2 edition of **effects of fluid resonance on the boundary stresses of a fluid-filled cavity** found in the catalog.

effects of fluid resonance on the boundary stresses of a fluid-filled cavity

C. C. Mow

- 161 Want to read
- 2 Currently reading

Published
**1965** by Rand Corporation in Santa Monica, Calif .

Written in English

- Elastic waves -- Diffraction.,
- Seismic waves.

**Edition Notes**

Bibliography: p. 33.

Statement | C.C. Mow and J.W. Workman. |

Series | Memorandum -- RM-4453-PR, Research memorandum (Rand Corporation) -- RM-4453-PR.. |

Contributions | Workman, J. W. |

The Physical Object | |
---|---|

Pagination | xii, 33 p. : |

Number of Pages | 33 |

ID Numbers | |

Open Library | OL17984418M |

chemistry/anatomy. STUDY. PLAY. Sodium citrate is used in embalming fluid as. in comparing cavity fluid to arterial fluid cavity fliud wil have. no active dyes. reodorants are used as. masking agents. Surgical Technology Examination Book. 81 terms. Embalming Theory II Final. 95 terms. The fluid that resides within cranial and spinal cavities, cerebrospinal fluid (CSF), moves in a pulsatile fashion to and from the cranial cavity. This motion can be measured by magnetic resonance imaging (MRI) and may be of clinical importance in the diagnosis of several brain and spinal cord disorders such as hydrocephalus, Chiari Cited by: **Gather, Amplify, Transfer sound waves to Fluid Filled spaces. Fluid Filled spaces--> Inner Ear Sense Organs for Balance and Hearing. Pinna. --> can lead to tympanic cavity filling with fluid/pus > the movement of the basilar membrane leads to effects on NT release. Helicotrema.

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Determination of the dynamic stresses at the boundary of a cavity filled with an inviscid compressible fluid during the passage of a plane dilatational wave train. The steady-state response or admittance function is obtained for a circular cavity of infinite : C.

Mow, J. Workman. Workman. The effects of fluid resonance on the boundary stresses of a fluid-filled cavity About RAND Reports. Quality Standards; Publishing Overview; Ordering Information; Information for Libraries; Reprint & Linking Permissions; Explore.

By Author. It is found that, at critical wave numbers, the intensity of the boundary stresses is significantly higher than that predicted under static loading. It is shown that these high intensities are due to resonance in the fluid and that the resonance conditions can be predicted once the properties of the medium and the fluid are by: On the Effect of Boundary Vibration on Poiseuille Flow of an Elastico-Viscous Liquid.

The longitudinal and orthogonal superposition of boundary driven, small strain, oscillatory shear flow and steady Poiseuille flow is investigated. Boundary oscillations are of different frequencies and amplitudes and are represented by sinusoidal : Dennis Siginer.

The tangential stresses created on the free boundary by an adjoint gas flow are considered to be a driving force for a fluid motion. The influence of the cavity geometry (cavity aspect ratio) and of the free boundary (length of the open part of the boundary) on the velocity field is investigated by: 2.

An increase in the Rayleigh number results in increasing the effects of the interaction between fluid and structure and strengthens the natural convection inside the cavity.-During the transient process, the baffle and the top wall of the cavity, which are considered elastic, undergo an oscillatory by: From the results in Fig.

1, Fig. 2, Fig. 3, it then can be said that for extension-thickening fluids the fluid viscoelasticity has stabilizing effect on spinning whereas it has destabilizing effect for extension-thinning by: the surface of a fluid-filled crack excited into resonance by an impul- and y directions in the sketch of Figure 3).

By carefully select- sive pressure transient. Spin‐stabilized projectiles with liquid payloads may experience different types of flight instabilities caused by the fluid motion in the payload cylinder. The first type is known to occur in low‐viscosity fluids, i.e., at high Reynolds numbers, owing to resonance with inertial waves at critical frequencies.

The second type originates from a forced secondary flow at arbitrary frequency Cited by: 7. MOMENTUM LOSS IN A BOUNDARY LAYER There is a shear stress at the boundary and therefore the ﬂuid loses momentum as the boundary layer grows. The rate of momentum loss can be related to the shear stress.

One way to do this calculation is to consider the control volume shown below: By conservation of mass (per unit length into the page), m File Size: 1MB.

