5 notes which are usually called ‘pentatonic Ragas or scales’. Each Raga evokes not a particular emotion (rasa) but a superposition of different emotional states such as joy, sadness, anger, disgust, fear etc. A mere change in the single frequency of a Raga clip changes it to another Raga and also the associated emotional states change along with it. In this work, for the first time, we envisage to study how the emotion perception in listeners’ change when there is an alteration of a single note in a pentatonic Raga and also when a particular note(s) is replaced by its flat/sharp counterpart. Robust nonlinear signal processing methods have been utilized to quantify the acoustical signal as well as the brain arousal response corresponding to the two pair of Ragas taken for our study.

The two pair of ragas chosen for our study:

Raga Durga- sa re ma pa dha sa 

Raga Gunkali– sa RE ma pa DHA sa

The notes ‘re’ and ‘dha’ of Durga is changed to their respective sharp/flat counterparts which change Raga Durga to Raga Gunkali.

Raga Durga- sa re ma pa dha sa

Raga Bhupali-  sa re ga pa dha sa

The note ‘ma’ in Raga Durga, when changed to ‘ga’, makes the Raga Bhupali

Human Response Analysis-
A human response study was done with 50 subjects who were provided with an emotion chart of the basic 4 emotions, and were asked to mark the clips with their perceived emotional arousal.

The radar plots for the human response analysis:

Indian Classical music Indian Classical music

(Fig. 1 a-b) Pair 1

Indian Classical music Indian Classical music

(Fig. 1 c-d) Pair 2

It is seen that the change of a single note manifests in a complete change in emotional appraisal at the perceptual level of the listeners. In the next section, EEG response of 10 participants (who were made to listen to these raga clips) has been studied using nonlinear multifractal tools. Multifractality is an indirect measure of the inherent signal complexity present in the highly non-stationary EEG fluctuations.

The following figures give the averaged multifractality corresponding to the frontal and temporal lobes in alpha and theta EEG frequency range for the two pair of raga clips. P1…P5 represents the different phrases (note sequences) in which the main changes between the two ragas have been done.

(Fig. 2 a-b) Pair 1

(Fig. 2 c-d) Pair 2

For the first pair, alpha and theta power decreases considerably in the frontal lobe, while in temporal lobes, phrase specific arousal is seen. For the second pair, the arousal is very much specific to the phrases. This can be attributed to the fact that the human response data showed the emotional arousal in second pair is not strongly opposite to each other, but a mixed response is obtained. For the first time, a scientific analysis on how the acoustic, perceptual and neural features change when the emotional appraisal is changed due to the change of a single frequency in a particular Raga is reported in the context of Indian Classical Music

3pMUa4 – Acoustical analysis of 3D-printed snare drums

Chris Jasinski – jasinski@hartford.edu
University of Hartford
200 Bloomfield Ave
West Hartford, CT 06117

Popular version of paper 3pMUa4
Presented Wednesday afternoon, December 09, 2020
179th ASA Meeting, Acoustics Virtually Everywhere

For many years, 3D printing (or additive manufacturing) has been a growing field with applications ranging from desktop trinkets to prototypes for replacements of human organs. Now, Klapel Percussion Instruments has designed its first line of 3D-printed snare drums.

Snare drums are commonly used in drum sets, orchestras, and marching bands. They are traditionally made with wood or metal shells, metal rims, plastic (mylar) skins, and metal connective hardware including bolts, lugs, and fasteners. For the first phase of Klapel prototypes, the shell and rim are replaced with a proprietary carbon fiber composite. Future iterations intend to replace all of the hardware with 3D printing as well.  The shell and rim are produced layer by layer until the final shape is formed. Even with high quality printers, layers can be seen in the final texture of 3D-printed objects. These layers appear as horizontal lines and vertical seams where each layer starts and finishes.

Snare drums

3D-printed snare drum and detail of finished texture.

Klapel Percussion Instruments contacted the University of Hartford Acoustics Program to assess if having a 3D-printing shell and rim changes the fundamental vibrational and acoustical characteristics of the drum. To test this, undergraduate students developed a repeatable drum striking device. The machine relies on gravity and a nearly zero-friction bearing to strike a snare drum from a consistent height above the playing surface. With precise striking force, the resulting sound produced by the drum was recorded in the University of Hartford’s anechoic chamber (a laboratory designed to eliminate all sound reflections or ‘echoes’, shown in the example photo of the striking machine). The recordings were then analyzed for their frequency content.

Snare drums

Snare drum striking machine inside Paul S. Veneklasen Research Foundation Anechoic Chamber at University of Hartford.

