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

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CHAPTER 3. MEASURING ACOUSTIC IMPEDANCE 50<br />

(a)<br />

10 6<br />

10 4<br />

10 8<br />

(b)<br />

10 6<br />

|Z| (Pa s m -3 )<br />

10 4<br />

10 8<br />

(c)<br />

10 6<br />

10 4<br />

10 8<br />

(d)<br />

10 6<br />

|(Z meas - Z theo ) / Z theo |<br />

10 8 (e)<br />

10 4<br />

10 0<br />

10 -2<br />

10 -4<br />

0 1 2 3 4<br />

Frequency (kHz)<br />

Figure 3.5: The input impedance for a closed 15 mm pipe, 200 mm long. In (a) <strong>and</strong> (b) the signals<br />

from microphones 2 <strong>and</strong> 3 were multiplied by 1.2 <strong>and</strong> 0.8 respectively to deliberately introduce<br />

errors. The impedance was measured before calibration (a) <strong>and</strong> after calibrating using<br />

one known load (b). In (c) the impedance is given for matched microphones before (grey, solid<br />

line) <strong>and</strong> after (black, dotted line) calibration with two known loads, <strong>and</strong> in (d) the calibrated<br />

<strong>measurement</strong> from (c) (black, dotted line) is compared with the theoretical impedance for an<br />

ideal tube (grey, solid line). The fractional difference between this theory <strong>and</strong> the <strong>measurement</strong><br />

is shown in (e).

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