4 research outputs found
ΠΠ‘ΠΠΠΠΠΠΠ‘Π’Π ΠΠΠΠΠ’Π ΠΠΠΠ₯ΠΠΠΠΠΠ£Π‘Π’ΠΠ§ΠΠ‘ΠΠΠΠ ΠΠ ΠΠΠΠ ΠΠΠΠΠΠΠΠ― ΠΠΠΠ ΠΠΠ Π¦ΠΠΠΠΠΠ ΠΠ§ΠΠ‘ΠΠΠΠ ΠΠ¬ΠΠΠΠΠΠ ΠΠΠΠ§ΠΠ‘ΠΠΠΠ ΠΠΠΠ£Π§ΠΠ’ΠΠΠ―ΠΠ Π‘ ΠΠΠ£Π’Π ΠΠΠΠΠΠ ΠΠΠ ΠΠΠΠΠ Π Π‘ΠΠ‘Π’ΠΠΠ ΠΠΠΠ‘ΠΠΠ₯ Π‘ΠΠ‘Π’ΠΠ
The problem of sound emission is considered by a system formed from cylindrical piezoceramic radiators with internal acoustically soft screens. Longitudinal axis of emitters lie in one plane. This system is characterized by the interaction of electric, mechanical and acoustic fields in the process of conversion electrical energy to acoustical energy and acoustic fields in the process of forming them in the environments. The purpose of the work is to determine the peculiarities of the electromechanical acoustic transformation of energy by cylindrical piezoceramic radiators with internal screens in the composition of flat systems, taking into account all types of interaction.The research was carried out by the method of bound fields in multiply connected domains with the use of addition theorems for the cylindrical wave functions. The physical fields arising from the emission of sound by such a system are determined by the joint solution of the system of differential equations: the wave equation; equations of motion of thin piezoceramic shells with circular polarization in displacements; the equations of forced electrostatics for piezoceramics at given boundary conditions, the conditions of conjugation of fields at the boundaries of the division of domains and electric conditions.The solution of the problem is reduced to the solution of an infinite system of linear algebraic equations with respect to unknown coefficients of field expansions.An analysis of the results of numerical calculations, performed on the basis of the obtained analytical relations, called to establish a number of features in the electromechanical acoustic transformation of energy by emitters in the composition of flat systems. They include: the role of acoustic interaction in the process of energy conversion; determination of the mechanism of quantitative assessment of the influence of interaction on these processes; the dependence of the degree of violation of the radial symmetry of the acoustic loading of the emitters on the amount of acoustic interaction; the appearance of multimodality of the mechanical field of emitters in the structure of the plane system and the dependence of the redistribution of energy between all modes on the degree of disturbance of the radial symmetry of the acoustic loading of the emitters.