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    Dept. for Speech, Music and Hearing

    Quarterly Progress andStatus Report

    Input admittance,

    eigenmodes, and quality of

    violins

    Alonso Moral, J. and Jansson, E. V.

    journal: STL-QPSR

    volume: 23

    number: 2-3

    year: 1982

    pages: 060-075

    http://www.speech.kth.se/qpsr

    http://www.speech.kth.se/http://www.speech.kth.se/qpsrhttp://www.speech.kth.se/qpsrhttp://www.speech.kth.se/
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    IV. MUSIC ACOUSTICS

    A-INPUT ADMITTANCE, EIGENMODES, AND QUALITY OF VIOLINS*

    ~e sGs lonso Moral and Erik

    V

    Jansson

    Abstract

    From a Scandinavian violinmakers' competition, a number of 24 vio-

    lins of different qualities were selected. Input admittances

    as

    function

    of frequency were recorded perpendicularly to the top plate at two

    positions on top of the bridge. The admittance curves at the side of

    the

    bass

    bar

    show

    three

    resonances at approximately

    400

    500,

    and 700 Hz and

    a broad resonance around 3 kHz. Three acoustical quality criteria were

    extracted from these curves:

    1) the average level of the three resonance

    peaks (high is favorable), 2) the discrepancies between

    single peak

    levels and the average level (small is favorable), and 3) steepness of

    upwards slope from a 1.4 to a

    3

    kHz region (steep is favorable).

    Be

    tween 1.4 and 3

    kHz

    the levels or input admittances of the bass

    bar

    and

    soun post sides tend to

    be

    the same. A fourth acoustical quality crite-

    rion was extracted from the two curves:

    4)

    the level discrepancies bet-

    ween the two curves (small is favorable). Calculated acoustical qudli-

    ty points correlate well with given tonal quality points (a correlation

    me cient of 0.96 with five deficient violins, xcluded.

    Introduction

    In a previous paper we presented representative acoustical pro-

    perties of violins.

    In this following paper we report on an investiga-

    tion of relations between these acoustical properties and tonal quality

    of violins. We seek answers to two questions:

    1.

    What are the most important properties of the violin?

    2. How

    well

    do

    these properties predict the quality of

    a violin?

    Eigenmodes

    and

    input admittance

    In a previous investigation we recorded representative eigenmodes

    for the violin (~lonsooral Jansson, 1982), see Fig

    1.

    In the eigen-

    mode T1 the main vibrations are in the top plate. We have interpreted

    this resonance as being the first top plate mode. Similar vibration

    pattern is to

    be

    found for the ~elmholtz' esonance

    A0

    our labelling),

    which seems strongly connected with the T1-resonance. In the eigenmode

    C3, the top

    and

    the back plates vibrate in phase. The vibration patterns

    are similar to that of the second mode of each of the two plates free

    This paper was presented to the 103rd Meeting of the Acoustical Socie-

    ty of America held in Chicago,

    Illinois, April 1982, paper U-3.

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    (~utchins,980). In the mode labelled C4

    the two plates also vibrate

    n

    phase. The vibration pattern is similar to that of the ring mode of

    free plates.

    At approximately 3 kHz the violin has its main bridge resonance, a

    tilting motion (Reinicke, 1973).

    y means of the so-called input admittance, that is, the resulting

    velocity at the driving point for given force, resonance frequencies,

    vibration levels,

    and @factors are easily recorded.

    n illustrative exampleof an input admittance curve is given in

    Fig 2. The curve shows a small

    peak

    marked AO,

    and

    four

    prominent pedks

    T1,

    C3,

    C4,and

    F.

    Thereafter follows a wiggly curve from which we can

    extract a hill with a maximum at - say - 3

    kHz

    These peaks corresponds

    to

    the resonance frequencies of the eigenmodes A01 T1, C3, C4, and a

    mode F yet not mapped.

    The 3-kHz hill corresponds mainly to the bridge

    resonance (Alonso Moral Jansson, 1982), although oth r contructimal

    details may affect it (Hutchins, personal communication).

