Vibroacoustical modeling and modal analysis of a double wall panel

1998 ◽  
Vol 103 (5) ◽  
pp. 2814-2814
Author(s):  
Stan Josef Pietrzko
Keyword(s):  
Modal Analysis ◽  
Wall Panel ◽  
Double Wall

scholarly journals A mobility based vibroacoustic energy transmission simulation into an enclosure through a double-wall panel

2017 ◽  
Vol 141 (6) ◽  
pp. EL598-EL604 ◽  
Author(s):  
Atanu Sahu ◽  
Partha Bhattacharya ◽  
Arup Guha Niyogi ◽  
Michael Rose
Keyword(s):  
Wall Panel ◽  
Energy Transmission ◽  
Double Wall

Optimization for sound transmission through a double-wall panel

2013 ◽  
Vol 74 (12) ◽  
pp. 1422-1428 ◽  
Author(s):  
Jie Zhou ◽  
Atul Bhaskar ◽  
Xin Zhang
Keyword(s):  
Sound Transmission ◽  
Wall Panel ◽  
Double Wall

Modal Analysis of Turbulent Flow near an Inclined Bank–Longitudinal Structure Junction

2021 ◽  
Vol 147 (3) ◽  
pp. 04020100
Author(s):  
Nasser Heydari ◽  
Panayiotis Diplas ◽  
J. Nathan Kutz ◽  
Soheil Sadeghi Eshkevari
Keyword(s):  
Turbulent Flow ◽  
Modal Analysis ◽  
Longitudinal Structure

Effect of Bass Bar Tension on Modal Parameters of a Violin's Top Plate

2015 ◽  
Vol 39 (1) ◽  
pp. 145-149 ◽  
Author(s):  
Ewa B. Skrodzka ◽  
Bogumił B.J. Linde ◽  
Antoni Krupa
Keyword(s):  
Modal Analysis ◽  
Experimental Modal Analysis ◽  
Mode Shapes ◽  
Modal Parameters ◽  
Normal Value ◽  
Modal Damping

Abstract Experimental modal analysis of a violin with three different tensions of a bass bar has been performed. The bass bar tension is the only intentionally introduced modification of the instrument. The aim of the study was to find differences and similarities between top plate modal parameters determined by a bass bar perfectly fitting the shape of the top plate, the bass bar with a tension usually applied by luthiers (normal), and the tension higher than the normal value. In the modal analysis four signature modes are taken into account. Bass bar tension does not change the sequence of mode shapes. Changes in modal damping are insignificant. An increase in bass bar tension causes an increase in modal frequencies A0 and B(1+) and does not change the frequencies of modes CBR and B(1-).

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