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Π° Π·Π°Π΄Π°ΡΠ° ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π·Π²ΡΠΊΠ° ΠΏΠ»ΠΎΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠΎΠΉ, ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΈΠ· ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ Ρ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈ ΠΌΡΠ³ΠΊΠΈΠΌΠΈ ΡΠΊΡΠ°Π½Π°ΠΌΠΈ. ΠΡΠΎΠ΄ΠΎΠ»ΡΠ½ΡΠ΅ ΠΎΡΠΈ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½Ρ ΠΈ Π»Π΅ΠΆΠ°Ρ Π² ΠΎΠ΄Π½ΠΎΠΉ ΠΏΠ»ΠΎΡΠΊΠΎΡΡΠΈ. Π£ΠΊΠ°Π·Π°Π½Π½Π°Ρ ΡΠΈΡΡΠ΅ΠΌΠ° Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΠ΅ΡΡΡ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
, ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»ΡΠΌΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π² Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΡΡ ΠΈ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΎΠΊΡΡΠΆΠ°ΡΡΠΈΡ
ΡΡΠ΅Π΄Π°Ρ
. Π¦Π΅Π»ΡΡ ΡΠ°Π±ΠΎΡΡ ΡΠ²Π»ΡΠ»ΠΎΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠ΅ΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ
Π°Π½ΠΎΠ°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»ΡΠΌΠΈ Ρ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌΠΈ ΡΠΊΡΠ°Π½Π°ΠΌΠΈ Π² ΡΠΎΡΡΠ°Π²Π΅ ΠΏΠ»ΠΎΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ Ρ ΡΡΠ΅ΡΠΎΠΌ Π²ΡΠ΅Ρ
Π²ΠΈΠ΄ΠΎΠ² Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈΡΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ²ΡΠ·Π°Π½Π½ΡΡ
ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΌΠ½ΠΎΠ³ΠΎΡΠ²ΡΠ·Π½ΡΡ
ΠΎΠ±Π»Π°ΡΡΡΡ
Ρ ΠΏΡΠΈΠ²Π»Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΎΡΠ΅ΠΌ ΡΠ»ΠΎΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΠΎΠ»Π½ΠΎΠ²ΡΡ
ΡΡΠ½ΠΊΡΠΈΠΉ. Π€ΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠΎΠ»Ρ, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΠ΅ ΠΏΡΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠΈ Π·Π²ΡΠΊΠ° ΡΠ°ΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΠΎΠΉ, ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ ΠΏΡΡΠ΅ΠΌ ΡΠΎΠ²ΠΌΠ΅ΡΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΠΈΡΡΠ΅ΠΌΡ Π΄ΠΈΡΡΠ΅ΡΠ΅Π½ΡΠΈΠ°Π»ΡΠ½ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ: Π²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ; ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΠ±ΠΎΠ»ΠΎΡΠ΅ΠΊ Π² ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΡΡ
; ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π²ΡΠ½ΡΠΆΠ΄Π΅Π½Π½ΠΎΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΡΡΠ°ΡΠΈΠΊΠΈ Π΄Π»Ρ ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΠΊΠΈ ΠΏΡΠΈ Π·Π°Π΄Π°Π½Π½ΡΡ
Π³ΡΠ°Π½ΠΈΡΠ½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
, ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΡΠΎΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΠΎΠ»Π΅ΠΉ Π½Π° Π³ΡΠ°Π½ΠΈΡΠ°Ρ
ΡΠ°Π·Π΄Π΅Π»Π° ΠΌΠ½ΠΎΠ³ΠΎΡΠ²ΡΠ·Π½ΡΡ