Along with the acoustical testing, the drum shell (the largest single component of a snare drum) underwent ‘modal analysis’, where 30 points are marked on each shell and struck with a calibrated force-sensing hammer. The resulting vibration of the drum is measured with an accelerometer. The fundamental shapes (or ‘modes’) of vibration can then be visualized using processing software.

Snare drums

Vibrational mode shapes for maple drum shell [left] and 3D-printed shell [right].

Ultimately, the vibrational and acoustical analysis resulted in the same conclusions. The fundamental shapes of vibration and the primary frequency content of the snare drum is unaffected by the process of 3D printing. The most prominent audible frequencies and vibrational shapes are identical in both the maple wood shell and the carbon fiber 3D-printed shell, as seen in the visualized modes of vibration. This means that the 3D-printed drum technology is a viable alternative to more traditional manufacturing techniques for drums.

There are substantial, measurable variations that impact the more subtle characteristics of the drum at higher, less prominent frequencies, and for more complex vibration shapes. These are noticeable above 1000 Hz in the frequency analysis comparison.

Snare drums

Frequency analysis at two striking locations for maple (wood) and carbon fiber (3D-printed) drum.

Future testing, including subjective listening tests, will aim to identify how these smaller variations impact listeners and performers. The results of the future tests can help determine how acoustical metrics can predict listener impressions.

4aMUa1 – Songs: Lyrics on the melody or melody of the lyrics?

Archi Banerjee – archibanerjee7@iitkgp.ac.in
Priyadarshi Patnaik – bapi@hss.iitkgp.ac.in
Rekhi Centre of Excellence for the Science of Happiness
Indian Institute of Technology Kharagpur, 721301, INDIA

Shankha Sanyal – ssanyal.ling@jadavpuruniversity.in
Souparno Roy – thesouparnoroy@gmail.com
Sir C. V. Raman Centre for Physics and Music
Jadavpur University, Kolkata: 700032, INDIA

Popular version of paper 4aMUa1 Lyrics on the melody or melody of the lyrics?
Presented Thursday morning, December 10, 2020
179th ASA Meeting, Acoustics Virtually Everywhere
Read the article in Proceedings of Meetings on Acoustics

The musicians often say “When a marriage happens between a lyric and a melody, only then a true song is born”! But, which impacts the audience more in a song – Melody or lyrics? The answer to this question is still unknown. What happens when the melody is hummed independently without the lyrics? How does that affect the acoustical waveform of the original song? Does the emotional appraisal remain same in both cases? The present work attempts to answer these questions using songs from different genres of Indian music. Recordings of two pairs of contrast emotion (happy-sad) evoking Raga bandishes from Indian Classical Music (ICM) and one pair of Bengali contemporary songs of opposite emotions (happy-sad) were taken from an experienced female professional singer who was asked to consecutively sing (with proper meaningful lyrics) and hum (without using any lyric or meaningful words) the songs, keeping the melodic structure, pitch and tempo same. In ICM, the basic building blocks are Ragas – bandish is a song composed in a particular Raga. The chosen audio clips are:

Genre  Chosen Songs Primary emotion Tempo
Indian Classical Music Raga Multani vilambit bandish Sad ~ 45 bpm
Raga Hamsadhwani vilambit bandish Happy ~ 50 bpm
Raga Multani drut bandish Sad ~ 90 bpm
Raga Hamsadhwani drut bandish Happy ~ 110 bpm
Bengali Contemporary Music O tota pakhi re Sad ~ 50 bpm
Ami cheye cheye dekhi Happy ~ 130 bpm
a)

b)

Audio 1(a,b): Sample audios of (a) Humming and (b) Song versions of same melodic part

a)Song b)
Song

Figure 1(a,b): Sample acoustical waveforms and pitch contours of (a) Humming and (b) Song versions of same melodic part

Next, using different sets of humming-song pairs from the chosen songs as stimuli, Electroencephalogram (EEG) recordings were taken from 5 musically untrained participants who understand the languages Hindi (of bandishes) and Bengali. Both music and EEG signals have highly complex structures, but their inherent geometry features self similarity or structural repetitions. Chaos based nonlinear fractal technique (Detrended fluctuation analysis or DFA) was applied both on the acoustical waveforms and their corresponding EEG signals. The changes in self similarity were calculated for each humming-song pair to study the impact of lyrics both in acoustical and neurological levels.

a)song pairs b)song pairs

Figure 2(a,b): Variation in DFA scaling exponent in acoustical signals of humming-song pairs taken from songs of (a) Indian Classical music and (b) Bengali contemporary music