    Violins for the investigation

    For the investigation we selected violins from a violin makers'

    competition,

    FIOG80, arranged by the Nordisk Violinbyggareforening .

    The 77 violins of the competition had been tested and given tonal quali-

    ty

    pants by two professional violin players regarding evenness,

    volume,

    and brilliance of tones together with playability.

    We selected

    24

    vie

    lins covering the full range of ratings, see Table I. The

    violins were

    grouped in three classes after quality points in order

    to

    make campari-

    sons possible between group averages. In addition,

    a concert violin

    labelled

    ndrea

    Guarneri (certificate from amma Sohn gives Fran-

    es o Rugeri,

    Cremona approx 1690 as maker, place and year of making)

    was investgated. Thus

    ur

    investigation included a total of 25 violins,

    24 quality-rated violins, and a concert violin.

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    ON ERT VIOLIN

    Fig.

    2.

    Input

    admittance at

    the

    bass bar side

    of

    the

    Andrea Guameri violin.

    TABLE

    I.

    Violins of the investigation: Types of violins, tonal

    quality points

    TQ

    max=80), and number of violins

    class limits

    selected

    by

    authors).

    Types of violins

    TQP

    nLOnber

    Class

    I

    72 62 1

    Class I

    6

    50

    7

    Class

    I

    48 32

    7

    Andrea Guarneri

    concert violin 1

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    Investiuationmetho

    For the present investigation it was decided to record the input

    admittance in two positions on top of the violin bridge, just outside

    the

    G-

    and E-strings, cf. Fig. 3.

    In

    both cases the input admittances

    were recorded in perpendicular to the top plates of the violins. Fur-

    thermore, it was decided to accurately measure the peak frequencies of

    four resonances, AO, T1,

    C3

    and C4. The corresponding peak levels were

    generally measured and noted too. The long term stability of the meas-

    urements were controlled

    by

    repeated calibration every hcur.

    The measured peak frequencies and levels (average and standard

    deviations) for the AO, T1, C3, and C4 peaks are given in Table

    11.

    When

    the Tl-peak consisted of a double or a triple peak,

    the peak of the

    highest level was selected to represent the T1 resonance.

    Analyzed acoustical parameters

    Three

    types of acoustical properties and their possible relations

    with tonal qualities were tested. First we tested relations between

    tonal quality and resonance frequencies of the AO, T1, C3, and C4

    Secondly we tested relations between quality and levels: below 1 k b the

    levels of the AO, T1, C3, and C4 peaks and above 1 kHz the levels

    averaged in critical bands of hearing, Bark. Finally we tested relations

    beween quality points and level differences bass bar sound post

    sides. The importance of different acoustical properties were tested,

    mainly by calculating the correlation between their acoustical meas-

    ures and given tonal quality points for each violin. In some cases a

    first study was done

    by

    comparing averages of classes.

    Calculated correlations, for instance, average frequencies of the

    different classes,

    showed a somewhat astonishing result. The

    A arsd

    T1

    peaks of the violins of class I

    and

    class

    111

    have higher resonance

    frequencies than class 11 . This means that one should not expect a

    simple correlation between tonal quality and

    resonance frequencies. For

    A there is a relative

    g o

    correlation (correlation coefficient ~0.45)

    between low frequencies and high tonal quality for class

    I

    but small

    (~0.12) or all three classes taken together. The same trend was found

    for several parameters.

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    L FT

    RI HT

    Fig. 3. Positions and directions

    of input admittance meas-

    wements

    Table

    11

    Measured frequencies and levels of resonance peaks,

    average and standard deviations 0

    dB

    corresponds to 3 s/kg).

    Peak

    A0 T1 C3 C

    Average frequency Hz) 272 403 500

    686

    Standard deviation Hz) 11 22 27 54

    Average level dB)

    -35 -24 -27 29

    Standard deviation

    a)

    4

    4

    3

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    obtained for the T1 and the C4 levels, the steps T1 to C3 and C3 to C4.

    Moderate correlations approx. 0.2) are obtained for the A0 level, the

    level step A0 to T1, and the equality of steps.