ΠΎΠ±Π»Π°ΡΡΠ΅ΠΉ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
.Π Π΅ΡΠ΅Π½ΠΈΠ΅ Π·Π°Π΄Π°ΡΠΈ ΡΠ²Π΅Π΄Π΅Π½ΠΎ ΠΊ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π±Π΅ΡΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
Π°Π»Π³Π΅Π±ΡΠ°ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π½Π΅ΠΈΠ·Π²Π΅ΡΡΠ½ΡΡ
ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠ² ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΠΉ ΠΏΠΎΠ»Π΅ΠΉ Π² ΡΡΠ΄Ρ ΠΏΠΎ Π²ΠΎΠ»Π½ΠΎΠ²ΡΠΌ ΡΡΠ½ΠΊΡΠΈΡΠΌ.ΠΠ½Π°Π»ΠΈΠ· ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΡΠΈΡΠ»Π΅Π½Π½ΡΡ
ΡΠ°ΡΡΠ΅ΡΠΎΠ², Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π½ΡΡ
Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΎΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠΉ, ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΡ ΡΡΠ΄ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠ΅ΠΉ Π² ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ΅Ρ
Π°Π½ΠΎΠ°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»ΡΠΌΠΈ Π² ΡΠΎΡΡΠ°Π²Π΅ ΠΏΠ»ΠΎΡΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ. ΠΡΠΈ ΡΡΠΎΠΌ ΡΡΡΠ΅Π½Ρ: Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΏΠΎΠ»Π΅ΠΉ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ; Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ ΠΈ ΡΠΈΡΡΠ΅ΠΌΡ ΠΏΠΎ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠΌΡ ΠΏΠΎΠ»Ρ; ΡΡΠ΅ΠΏΠ΅Π½Ρ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΡΠ°Π΄ΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π°Π³ΡΡΠΆΠ΅Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ ΠΎΡ Π²Π΅Π»ΠΈΡΠΈΠ½Ρ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ; ΠΌΠ½ΠΎΠ³ΠΎΠΌΠΎΠ΄ΠΎΠ²ΠΎΡΡΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠΎΠ»Π΅ΠΉ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ Π² ΡΠΎΡΡΠ°Π²Π΅ ΠΏΠ»ΠΎΡΠΊΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΠΈ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΏΠ΅ΡΠ΅ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΠΌΠ΅ΠΆΠ΄Ρ ΠΌΠΎΠ΄Π°ΠΌΠΈ ΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΠΉ ΠΎΡ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ Π½Π°ΡΡΡΠ΅Π½ΠΈΡ ΡΠ°Π΄ΠΈΠ°Π»ΡΠ½ΠΎΠΉ ΡΠΈΠΌΠΌΠ΅ΡΡΠΈΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π°Π³ΡΡΠΆΠ΅Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Π΅ΠΉ
ΠΠ½Π°Π»ΡΠ· Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΠ΅ΠΉ ΡΡΠ·ΠΈΡΠ½ΠΈΡ ΠΏΠΎΠ»ΡΠ², ΡΠΎ ΡΡΠ²ΠΎΡΡΡΡΡΡΡ ΡΠΈΡΡΠ΅ΠΌΠ°ΠΌΠΈ ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ ΡΠΈΠ»ΡΠ½Π΄ΡΠΈΡΠ½ΠΈΡ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΡΠ²Π°ΡΡΠ², ΡΠΎΠ·ΡΠ°ΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ±Π»ΠΈΠ·Ρ Π°ΠΊΡΡΡΠΈΡΠ½ΠΎΠ³ΠΎ Π΅ΠΊΡΠ°Π½Ρ Ρ Π²ΠΈΠ³Π»ΡΠ΄Ρ ΠΏΠΎΡΠΎΠΆΠ½ΡΠΎΠ³ΠΎ ΠΏΡΡΠΆΠ½ΠΎΠ³ΠΎ ΡΡΠ»ΡΠ½ΡΡΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΡΠ»Π°