The fundamental effect the two ridge sinusoidal topography exerts on the large scale motion in the baroclinic fluid is (1) to modulate the flow and thus to make the flow uneven both in time and in space, (2) to suppress the odd modes.

The vacillation with time in the flow aroused by the topography is. A surface-based hydrostatic fluid cavity could be de-fined for the gas. A simple surface pressure load could be applied to the free surface of the fluid. Bottle drop analysis. The purpose of this analysis is to determine the integrity of a fluid-filled bottle when dropped from a height of 3 Size: 1MB.

As there is no Rayleigh poles in the set of poles of the fluid-filled cavity, the factorization of the “soft” background compensates the effects of the so-called leaky Rayleigh-type surface modes analyzed and discussed in Ref. These last modes consist of the fluid cylinder modes occurring when their dispersion curves strongly by: 9.

The temperature distribution and fluid velocity field are found in the limit of vanishingly small Reynolds and Peclet numbers under the following boundary condition: temperature jump, thermal creep, viscous slip, and in addition of thermal stress slip at the particle surface and cavity by: 1.

Collapse of an initially spherical vapour cavity in the neighbourhood of a solid boundary. Vapour bubble collapse problems lacking spherical symmetry are solved here using a numerical method designed especially for these problems.

Viscosity and compressibility Cited by: impingement on the acoustic resonance excitation in the cavity and Strouhal number values. The experiments are conducted in an open loop wind tunnel that can generate a flow with a Mach number up to The results of each case are compared with a base case where sharp edges are installed upstream and downstream.

It is observed that. The expressions for the vorticity on the boundary are usually obtained from the viscous no-slip condition [8, 9]. In the present paper, expressions are obtained for the vorticity on a wall in the presence of slip.

The obtained expressions are used to solve a test problem on the flow of a viscous incompressible fluid in a by: 4. The conformal mapping method of complex functions and expansion method of wave functions are adopted, the stresses and displacements at the cavity boundary are. Radial displacement of a fluid-filled cavity within either a poroelastic or poroelasto-plastic geomaterial.

The geomaterial is first subjected to a compressive radial stress applied at infinity and, after reaching a steady state, a pressure pulse is applied within the fluid-filled cavity.

Maximum resulting fluid pressure is Cited by: The Fluid-filled Spherical Cavity in a Damage-susceptible Poroelastic Medium A. SELVADURAI* AND A. SHIRAZI Department of Civil Engineering and Applied Mechanics McGill University, Sherbrooke Street stress field with provision for complete fluid drainage at the boundary.

quency of a fluid-filled cavity is dependent on the speed of sound in the fluid. The introduction of a sample (e.g., rock) perturbs the resonance properties of the cavity. The resonant frequency difference between the empty cavity (f 1) and the sample-loaded cavity (f 2) is used to predict the acoustic properties of the loaded Size: 1MB.

In this study, we report the effects of a uniform stationary magnetic field on the flow of ferrofluid (FF) inside a boundary driven cavity. A coupled set of conservation equations for the flow field, the Maxwell’s magnetostatic equations, and the constitutive magnetization equation are solved numerically.

The non-dimensional groups primarily influencing the phenomenon are first Cited by: 3. EFFECT OF CAVITATION ON THE STRUCTURE OF THE BOUNDARY LAYER region and showed the contribution of the fluid lightening on the wall shear stress.

Djéridi et al. () observed in turbulent flow properties of the boundary layer with and without cavity in order to identify the modifications of theAuthor: Ch.

Sarraf, Y. Ait Bouziad, H Djeridi, M. Farhat, F. Deniset, J.-Y. Billard. The effect of viscosity on the axisymmetric, forced vibrations of a fluid-filled, elastic, spherical shell is studied analytically. Necessary theory, using boundary layer approximation for the fluid as developed in a previous paper for free vibrations, has been extended to incorporate an external forcing by: Steady flow generated by oscillations of an inner solid core in a fluid-filled rotating spherical cavity is experimentally studied.

The core with density less than the fluid density is located. Experiments were performed to understand the complex fluid-structure interactions that occur during aircraft internal store carriage.

A cylindrical store was installed in a rectangular cavity having a length-to-depth ratio of and a length-to-width ratio of 1. The Mach number ranged from to and the incoming boundary layer was turbulent.

