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validation of caa prediction of noise radi- ated from turbofan intakes

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16 th International Congress on Sound and Vibration, Kraków, Poland, 5–9 July 2009<br />

4<br />

TCS<br />

Baffle<br />

Figure 3. Intake <strong>of</strong> 1/3 scale model fan rig with acoustic baffle and Turbulence Control Screen (TCS).<br />

4. Mode Detection Data<br />

Transducers ring Intake barrel<br />

Transition casing<br />

Fan case<br />

Cylindrical section<br />

The measured data obtained <strong>from</strong> the pressure transducers mounted in the mode detection ring<br />

are converted to wall sound pressure levels <strong>of</strong> the circumferential duct modes using the method dedescribed<br />

by Rademaker et al. 7 .<br />

5. Tone Predictions at the Blade Passing Frequency (BPF)<br />

Spinner<br />

Predictions at BPF were performed for the fan rig described above. Predictions <strong>of</strong> the far-field<br />

sound pressure level (SPL) were made for hard-walled and lined configurations at a number <strong>of</strong> fan<br />

speeds. The source is assumed to consist <strong>of</strong> a multimodal base and a single BPF tone at higher fan<br />

speeds. The distribution <strong>of</strong> acoustic power in the multimode source is modelled by assuming equal<br />

power per mode for all cut-on modes. When the fan tip speed is supersonic, an additional rotorlocked<br />

component is included which corresponds to the first <strong>radi</strong>al BPF tone for which (in this<br />

case) m = 24. All <strong>of</strong> the cut-on modes which are included in the mutimodal content, as well as the<br />

'm = 24' mode, are assumed to be uncorrel<strong>ated</strong>. At subsonic tip speeds (50% to 70% fan speed), the<br />

‘m = 24’ mode is cut-<strong>of</strong>f and the source model then consists only <strong>of</strong> the multimodal, equal power,<br />

component. Above 80% fan speed however, the ‘m = 24’ mode is cut-on and the fan source contains<br />

both contributions. In all cases and at all frequencies, far-field directivities are computed for<br />

each <strong>of</strong> the modes present at the fan plane, and these are summed in the far field as contributions<br />

<strong>from</strong> uncorrel<strong>ated</strong> sources. The sound pressure level is then calcul<strong>ated</strong> as;<br />

p 1<br />

SPL = 20. log10<br />

. , (1)<br />

2 pref<br />

where p 2 is the root mean square pressure and Pref is a reference pressure, 2.10 -5 Pa.<br />

Measured data are taken for the case <strong>of</strong> a hard (i.e. no liners) and a lined intake. The hardwalled<br />

case is used to calibrate the source model. Fig. 4 shows mode detection data for a hardwalled<br />

intake taken <strong>from</strong> the ring <strong>of</strong> transducers close to the outlet flare (see Fig. 3). The measured<br />

SPL on the wall is sampled at a frequency which corresponds, at each fan operating speed, to an<br />

'Engine Order' (EO) <strong>of</strong> 24, corresponding to BPF for a 24 bladed fan. At each fan speed the measured<br />

data is decomposed into components corresponding to each circumferential mode number m.<br />

Fan

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