The thesis deals with the analysis of numeral results of physical characteristics of connected fields which appear in pies ceramic cylindrical transformations of round and arch cylindrical lattices with resilient acoustic cylindrical screen in their inner laprobe together with interaction of flat acoustic waves depending on parameters of transducers, lattices and waves. Conformity to natural laws of this interaction on acoustic, mechanic and electric fields of lattices and transformations were determinedΠΡΠΏΠΎΠ»Π½Π΅Π½ ΡΠΈΡΠ»Π΅Π½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΡΠ²ΡΠ·Π°Π½Π½ΡΡ
ΠΏΠΎΠ»Π΅ΠΉ, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΡ
Π² ΠΏΡΠ΅Π·ΠΎΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»ΡΡ
ΠΊΡΡΠ³ΠΎΠ²ΡΡ
ΠΈ Π΄ΡΠ³ΠΎΠ²ΡΡ
ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅ΡΠ΅ΡΠΎΠΊ Ρ ΡΠΏΡΡΠ³ΠΈΠΌ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠΊΡΠ°Π½ΠΎΠΌ Π² ΠΈΡ
Π²Π½ΡΡΡΠ΅Π½Π½Π΅ΠΉ ΠΏΠΎΠ»ΠΎΡΡΠΈ ΠΏΡΠΈ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΈ ΡΠ΅ΡΠ΅ΡΠΎΠΊ Ρ ΠΏΠ»ΠΎΡΠΊΠΈΠΌΠΈ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ Π²ΠΎΠ»Π½Π°ΠΌΠΈ, Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Π΅ΠΉ,Β ΡΠ΅ΡΠ΅ΡΠΎΠΊ Β ΠΈΒ Π²ΠΎΠ»Π½. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΒ ΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ Β ΡΡΠΎΠ³ΠΎ Β Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ Β Π½Π° Β Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅, ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠΎΠ»Ρ ΡΠ΅ΡΠ΅ΡΠΎΠΊ ΠΈ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Π΅ΠΉ.ΠΠΈΠΊΠΎΠ½Π°Π½ΠΎ ΡΠΈΡΠ΅Π»ΡΠ½ΠΈΠΉ Π°Π½Π°Π»ΡΠ· ΡΡΠ·ΠΈΡΠ½ΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ ΠΏΠΎΠ²'ΡΠ·Π°Π½ΠΈΡ
ΠΏΠΎΠ»ΡΠ², ΡΠΎ Π²ΠΈΠ½ΠΈΠΊΠ°ΡΡΡ Π² ΠΏ'ΡΠ·ΠΎΠΊΠ΅ΡΠ°ΠΌΡΡΠ½ΠΈΡ
ΡΠΈΠ»ΡΠ½Π΄ΡΠΈΡΠ½ΠΈΡ
ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΡΠ²Π°ΡΡΠ² ΠΊΡΡΠ³ΠΎΠ²ΠΈΡ
Ρ Π΄ΡΠ³ΠΎΠ²ΠΈΡ
ΡΠΈΠ»ΡΠ½Π΄ΡΠΈΡΠ½ΠΈΡ
ΡΠ΅ΡΡΡΠΎΠΊ Π· ΠΏΡΡΠΆΠ½ΠΈΠΌ Π°ΠΊΡΡΡΠΈΡΠ½ΠΈΠΌ ΡΠΈΠ»ΡΠ½Π΄ΡΠΈΡΠ½ΠΈΠΌ Π΅ΠΊΡΠ°Π½ΠΎΠΌ Π² ΡΡ
Π²Π½ΡΡΡΡΡΠ½ΡΠΎΡ ΠΏΠΎΡΠΎΠΆΠ½ΠΈΠ½ΠΈ ΠΏΡΠΈ Π²Π·Π°ΡΠΌΠΎΠ΄ΡΡ ΡΠ΅ΡΡΡΠΎΠΊ Π· ΠΏΠ»ΠΎΡΠΊΠΈΠΌΠΈ Π°ΠΊΡΡΡΠΈΡΠ½ΠΈΠΌΠΈ Ρ
Π²ΠΈΠ»ΡΠΌΠΈ, Π² Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ Π²ΡΠ΄ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡΠ² ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΡΠ²Π°ΡΡΠ², ΡΠ΅ΡΡΡΠΎΠΊ ΡΠ° Ρ
Π²ΠΈΠ»Ρ. ΠΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ Π·Π°ΠΊΠΎΠ½ΠΎ ΠΌΡΡΠ½ΠΎΡΡΡ ΡΡΡΡ Π²Π·Π°ΡΠΌΠΎΠ΄ΡΡ Π½Π° Π°ΠΊΡΡΡΠΈΡΠ½Ρ, ΠΌΠ΅Ρ
Π°Π½ΡΡΠ½Ρ ΡΠ° Π΅Π»Π΅ΠΊΡΡΠΈΡΠ½Ρ ΠΏΠΎΠ»Ρ Π³ΡΠ°ΡΠΎΠΊ Ρ ΠΏΠ΅ΡΠ΅ΡΠ²ΠΎΡΡΠ²Π°ΡΡΠ²
FEATURES OF ELECTROMECHANICAL ACOUSTIC ENERGY CONVERSION BY CYLINDRICAL PIEZOCERAMIC TRANSDUCERS WITH INTERNAL SCREENS IN COMPOSITION OF FLAT SYSTEMS
The problem of sound emission is considered by a system formed from cylindrical piezoceramic radiators with internal acoustically soft screens. Longitudinal axis of emitters lie in one plane. This system is characterized by the interaction of electric, mechanical and acoustic fields in the process of conversion electrical energy to acoustical energy and acoustic fields in the process of forming them in the environments. The purpose of the work is to determine the peculiarities of the electromechanical acoustic transformation of energy by cylindrical piezoceramic radiators with internal screens in the composition of flat systems, taking into account all types of interaction.The research was carried out by the method of bound fields in multiply connected domains with the use of addition theorems for the cylindrical wave functions. The physical fields arising from the emission of sound by such a system are determined by the joint solution of the system of differential equations: the wave equation; equations of motion of thin piezoceramic shells with circular polarization in displacements; the equations of forced electrostatics for piezoceramics at given boundary conditions, the conditions of conjugation of fields at the boundaries of the division of domains and electric conditions.The solution of the problem is reduced to the solution of an infinite system of linear algebraic equations with respect to unknown coefficients of field expansions.An analysis of the results of numerical calculations, performed on the basis of the obtained analytical relations, called to establish a number of features in the electromechanical acoustic transformation of energy by emitters in the composition of flat systems. They include: the role of acoustic interaction in the process of energy conversion; determination of the mechanism of quantitative assessment of the influence of interaction on these processes; the dependence of the degree of violation of the radial symmetry of the acoustic loading of the emitters on the amount of acoustic interaction; the appearance of multimodality of the mechanical field of emitters in the structure of the plane system and the dependence of the redistribution of energy between all modes on the degree of disturbance of the radial symmetry of the acoustic loading of the emitters
Radiation field angled horn antenna with a piezoceramic transducer with radial polarization
ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΠΈΡΠ΅Π»ΡΠ½ΠΈΠΉ Π°Π½Π°Π»ΡΠ· Π°ΠΊΡΡΡΠΈΡΠ½ΠΈΡ
Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΠ΅ΠΉ ΡΠΈΠ»ΡΠ½Π΄ΡΠΈΡΠ½ΠΎΡ Π°Π½ΡΠ΅Π½ΠΈ Π· ΠΏΠ»ΠΎΡΠΊΠΈΠΌ Π°ΠΊΡΡΡΠΈΡΠ½ΠΎ ΠΌβΡΠΊΠΈΠΌ Π΅ΠΊΡΠ°Π½ΠΎΠΌ, ΡΠΎΠ·ΠΌΡΡΠ΅Π½ΠΈΠΌ Π² Π΄ΡΠ°ΠΌΠ΅ΡΡΠ°Π»ΡΠ½ΡΠΉ ΠΏΠ»ΠΎΡΠΈΠ½Ρ ΡΡ Π²ΠΈΠΏΡΠΎΠΌΡΠ½ΡΠ²Π°ΡΠ°, Π²ΠΈΠΊΠΎΠ½Π°Π½ΠΎΠ³ΠΎ Ρ Π²ΠΈΠ³Π»ΡΠ΄Ρ ΡΠΈΠ»ΠΎΠ²ΠΎΡ ΡΠΈ ΠΊΠΎΠΌΠΏΠ΅Π½ΡΠΎΠ²Π°Π½ΠΎΡ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΡΠΉ. ΠΠΎΡΡΠ²Π½ΡΠ»ΡΠ½ΠΈΠΉ Π°Π½Π°Π»ΡΠ· ΡΠ°ΡΡΠΎΡΠ½ΠΈΡ
Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΠ΅ΠΉ Π·Π²ΡΠΊΠΎΠ²ΠΈΡ
ΠΏΠΎΠ»ΡΠ² Ρ ΠΊΡΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΠ·ΠΏΠΎΠ΄ΡΠ»Π΅Π½Π½Ρ ΠΏΠΎΠ»ΡΠ² Π² Π΄Π°Π»ΡΠ½ΡΠΉ Π·ΠΎΠ½Ρ Π°Π½ΡΠ΅Π½ΠΈ Π΄ΠΎΠ·Π²ΠΎΠ»ΠΈΠ² Π²ΡΡΠ°Π½ΠΎΠ²ΠΈΡΠΈ ΡΡΠ΄ ΡΠΎΠ½ΠΊΠΈΡ
Π΅ΡΠ΅ΠΊΡΡΠ² Ρ ΡΠΎΡΠΌΡΠ²Π°Π½Π½Ρ ΠΏΠΎΠ»ΡΠ², ΡΠΎ Π·Π°Π»Π΅ΠΆΠ°ΡΡ ΡΠΊ Π²ΡΠ΄ ΡΠΈΠΏΡ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π²ΠΈΠΊΠΎΠ½Π°Π½Π½Ρ Π²ΠΈΠΏΡΠΎΠΌΡΠ½ΡΠ²Π°ΡΠ° Π°Π½ΡΠ΅Π½ΠΈ, ΡΠ°ΠΊ Ρ Π²ΡΠ΄ ΡΠΎΠ·ΠΌΡΡΡΠ² ΡΡ Π°ΠΊΡΡΡΠΈΡΠ½ΠΎΠ³ΠΎ Π΅ΠΊΡΠ°Π½Π°.The numerical analysis of the acoustic properties of a cylindrical antenna with a flat acoustically soft baffle located in the diametral plane of its transmitter, made in the form of power or compensated structures was performed. Comparative analysis of the frequency characteristics of the sound fields and the angular distribution of the fields in the far field of the antenna allowed us to establish a number of subtle effects in the formation of fields depending on both the type of embodiment the transmitter of antenna and the size of the acoustical baffle.ΠΡΠΎΠ²Π΅Π΄Π΅Π½ ΡΠΈΡΠ»Π΅Π½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ²ΠΎΠΉΡΡΠ² ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°Π½ΡΠ΅Π½Π½Ρ Ρ ΠΏΠ»ΠΎΡΠΊΠΈΠΌ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΈ ΠΌΡΠ³ΠΊΠΈΠΌ ΡΠΊΡΠ°Π½ΠΎΠΌ, ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½Π½ΡΠΌ Π² Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΏΠ»ΠΎΡΠΊΠΎΡΡΠΈ Π΅Ρ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Ρ, Π²ΡΠΏΠΎΠ»Π½Π΅Π½Π½ΠΎΠ³ΠΎ Π² Π²ΠΈΠ΄Π΅ ΡΠΈΠ»ΠΎΠ²ΠΎΠΉ ΠΈΠ»ΠΈ ΠΊΠΎΠΌΠΏΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΉ. Π‘ΠΎΠΏΠΎΡΡΠ°Π²ΠΈΡΠ΅Π»ΡΠ½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΡΠ°ΡΡΠΎΡΠ½ΡΡ
ΡΠ²ΠΎΠΉΡΡΠ² Π·Π²ΡΠΊΠΎΠ²ΡΡ
ΠΏΠΎΠ»Π΅ΠΉ ΠΈ ΡΠ³Π»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΏΠΎΠ»Π΅ΠΉ Π² Π΄Π°Π»ΡΠ½Π΅ΠΉ Π·ΠΎΠ½Π΅ Π°Π½ΡΠ΅Π½Π½Ρ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΡ ΡΡΠ΄ ΡΠΎΠ½ΠΊΠΈΡ
ΡΡΡΠ΅ΠΊΡΠΎΠ² Π² ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΠΎΠ»Π΅ΠΉ, Π·Π°Π²ΠΈΡΡΡΠΈΡ
ΠΊΠ°ΠΊ ΠΎΡ ΡΠΈΠΏΠ° ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΠΈΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΠΈΠ·Π»ΡΡΠ°ΡΠ΅Π»Ρ Π°Π½ΡΠ΅Π½Π½Ρ, ΡΠ°ΠΊ ΠΈ ΠΎΡ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠ² Π΅Ρ Π°ΠΊΡΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΊΡΠ°Π½Π°