Cited by: Buoyancy driven cavity flow of a micropolar fluid with variably heated bottom wall while the upper boundary of the cavity is adiabatic. part of the stress tensor. Physically these boundary. The effects of fluid resonance on the boundary stresses of a fluid-filled cavity On the effects of stress-wave diffraction on ground-shock measurements: part I Dynamic Response of Lined and Unlined Underground Openings.

This review pertains to the body of work dealing with internal recirculating flows generated by the motion of one or more of the containing walls.

These flows are not only technologically important, they are of great scientific interest because they display almost all fluid mechanical phenomena in the simplest of geometrical settings. Thus corner eddies, longitudinal vortices, nonuniqueness.

27 Index Cavity Fluid with fast firming action to the CORE. Cinnamon scented to make the working area more pleasant. 30 Index Cavity. 27 Index Cavity. 20 Index Cavity. 20 Index Cavity. 45 Index Cavity. 11 Index Cavity. Fluid-acoustic interactions in fluid-dynamic oscillations of a flow over a two-dimensional cavity were investigated by directly solving the compressible Navier-Stokes equations.

It was assumed that the upstream boundary layer is turbulent and the depth-to-length ratio of the cavity is Cited by: 1. It should be emphasized that we are concerned only with the effect on shell resonance frequencies due to static internal pressure, regardless of the specific fluid contained in the shell, rather than acoustic pressures associated with spherical cavity modes.

The mechanism by which prestress within a shell causes the resonance frequencies to shift is clearly by: 4. A series of experiments has been conducted in a lid‐driven cavity of square cross section (depth=width= mm) for Reynolds numbers (Re, based on lid speed and cavity width) between and 10and spanwise aspect ratios (SAR) between and Flow visualization using polystyrene beads and two‐dimensional laser‐Doppler anemometer (LDA) measurements have shed Cited by: Experiments were performed to understand the complex fluid-structure interactions that occur during aircraft internal store carriage.

A cylindrical store was installed in a rectangular cavity having a length-to-depth ratio of and a length-to-width ratio of 1. The Mach number ranged from to and the incoming boundary layer was by: The averaged lift force acting on a cylindrical body near the boundary of a cavity with a fluid performing translational vibrations was studied.

Experiments were performed with variation the viscosity of the fluid, the size and relative density of the body, and vibration parameters were by: 6. Mohamed, S., and Ziada, S. "Effect of Cavity Volume on the Flow-Excited Acoustic Resonance of a Shallow Cavity in a Pipe-Line." Proceedings of the ASME Pressure Vessels and Piping Conference.

Volume 4: Fluid-Structure by: 2. Start studying A&P Chapter 8: Articulations. Learn vocabulary, terms, and more with flashcards, games, and other study tools. immovable joint created when 2 bones fuse and the boundary between them disappears (ex. Frontal suture of the frontal bone and the epiphyseal line of mature long bones) Pad of fibrous cartilage situated between.

a small, fluid-filled pocket that forms in a connective tissue. It contains synovial fluid and is lined by a synovial membrane. often form where a tendon or ligament rubs against other tissues. Located around most synovial joints, bursae reduce friction and act as shock absorbers.

@article{osti_, title = {Compressibility effects in the shear layer over a rectangular cavity}, author = {Beresh, Steven J.

and Wagner, Justin L. and Casper, Katya M.}, abstractNote = {we studied the influence of compressibility on the shear layer over a rectangular cavity of variable width in a free stream Mach number range of – using particle image velocimetry data in the.

Start studying Joints. Learn vocabulary, terms, and more with flashcards, games, and other study tools. Search. fluid-filled pocket that forms in connective tissue; often form where a tendon or ligament rub against other tissues effects of wear and tear on the joint surfaces or from genetic factors affection collagen formation.

However, it was found that strong coupling between the thin-walled structure and the acoustic cavity exists in the vicinity of any uncoupled acoustic resonance. Thus, the coupled properties of the systems were found to be dominated by the uncoupled acoustic by: 8.ratio for both the lid driven cavity [8] and for a range of other flows [12].

Grillet et. al. [16] used a finite element technique to compute the effect of fluid elasticity on the flow kinematics and stress distribution in lid driven cavity flow, with a view to better understand the appearance of purely elastic instabilities in recirculating Size: 4MB.

When the acoustic resonance is excited, the sound pressure level in the cavity reaches dB. Square blocks are attached to the surface of the channel and centred upstream of the cavity leading edge to suppress the flow-excited acoustic resonance in the cavity.

Six blocks of different widths are tested at three different upstream by: