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The sound field of a rotating monopole in a plug flow

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An Erratum to this article was published on 01 January 2018

This article has been updated

Abstract

A theoretical study is performed on the sound field generated by a rotating point monopole in a jet flow, the mixing layer of which is simulated by a velocity discontinuity. Its sound in the far field is compared to the sound field generated by a rotating monopole in a uniform flow in the absence of a velocity discontinuity, which makes it possible to estimate the size of the sound refraction effect.

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Change history

  • 01 March 2018

    The second equation in (9) should read:

    $$\begin{array}{*{20}c} {\tilde p_m = \left[ {C_m + \frac{{i\pi }} {2}Q_m H_m^{(1)} \left( {\Gamma _2 r_0 } \right)} \right]J_m (\Gamma _2 r)} \\ { + \left[ {D_m - \frac{{i\pi }} {2}Q_m J_m \left( {\Gamma _2 r_0 } \right)} \right]H_m^{(1)} \left( {\Gamma _2 r} \right),} \\ {r_0 \leqslant r \leqslant R_0 .} \\ \end{array}$$
  • 01 March 2018

    The second equation in (9) and Equation (21) were erroneous.Figure 2 does not change in this case.

  • 01 March 2018

    The second equation in (9) and Equation (21) were erroneous.Figure 2 does not change in this case.

  • 01 March 2018

    The second equation in (9) and Equation (21) were erroneous.Figure 2 does not change in this case.

  • 01 March 2018

    The second equation in (9) and Equation (21) were erroneous.Figure 2 does not change in this case.

  • 01 March 2018

    The second equation in (9) and Equation (21) were erroneous.Figure 2 does not change in this case.

  • 01 March 2018

    The second equation in (9) and Equation (21) were erroneous.Figure 2 does not change in this case.

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Correspondence to I. V. Belyaev.

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Original Russian Text © I.V. Belyaev, 2016, published in Akusticheskii Zhurnal, 2016, Vol. 62, No. 4, pp. 457–461.

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Belyaev, I.V. The sound field of a rotating monopole in a plug flow. Acoust. Phys. 62, 462–466 (2016). https://doi.org/10.1134/S1063771016040059

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