    High T1 level, large

    downward step T1 to C3

    large upward step C3 to C4,

    nd

    a large average

    step are favorable. A high A level,

    a large step A0

    to

    T1, nd equality

    of levels are favorable, but not as clear as previously mentimed

    param-

    eters.

    The calculated correlations between levels, averaged

    in

    Bark bands,

    and tonal quality are given in Fig

    4.

    The calculations

    indicate that

    low levels are favorable between 10 to 15 Bark and above 18 Bark a

    correlation of approx 0.4).

    3. Level differences between bass bar nd sound post sides

    For frequencies below the C4 peak the input admittance is higher

    for the bass bar side than for the sound post side, cf. Fig.

    5.

    Out of

    the 25 violins 20 have, say 5 10 dB, higher levels at the bass bar

    side, three less clear difference, one approximately the same level,

    nd

    only one with lower level at the bass bar side. For higher frequencies

    the inadmittance levels tend to be the same for both sides. Possible

    relations between tonal quality nd balance bass

    bar

    sound post sides

    were investigated.

    The following correlations were found between quality and level

    differences bass

    bar

    sound post sides: H.32 for T1, 0.21 for

    C3 and

    0.36 for the average of T1 and C3 A0 is not measurable at sound post

    side). Furthermore, a small level difference between the two sides is

    favorable for C4 ~0.42).

    For frequencies above 1.4 kHz small level differences seem favor-

    able in absolute values, ~0.14or 1.4 to 10 kHzI r=0.17 for 1.4 to 3

    kHzI and ~ 0.08or 3 to 10 kHz).

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    INPUT ADMITTANCE

    LEVEL 10

    d ~ / d i v

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    and given tonal quality points

    is 0.39 for all violins,

    0.46 for the

    nine best violins.

    Acoustical parameter four, AP4:

    he discrepancies between input admittance levels calculatedas

    the standard deviation) from 1.4 to 3 kHz A small summed discrepancy is

    favorable. The correlation-coefficient between this acoustical parameter

    and

    given tonal quality points is 0.17

    nd

    0.19, respectively.

    In extensive experiments with violins for many years, including

    amysis,

    making

    nd

    designing, Saunders, Hutchins and Schelleng found

    that two resonances, the Helmholtz and the Main ood resonances, fall

    close to the open middle strings in good violins, Hutchins 1980). The

    peak level, used in this investigation, is a measure that combines

    efficency of driving and resonance amplification,

    and

    gives thus cnly

    an

    indication of the properties outside the resonance frequency range as,

    for instance, in

    Bark

    bands. Still, the previous findings by Gabriels-

    son and Jansson l979), cf. Fig. 4, indicate that a high AO, T1, and C4

    are favorable.

    Both

    the present investigation and that by Gabrielsson

    and Jansson suggest that C3 in isolation is not important for the quali-

    ty*

    The correlation between tonal quality

    and

    levels

    in Bark bands do

    not agree in the present investigation and that by Gabrielsson and

    Jansson. Possibly the differences derives from a combination of effec-

    tive radiation and low driving level. The AP3 criterion may, however,

    fit well also in the previous investigation, i.e., the favorable large

    level increase is not contradicted.

    Thus the suggested parameters are reasonable, but not fully in

    agreement with previous findings. Furthermore, they do not cover all

    possible differences between violins. The suggested parameters can,

    however, be tested on the investigated 24

    violins, and thereby a measure

    of goodness for the suggested parameters is obtained.

    The four acoustical parameters were weighted and summed according

    to the formula to an Acoustical Quality Point, AQP

    AQP 6x 0.6xAP1 0.4 AP2 AP3

    -4

    27)

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    TON L QU LITY POINTS

    Fig. 6

    Iielation between Acoustical Quality Points,

    AQP:s and Tonal Quality Points, W:s: Ap

    proxhte

    r e la t io n ( f u l l l i n e ) ,

    separate

    vio-

    lins marked

    with

    circles

    th Guameri v io l in

    w i t AG and

    divergent vio li ns with squares.

    Class

    limits m r k e d I

    11 and 111.