Acoustical analysis revealed that in songs where the lyrics is highly projected or emphasized (slow tempo vilambit bandish and Bengali contemporary songs), the DFA scaling exponent or self similarity decreases from humming to song version if the melodic pattern remains same. The sudden and spontaneous fluctuations in the pitch and intensity levels of the song versions due to the introduction of several consonants, rhythmic variations and pauses between words embedded in the lyrics may help in lowering the scale of self similarity.

a)song pairs b)

Figure 3(a,b): Average of differences in DFA scaling exponent in (a) Frontal electrodes (F3, F4, F7, F8 & FZ) and (b) Occipital (O1 & O2), Parietal (P3 & P4) and Temporal (T3 &T4) electrodes for different Humming-Song pairs of Bengali contemporary songs

EEG analysis revealed that for both genres of music, in songs with highly projected lyrics, self similarity in frontal lobe electrodes increases from humming to song version of the same melody; whereas in occipital, temporal and parietal electrodes, we observed an increment in DFA scaling exponent from humming to song for the slow tempo songs and a decrement in the same for high tempo songs.

Combining results of acoustic analysis and EEG analysis, the impact of lyrics was found to be significantly higher in lower tempo songs compared to higher tempo songs both in acoustical and neuro-cognitive level. This is a pilot study in the context of Indian music which endeavors to quantitatively analyze the contribution of lyrics in songs of different genre as well as different emotional content in both acoustical and neuro-cognitive domain with the help of a unique scaling exponent.

3pMUb3 – Does the act of ‘playing’ a violin measurably change any of its acoustic properties? — preliminary results

Ms. Kourtney Adkisson – kourtney.adkisson@cwu.edu
Dr. Andy Piacsek – andrew.piacsek@cwu.edu

Department of Physics
Central Washington University
400 E University Way
Ellensburg, WA 98926

Popular version of paper 3pMUb3
Presented Wednesday afternoon, December 9, 2020
179th ASA Meeting, Acoustics Virtually Everywhere

Among many violinists and luthiers, it is believed that violins need to be played (or vibrated) for some time in order for the tone to develop, a process known as “playing in.”  Although it is not uncommon for makers and sellers of violins to mechanically vibrate instruments continuously for several weeks before selling them, there is no scientific consensus on how, or to what extent, the instrument is altered in this process.

The work that we are presenting is the first stage of a long-term project that seeks to answer the question, “Does the act of ‘playing’ a violin measurably change any of its acoustic properties?”

Because many factors contribute to the sound that violins produce, it is challenging to identify changes in tonal characteristics that are due specifically to the cumulative effects of being played.  To address this challenge, we are conducting a systematic study utilizing three new sibling violins (Andre Tellis model 200, made in 2018):  two of these will be mechanically vibrated to simulate playing for several months, while the third will be a control – kept in the same environment, but not played.  During this time, we will periodically measure the vibrational and acoustic response of all three violins.

Before we begin artificially playing the violins, however, we need to understand how much variability we can expect in our measurements of the vibration response, which is essential for identifying subtle systemic changes in violin response that correlate with being vibrated over time.  Therefore, minimizing and quantifying measurement uncertainty is the objective of the initial phase of our project, which is reported here.

The measurement setup we evaluated consists of a violin that is suspended with rubber bands and excited by a mechanical shaker that exerts a lateral force on the bridge at many different frequencies, similar to forces exerted by vibrating strings.   A Laser Scanning Doppler Vibrometer (LSDV) is used to measure the vibrational response, or the amplitude of motion plotted as a function of frequency, at several locations on the top plate of each violin.  Information from all the scan points can be combined to construct an image of how the top plate is actually moving at each frequency.

The LSDV set-up is shown including the acoustical table, laser head, computer, and mechanical shaker.

violin

A violin is ready to be measured, the body suspended with rubber bands and a mechanical shaker attached.

Seven different modes are shown, in which the violin displays a dramatic response to a specific frequency.

We compared the vibration response of the three sibling violins. With the caveat that our measurement locations varied slightly among the instruments, our results show that the differences in response among sibling violins are comparable to the differences between the siblings and a ten year old Yamaha violin of comparable quality.

Andre Tellis violins

A comparison between the vibration response of three sibling Andre Tellis violins.

Yamaha violin

The vibration response of two sibling Andre Tellis violins and an older Yamaha violin.

To assess the uncertainty associated with our measurement method, we measured the vibrational response of the same violin on different dates.  Our measured response curves for the same violin are quite similar, but they are not identical.  These preliminary results indicate inherent variability in our system caused by small differences in the testing set-up or by minute changes to the violins themselves.

The vibration response for one of the sibling violins is shown for two different measurements in May 2019 and March 2019.

The vibration response for the Yamaha is shown for two different measurements in May 2019 and March 2019.

Additional measurements are needed to determine ways to reduce and quantify this uncertainty before we proceed with the next phase of the project.