2015
DOI: 10.3813/aaa.918912
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Matching of Fundamental Modes at a Junction of a Cylinder and a Truncated Cone; Application to the Calculation of Some Radiation Impedances

Abstract: The problem of the junction between a cylinder and a truncated cone at frequencies below the first cutoff of the cylinder is investigated, in particular for the case of acute angles. An analytical model of the matching of a cylinder and a truncated cone is derived for the general case of a cone of finite length having a known terminal impedance. When the cone is infinite and the angle is right, the problem is similar to the classical problem of a tube radiating in an infinite baffle. The model is based on a ge… Show more

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Cited by 7 publications
(4 citation statements)
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“…The effect of the plane is interpreted by Dalmont as a correction ∆m r of the radiation inertance without plane m r0 (unflanged pipe). If the plane distance h p is short in comparison with the radius opening r o (h p ≪ r o ), the inertance correction is approximately proportional to the inverse of this distance: The junction of a cylinder and a truncated cone, studied by Kergomard et al [21], is also comparable to the problem studied here. Indeed, the case where the truncated cone is semi-infinite is equivalent to a cylinder surrounded by an inclined wall (Fig.…”
Section: Simplification and Generalizationsupporting
confidence: 56%
See 1 more Smart Citation
“…The effect of the plane is interpreted by Dalmont as a correction ∆m r of the radiation inertance without plane m r0 (unflanged pipe). If the plane distance h p is short in comparison with the radius opening r o (h p ≪ r o ), the inertance correction is approximately proportional to the inverse of this distance: The junction of a cylinder and a truncated cone, studied by Kergomard et al [21], is also comparable to the problem studied here. Indeed, the case where the truncated cone is semi-infinite is equivalent to a cylinder surrounded by an inclined wall (Fig.…”
Section: Simplification and Generalizationsupporting
confidence: 56%
“…It is only valid for acute cones (θ ≤ π).If the angle of the cone is sufficiently wide, this expression can be approximated for low frequencies by the expression of Eq. (2), leading to an inertance m (cone) r and a coefficient ζ (cone) [21]:…”
Section: Simplification and Generalizationmentioning
confidence: 99%
“…Thus, if this volume is set by means of a cylindrical mouthpiece, a new parameter is introduced (either the length y of the mouthpiece or its cross section area S m ) and this leads to the first model, described in the present section. The matching of the plane waves in the cylindrical mouthpiece with the spherical waves in the cone can be done with an excellent precision, 22 but for the present purpose, the continuity of the flow rate and mean pressure is assumed between the output of the cylinder and the input of the cone. Fig.…”
mentioning
confidence: 99%
“…At the open end, the radiation is modeled by the dimensionless radiation impedance Z R given by Silva et al [23] (see also [24]) as a fraction of two polynomials N R (ω)/D R (ω). Then, accounting for the transfer matrix between the input and the output of the pipe, the dimensionless input impedance can be expressed as the ratio of two functions Z(ω) = N (ω)/D(ω), N and D having zeros only (i.e., no poles)…”
Section: Example: the Cylindrical Pipementioning
confidence: 99%