Example: Acoustics in Coupled Rooms

Slides:



Advertisements
Similar presentations
Radially Polarized Spherical Piezoelectric Acoustic Transducer.
Advertisements

Kinetic Theory of Matter
Introduction to RF for Accelerators
Airborne Sound Insulation in Buildings
Acoustic-Structural Interaction in a Tuning Fork
Living room acoustics You can use the heading from the model documentation for the title. © 2013 COMSOL. All rights reserved.
Sedan Interior Acoustics
Course Introduction to virtual engineering Óbuda University John von Neumann Faculty of Informatics Institute of Intelligent Engineering Systems Lecture.
Absorptive Muffler with Shells
Example: Simulation of Electrochemical Impedance Spectroscopy
Example: Electrokinetic valve
Example: Vibration of a Disk Backed by an Air-Filled Cylinder.
Section 7 Mesh Control.
Abstract Velocity profiles of Byrd glacier show a transition from a parabolic transverse profile upstream to a plug flow transverse velocity profile. A.
Example: Acoustics in a Muffler. Introduction The damping effectiveness of a muffler is studied in the frequency range 100─1000 Hz In the low-frequency.
Example: Acoustics in a Muffler. Introduction The damping effectiveness of a muffler is studied in the frequency range 100─1000 Hz In the low-frequency.
Lesson 1 - Oscillations Harmonic Motion Circular Motion
Christopher Morehouse Julie Maier Ted Zachwieja Caroline Bills NOISE REDUCTION FOR INTERNAL COMBUSTION ENGINE.
NORMAL MODES AND COUPLED ROOMS ACOUSTICS OF CONCERT HALLS AND ROOMS Principles of Vibration and Sound Chapters 6 and 11.
EQUILIBRIUM OF RIGID BODIES. RIGID BODIES Rigid body—Maintains the relative position of any two particles inside it when subjected to external loads.
Chapter 5 Vibration Analysis
Chapters 16 – 18 Waves.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
Smoothed Particle Hydrodynamics (SPH) Fluid dynamics The fluid is represented by a particle system Some particle properties are determined by taking an.
Experiment 11 Gearing.
Modern Automotive Technology PowerPoint for by Russell Krick
Mechanical Waves & Sound. Wave Motion Waves are caused by.
1 SIMULATION OF VIBROACOUSTIC PROBLEM USING COUPLED FE / FE FORMULATION AND MODAL ANALYSIS Ahlem ALIA presented by Nicolas AQUELET Laboratoire de Mécanique.
Soundboards Function is to amplify the sound of vibrating strings –A surface pushes more air than a string, thus it is a more efficient radiator of sound.
1 Formulations variationnelles et modèles réduits pour les vibrations de structures contenant des fluides compressibles en l’absence de gravité Cours de.
Agenda: General kickers analysis Wang-Tsutsui method for computing impedances Benchmarks Conclusions Bibliography Acknowledgments: E.Métral, M.Migliorati,
1 Sound Field Modeling in Architectural Acoustics using a Diffusion Equation Based Model N. Fortin 1,2, J. Picaut 2, A. Billon 3, V. Valeau 4, A. Sakout.
Model: Sliding Wedge. Introduction This is a NAFEMS benchmark model which treats the behavior of a contactor wedge forced to slide over a stiff target.
© 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the.
S. Kahn 5 June 2003NuFact03 Tetra Cooling RingPage 1 Tetra Cooling Ring Steve Kahn For V. Balbekov, R. Fernow, S. Kahn, R. Raja, Z. Usubov.
Physical Fluid Dynamics by D. J. Tritton What is Fluid Dynamics? Fluid dynamics is the study of the aforementioned phenomenon. The purpose.
Modeling Signal Leakage Characteristics of Broadband Over Power Line (BPL) Using NEC With Experimental Verification Steve Cerwin WA5FRF Institute Scientist.
Numerical simulation of droplet motion and two-phase flow field in an oscillating container Tadashi Watanabe Center for Computational Science and e-Systems.
KINETIC THEORY OF MATTER. 3 STATES OF MATTER SOLID LIQUID GAS.
2.1 Position, Velocity, and Speed 2.1 Displacement  x  x f - x i 2.2 Average velocity 2.3 Average speed  
George David Associate Professor Ultrasound Physics 03A: Reflections ‘97.
Finite Element Solution of Fluid- Structure Interaction Problems Gordon C. Everstine Naval Surface Warfare Center, Carderock Div. Bethesda, Maryland
MOTION OF ERYTHROCYTES ALONG THE CAPILLARIES Alexander V. Kopyltsov.
SOUND INSULATION. SOUND INSULATION: Is process whereby structures and materials are arranged to reduce the transmission of sound from one room or area.
MECHANICS OF SOUND ABSORPTION
15.2 Sound Waves. Chapter 15 Objectives  Explain how the pitch, loudness, and speed of sound are related to properties of waves.  Describe how sound.
Waves & Sound Ch 10 6 th grade. What forms mechanical waves? A wave is a disturbance involving the transfer of energy from place to place. Waves that.
AROMA 2.0 Structural Damping – Influence of Variable Normal Load on Friction Damping Mohammad Afzal, KTH Sound and Vibration MWL TURBO POWER.
Hanyang University 1/29 Antennas & RF Devices Lab. Partially filled wave guide Jeong Gu Ho.
Force Vibration Response Spectrum
Simulation of the acoustics of coupled rooms by numerical resolution of a diffusion equation V. Valeau a, J. Picaut b, A. Sakout a, A. Billon a a LEPTAB,
Department of building structures, Czech Technical University, Ing. Jaroslav Hejl, Ing. Jiří Nováček, Ph.D. sound insulation.
Modelling and simulation of hydraulic motor tribology
Friction Investigating static and kinetic friction of a body on different surfaces.
Finite element mesh and load definition
Chapter 4 Fluid Mechanics Frank White
Muffler Basics.
WORKSHOP 12 BOUNCING BALL
Date of download: 10/16/2017 Copyright © ASME. All rights reserved.
Date of download: 10/26/2017 Copyright © ASME. All rights reserved.
Transformations of Stress and Strain
MASS LAW.
Ultrasound.
Modelling of Atomic Force Microscope(AFM)
326MAE (Stress and Dynamic Analysis) 340MAE (Extended Stress and Dynamic Analysis)
COMSOL Simulation of Air Pollutant Particle Transmission in a Building
ECE699 – 004 Sensor Device Technology
Finite element Analysis study of P-U based Acoustic Vector Sensor for Underwater Application in COMSOL Bipin Kumar1, Arun Kumar1, Rajendar Bahl1 1Centre.
PANDA Collaboration Meeting
Presentation transcript:

Example: Acoustics in Coupled Rooms

Introduction Acoustics in Coupled Rooms The sound transmission across a building element sample is simulated. The setup is similar to the one stipulated by the ISO 15186/3 standard as implemented at the Icelandic Building Research Institute (IBRI) in Reykjavik. This example shows how Extended Multiphysics can be used to split a model into separate exchangeable modules. In particular, a 2D model of the sample is inserted into the 3D test bench.

Geometry Acoustics in Coupled Rooms – Problem Definition In the 3D geometry, the rooms are modeled as much further apart than they really are. The rooms are connected via the sample plate, which is modeled in a separate 2D geometry. Sending room Receiving room Sound source Sample plate

Domain Equations – Acoustics Acoustics in Coupled Rooms – Problem Definition Domain Equations – Acoustics Frequency domain acoustics is goverened by a slightly modified Helmholtz’s equation for the acoustic pressure, p. Material properties are density, r0, and speed of sound, c. Note that the density cannot be eliminated from the equation unless it is a global constant

Domain Equations – Structure Acoustics in Coupled Rooms – Problem Definition Domain Equations – Structure As a simple example, a 1 cm thick, homogenous steel plate is used as sample. The plate is modeled using plate elements of Reissner-Mindlin type. The pressure difference between the rooms enter the plate equations as a surface load.

Boundary Conditions – Acoustics Acoustics in Coupled Rooms – Problem Definition Boundary Conditions – Acoustics The natural boundary condition corresponds to inward normal acceleration. Three types are used: Specified normal acceleration, given by plate movement Specified impedance, partly absorbing Hard wall

Boundary Conditions – Structure Acoustics in Coupled Rooms – Problem Definition Boundary Conditions – Structure The plate is mounted in the opening between the rooms using wooden spacers and wedges. Where the plate is in contact with the spacers, it is considered free to rotate, but not to move. The rest of the gap between plate and niche wall is filled with a soft sound absorbing material that does not restrict the plate’s movements.

Results Acoustics in Coupled Rooms – Results The instantaneous pressure pattern is shown as isosurfaces. The wall color represents the sound pressure level in the two rooms (in dB).

Results Acoustics in Coupled Rooms – Results The sound reduction index is not a smooth function of frequency. This is probably due to the absence of damping in the source room and the sample plate causing pronounced resonance effects.