Your email was sent successfully. Check your inbox.

An error occurred while sending the email. Please try again.

Proceed reservation?

Export
  • 1
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1958
    In:  The Journal of the Acoustical Society of America Vol. 30, No. 7_Supplement ( 1958-07-01), p. 698-698
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 30, No. 7_Supplement ( 1958-07-01), p. 698-698
    Abstract: A noise producer is usually pictured as a piece of rotating machinery mounted on a heavy base plate and insulated from the ground by means of an ideal spring. Such a model is too idealized to be of great value in many practical applications. The general case may be represented by a periodical force or statistical noise source that drives a point mass which, in its turn, excites a housing or shell with many natural vibrations. This case is dealt with in a rigid mathematical manner on the basis of the asymptotic laws of the natural modes of shells and membranes. The possibilities and methods of noise abatement for this general case in air and in water are discussed in detail.
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1958
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 2
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1959
    In:  The Journal of the Acoustical Society of America Vol. 31, No. 6_Supplement ( 1959-06-01), p. 845-845
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 31, No. 6_Supplement ( 1959-06-01), p. 845-845
    Abstract: In an acoustically inhomogeneous medium, such as the air or the sea, the sizes of the scattering patches are always distributed continuously. The patches vary from a maximum size determined by the geometry of the fluid to a minimum size prescribed by viscosity and heat conductance. The Kolmogorov equilibrium law seems to give a very realistic description of the dimensions of the scattering patches, though this law was originally derived for homogeneous turbulence only. The scattering integrals are evaluated for such a distribution of patch sizes. The results show backward scattering to be mainly determined by the patch sizes that have a diameter equal to the wavelength, whereas forward scattering is mainly produced by larger patches up to a certain size determined by the wavelength and distance. (The integrals have logarithmic infinities at the corresponding space-wave numbers of the patch distribution.) The results also show that backscattering radically limits the range of propagation at low frequencies to a value that depends on the distance from the nearest boundary.
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1959
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 3
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1962
    In:  The Journal of the Acoustical Society of America Vol. 34, No. 12_Supplement ( 1962-12-01), p. 2004-2004
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 34, No. 12_Supplement ( 1962-12-01), p. 2004-2004
    Abstract: Inhomogeneous mechanical vibrators usually consist of homogeneous plates, shells, bars (stiffening rings), and rigid masses and predominantly compliant elements. By generalizing the fundamental concepts of the theory of electrical networks for 3 dimensions, an attempt is made to derive a general theory of complex, 3-dimensional mechanical vibrators that is free of insignificant details. Because of the electrical analogies, the theory of inhomogeneous systems also contains the theory of electrical networks, electrical filters and telephone lines, and electrically coupled circuits. [This work was sponsored by the U. S. Atomic Energy Commission and by the Bureau of Weapons.]
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1962
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 4
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1981
    In:  The Journal of the Acoustical Society of America Vol. 70, No. 1 ( 1981-07-01), p. 1-9
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 70, No. 1 ( 1981-07-01), p. 1-9
    Abstract: The velocity amplitude of a thin, sperical shell can be rigorously described by a two-mesh electrical circuit, and a considerable amount of information can be obtained from this circuit without computations. The exact solutions for the radial and tangential velocity components for point excitation of the shell are represented by two oscillator terms with frequency-independent coefficients and are interpreted physically. It is proved that by confining the computations to resonance vibration (using only one generalized coordinate to represent the ’’two-resonance-frequencies’’ modes) the coefficients of the exact solution can be derived with the aid of the Hamilton principle. The resonance frequencies can be approximated with relatively high accuracy by a simple expression, and the mean-value solution and the envelopes through the resonance peaks and the anti-resonance minima are easily derived. The shell turns out to be very stiff at low frequencies; resonances occur only at relatively high frequencies, i.e., near and above the ring resonance frequency. As the frequency enters the resonance range, the shell becomes very soft but, with increasing frequency, it stiffens up again, and its impedance approaches that of an infinite plate of the same thickness.
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1981
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 5
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1981
    In:  The Journal of the Acoustical Society of America Vol. 70, No. S1 ( 1981-11-01), p. S62-S62
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 70, No. S1 ( 1981-11-01), p. S62-S62
    Abstract: The geometric mean between the resonance peaks and the antiresonance minima in the driving point response of a vibrator represents the mean line through the logarithmically recorded response curve. This mean is independent of the damping and is a simple function of the frequency difference, εν between successive mode resonance frequencies and the mode masses, Mν. The height of the peaks above this line and the minima below it are given by a factor β = 2εν/πωB ≈ εν/ωB, where ωB is the bandwidth, as long as the peaks are well separated (β & gt; 4). With decreasing β, peaks and minima decrease drastically and for β ≈ 1 the response curve is smooth without peaks and minima. The driving point admittance usually has a small reactive component (wattless field), but by adjusting ενMν it can be made real and matched to any prescribed resistance. Thus, it is possible to modify the frequency response of a vibrator within reasonable limits. Because the mean line through the response curve is not affected by reflections of the wave fields at the boundaries or by boundary conditions, coupled vibrators and vibrators with inhomogeneities, such as welds, ribs, and mass loads, can be easily investigated by the mean-value theory. Examples will be presented. [This work was sponsored by the Office of Naval Research, Code 474.]
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1981
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 6
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1982
    In:  The Journal of the Acoustical Society of America Vol. 72, No. S1 ( 1982-11-01), p. S43-S44
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 72, No. S1 ( 1982-11-01), p. S43-S44
    Abstract: Resonances of a point driven vibrator occur when the reflected waves reach the driver in phase with the outgoing wave, antiresonances occur when these two waves are in antiphase. The frequency response for the outgoing wave field determines the geometric mean line through the frequency response curve of the vibrator. Reflections at the boundaries of the vibrator, at ribs and appendages, or at material variations, have no effect on the “mean-line response.” Plate modes are scalar functions of the position. In contrast, shell modes are represented by three-dimensional functions. But they are also described by uncoupled and orthogonal mode functions. Isolated vibrating systems always have orthogonal modes. It may sometimes be convenient to describe a vibrator by mode functions of some simpler vibrator. Every mode then is represented by a sum of mode functions which are coupled (e.g., plate with a mass load). The transients of a complex vibrator can be built up from the transients of its modes. An understanding of the theory of transients is important, for instance, when frequency modulated pulses are generated; increasing the damping may lead to long duration transients; the aim here is to cancel the switching-on transient with the switching-off transient which can only be done if damping is small. The theory of natural modes and transients will be illustrated by practical examples. [This work was sponsored by the Office of Naval Research, Code 474.]
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1982
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 7
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1957
    In:  The Journal of the Acoustical Society of America Vol. 29, No. 1 ( 1957-01-01), p. 50-59
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 29, No. 1 ( 1957-01-01), p. 50-59
    Abstract: The standard mathematical procedure formally describes scattering by the superposition of a scattered pressure on the unscattered sound field. At low frequencies, because of the irregular distribution of the inhomogeneities, the phases of the scattered waves are at random and scattering is an interference phenomenon. As the frequency increases, scattering becomes highly collimated in the forward direction and the phase differences decrease to zero. At this point ray theory starts to apply. The scattered pressure, then, essentially describes only a phase change caused by the different sound velocities and the focusing and defocusing by the lens action of the patches. The medium in the neighborhood of the receiver can be shown to contribute only by focusing, the medium farther away only by interference fluctuations. Focusing leads to normally distributed amplitude fluctuations. The distribution of the interference fluctuations, however, passes from normal to Rayleigh with increasing values of range.
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1957
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 8
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1967
    In:  The Journal of the Acoustical Society of America Vol. 42, No. 5_Supplement ( 1967-11-01), p. 1196-1196
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 42, No. 5_Supplement ( 1967-11-01), p. 1196-1196
    Abstract: The simplest type of vibrators are point and line sources. The sound fields of such vibrators are uncorrelated over space and their energies add, if they are separated by a distance greater than about 14 wavelength. Vibrators with nodal lines radiate as if their radiation impedance were ρc if the distance between the nodal lines is greater than half a sound wavelength. If their distance is smaller, they generate sound because of the distortion of the natural mode patterns by the driving force and because of the discontinuity of the vibration pattern near the edges of the vibrator. Both types of sound radiation turn out to be predictable in a very simple manner by a kind of Huygen's principle. Because ribs also distort the vibration field, they lead to increased sound radiation. [Work sponsored by the Office of Naval Research, Washington, D. C.]
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1967
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 9
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1958
    In:  The Journal of the Acoustical Society of America Vol. 30, No. 12 ( 1958-12-01), p. 1140-1152
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 30, No. 12 ( 1958-12-01), p. 1140-1152
    Abstract: The study is based on the general differential equation of a mechanical system. Driving force and solution are expressed as a series of natural functions of the dissipationless system. Dissipation is taken into account by introducing complex elastic constants. Each Fourier coefficient of the driving force is written as the product of an excitation constant and the total driving force. The excitation constants can then be included in the mode parameters of the system and the solution, written as the product of the total driving force and the “mechanical impedance” of the system. The solution is exact and useful at the lower frequencies. A simple solution for higher frequencies can be derived by replacing the series by an integral and evaluating this integral. Three important parameters can thus be obtained: the driving-point impedance that describes the velocity of the driving point and the reaction of the system to the driving force, the effective impedance that represents the average velocity amplitude over the system, and the effective dissipation resistance with respect to this average-velocity amplitude. The expression derived for the high-frequency driving-point impedance then turns out to represent, also, the general background level at lower frequencies. The solution for the driving-point impedance in the intermediate frequency range is obtained by adding to this background the contribution of the natural mode that has its resonant frequency closest to the frequency of the force; the effective impedance, on the other hand, is given with good approximation as the impedance of the mode whose resonance frequency is closest to the frequency of the force; and the effective dissipation resistance is given by the resistive component of this mode impedance. The mode parameters are computed for rods, membranes, plates, and shells for three situations—a point force, a linear force distribution, and a force distribution given by a Fourier integral. The results make it possible to handle complicated mechanical systems with almost the same ease as simple mass points, and to compute their sound radiation.
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1958
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 10
    Online Resource
    Online Resource
    Acoustical Society of America (ASA) ; 1959
    In:  The Journal of the Acoustical Society of America Vol. 31, No. 1_Supplement ( 1959-01-01), p. 111-111
    In: The Journal of the Acoustical Society of America, Acoustical Society of America (ASA), Vol. 31, No. 1_Supplement ( 1959-01-01), p. 111-111
    Abstract: The propagation of sound pulses in rods is extremely complex. At very low frequencies Young's modulus determines the sound phenomenon. As the frequency increases shear waves are generated simultaneously and are generated, whenever a sound pulse is reflected at the end of the rod. At still higher frequencies dilatational modes of different phase and group velocities can be distinguished. The order of the energy carrying modes increases as the frequency increases and the losses in the rod are due to the losses in the shear and the dilatation moduli, the ratio between the two kinds of losses varying with the frequency. Finally, at high frequencies only high-order modes seem to be excited and the propagation velocity of pulses approaches the sound velocity of the infinite medium. An evaluation of sound velocity and attenuation measurements at high frequencies is therefore a very difficult task. The theory is illustrated by experimental results.
    Type of Medium: Online Resource
    ISSN: 0001-4966 , 1520-8524
    RVK:
    Language: English
    Publisher: Acoustical Society of America (ASA)
    Publication Date: 1959
    detail.hit.zdb_id: 1461063-2
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
Close ⊗
This website uses cookies and the analysis tool Matomo. Further information can be found on the KOBV privacy pages