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    investigation. Such gross parameters, as balance-unbalance between the

    bass bar and the sound post sides, and levels from 900 to 1300 Hz are

    not included.

    Four of the five divergent violins score poorly in these parame-

    ters. Two have the very lowest levels from 900 to 1300

    Hz

    and two other

    have exceptionally small level differences between the bass bar and the

    soun

    post sides for, he T1 and the C3 peaks.

    Possibly, these proprties give the serious divergencies not ac-

    counted for. The fifth violin has a split, a double, T1 peak. Several

    violins have this and it does not seem likely that this defect ex-

    plains the

    P

    divergency from the prediction.

    Conclusions

    Simple calculations have shown that the levels

    of

    resonances la-

    belled AO T1, and C4 correlates with tonal quality. Furthermore, pro-

    perties around the frequency of the main bridge resonance correlates

    with the quality. For low frequencies, below C4, the bridge foot

    on

    the

    bass bar side is most efficient in driving the violin, while for higher

    frequencies both bridge feet are abcut equally efficient. The difference

    at low frequencies and the equality at high frequencies also correlate

    with tonal quality.

    function, weighting together levels of the T1, C3, C4 peaks

    and

    average levels from 1 to 3 kHz, predicts the tonal quality well for 19

    of the 24 violins, and especially well for the six highest rated vio-

    lins. The C3 level does not correlate separately with the tonal quality,

    but increases the correlation noticeably together with the T1 and C4

    peaks. This makes us believe that we have traced major parameters of

    quality, not only for the nineteen tested violins, but for the violin n

    general.

    Thus, this investigation has given the following answers to the

    introductory questions:

    1. The resonance peaks T1, C3, and C4, and a hill around 3 kHz are the

    most important properties of the input admittance. The resonance

    peaks

    r

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    STL-QPSR 2-3/1982

    should be equally high when excited at the bass

    bar

    side. The favorable

    high peak levels indicate: 1) that stiff and light wood with low inter-

    nal friction is favorable, and

    2)

    that the properties in top and back

    should match (C3 and C4). The 3 kHz hill should have

    a

    large level

    increase from 1.4 to

    3

    kHz, and it should be equallly well driven from

    the bass bar and the sound post sides. This indicates that a well

    developed bridge resonance and a good balance

    between the bass bar and

    sound post sides are important.

    2.

    These properties predict tonal quality reasonably well (~0.76) or

    all violins, very well (r=0.96) with five divergent violins excluded.

    The rather high correlation between tonal quality and low frequency

    properties indicates that good low frquency properties may predict

    good

    high frequency properties to a large extent. Some additional factor

    must, however be important as the five violins represent large divergen-

    cies from predictions.

    This investigation was possible through the cooperation of ''KbNordisk

    Violinbyggareforening

    and

    Mr. Gunnar Mattsson. The measurements were

    made at the Stockholm Music Museum. Lars Frydgn

    lent us his Guarneri

    violin for the investigation. This support

    and

    cooperation is gratefully

    acknowledged.

    Alonso Mral, J.

    and Jansson,

    E.V.

    (1982):

    Eigammdes, nput admittance, and

    fhctidn of

    the

    violin , Acustica 50, pp. 329-337.

    -

    Gabrielsson,

    A

    and Jansson, E.V. (1979): Long-tim-average-spectra and rated

    qualities of twnty-two violins , Acustica 42,

    pp

    47-55.

    -

    Hutchins, C.M. (1980):

    The new violin family ,pp 182-203 in Sound Genera-

    tion in Winds, Strings, Computers, faoyal Shedish Acaderry of Music, Stockholm.

    Hutchins, C. M. 1980)

    Tuning of violin plates , ~nSound rkneration in

    winds,

    Strings, Camputers Royal Swedish Acadq of Music, Stockholm, Fig.

    Hutchins, C.M., personal comication.

    Reinicke W. 9

    :

    ijbertraWgseigenschaften des Streichins~tenstegs

    Dr.?hesis, Technische Universitat, Berlin 1972; shortened version in Catgut

    Ac

    Soc Newsletter

    No.

    19, pp 26-34.