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Flute acoustics: measurement, modelling and design - School of ...

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70 CHAPTER 5. IMPEDANCE SPECTRA OF THE FLUTE AND CLARINET<br />

The position <strong>of</strong> the cork in the head joint <strong>of</strong> the modern flute was set at 17.5 mm from the<br />

centre <strong>of</strong> the embouchure hole, <strong>and</strong> the tuning slide was set at 4 mm. These are typical values<br />

used by flutists playing at st<strong>and</strong>ard pitch. For the classical flute the cork was set at 19 mm <strong>and</strong><br />

the tuning slide at 12.8 mm (this was determined empirically by the maker Terry McGee as the<br />

correct position for the flute to play at A 440, although his playing style may not be typical).<br />

All st<strong>and</strong>ard <strong>and</strong> many alternative <strong>and</strong> multiphonic fingerings were measured for the modern<br />

flute with both C <strong>and</strong> B foot. Classical flutes currently available differ widely in <strong>design</strong> <strong>and</strong><br />

hence no authoritative st<strong>and</strong>ard exists. For the <strong>measurement</strong>s in this chapter, the fingerings<br />

given in Porter (2005) were used. In all cases the fingerings are shown on each graph <strong>of</strong> the<br />

results.<br />

The impedance <strong>of</strong> the clarinets were measured over the range from E3 to E7 (written) for all<br />

st<strong>and</strong>ard fingerings <strong>and</strong> a selection <strong>of</strong> multiphonic <strong>and</strong> alternate fingerings.<br />

5.2.2 The impedance spectrometer<br />

The details <strong>of</strong> the impedance spectrometer have been described in Chapter 3. The impedance<br />

spectra are measured between 200 Hz <strong>and</strong> 4 kHz for the flute <strong>and</strong> between 120 Hz <strong>and</strong> 4 kHz<br />

for the clarinet (a range that encompasses the fundamental frequency <strong>of</strong> all <strong>of</strong> the instruments’<br />

notes <strong>and</strong> includes their cut <strong>of</strong>f frequencies).<br />

A 7.8 mm inner diameter brass <strong>measurement</strong> head is used in addition to the 15 mm head<br />

described in Chapter 3. In all other respects this impedance head is identical to the 15 mm<br />

version. The 7.8 mm impedance head may be used to measure the input impedance <strong>of</strong> flutes<br />

<strong>and</strong> clarinets as the outlet fits within the embouchure hole <strong>of</strong> a flute <strong>and</strong> the mouthpiece <strong>of</strong> a<br />

clarinet. (The cross-sectional area <strong>of</strong> this head is comparable with the area through which air<br />

flows between clarinet <strong>and</strong> mouthpiece, i.e. the gap between reed <strong>and</strong> mouthpiece. It is also<br />

comparable with the area <strong>of</strong> the hole at the embouchure <strong>of</strong> a flute when played.)<br />

The impedance head is calibrated as described in Chapter 3 using a solid stop (infinite impedance<br />

load) <strong>and</strong> a 7.8 mm semi-infinite pipe.<br />

5.2.3 Attachment <strong>of</strong> instruments<br />

The flutes were coupled to the impedance head as in Wolfe et al. (2001a) (see also Smith et al.<br />

1997) with a concave attachment matching the curvature <strong>of</strong> the embouchure striker plate (Figure<br />

5.1 (a)). The thickness <strong>of</strong> the concave attachment was accounted for in calibration, so that<br />

the reference plane for impedance <strong>measurement</strong>s was situated at the embouchure hole. For<br />

the spectra presented in this chapter <strong>and</strong> in Appendix A the impedance <strong>of</strong> a stub <strong>of</strong> length<br />

5 mm <strong>and</strong> diameter 7.8 mm was added to the measured impedance to account (at least approximately)<br />

for the radiation impedance baffled by the player’s face <strong>and</strong> lips (see Wolfe et al.<br />

2001a). The impedance was thus measured upstream <strong>of</strong> a discontinuity, since the diameter <strong>of</strong><br />

the embouchure hole on the outside <strong>of</strong> the instrument is greater than 7.8 mm for both headjoints<br />

measured. This measured impedance will be different to the impedance that would be<br />

measured by an impedance head with diameter matched to the input radius <strong>of</strong> the instrument.<br />

However, in the played instrument a similarly sized discontinuity exists, since the player’s lips<br />

occlude the embouchure hole to a significant extent.

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