2006
DOI: 10.1143/jjap.45.1743
|View full text |Cite
|
Sign up to set email alerts
|

Longitudinal Plane Wave Propagation in Elastic-Micropolar Porous Media

Abstract: Porous materials are widely used in the passive noise control field as sound absorbers. Conventional models of porous materials are assumed to have a rigid frame and to satisfy finite bulk elasticity. However, it may be the case that when high-frequency sound is applied to porous materials for nanotechnology applications, the classical theory of elasticity cannot be satisfied. Generalized continuum theories, such as coupled stress theory and micropolar theory, have additional degrees of freedom compared with c… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
21
0

Year Published

2007
2007
2016
2016

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 16 publications
(21 citation statements)
references
References 13 publications
0
21
0
Order By: Relevance
“…For micropolar elastic solid -M 1 (Polyurethane closed cell foam) (see Hsia and Cheng, 2006): k s = 2.09730 · 10 10 dyne/cm 2 , l s = 0.91822 · 10 10 dyne/cm 2 , K s = 0.22956 · 10 10 dyne/cm 2 , a s = À0.0000291 · 10 10 dyne, b s = 0.000045 · 10 10 dyne, c s = 0.0000423 · 10 10 dyne, j s = 0.037 cm 2 , q s = 0.0034 g/cm 3 . For micropolar viscous fluid medium -M 2 : k f = 1.5 · 10 10 dyne s/cm 2 , l f = 0.3 · 10 10 dyne s/cm 2 , K f = 0.00223 · 10 10 dyne s/cm 2 , a f = 0.00111 · 10 10 dyne s, b f = 0.0022 · 10 10 dyne s, c f = 0.000222 · 10 10 dyne s, j f = 0.0400 cm 2 , q f = 0.8 g/cm 3 and x/x 0 = 100.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…For micropolar elastic solid -M 1 (Polyurethane closed cell foam) (see Hsia and Cheng, 2006): k s = 2.09730 · 10 10 dyne/cm 2 , l s = 0.91822 · 10 10 dyne/cm 2 , K s = 0.22956 · 10 10 dyne/cm 2 , a s = À0.0000291 · 10 10 dyne, b s = 0.000045 · 10 10 dyne, c s = 0.0000423 · 10 10 dyne, j s = 0.037 cm 2 , q s = 0.0034 g/cm 3 . For micropolar viscous fluid medium -M 2 : k f = 1.5 · 10 10 dyne s/cm 2 , l f = 0.3 · 10 10 dyne s/cm 2 , K f = 0.00223 · 10 10 dyne s/cm 2 , a f = 0.00111 · 10 10 dyne s, b f = 0.0022 · 10 10 dyne s, c f = 0.000222 · 10 10 dyne s, j f = 0.0400 cm 2 , q f = 0.8 g/cm 3 and x/x 0 = 100.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…Different authors (Parfitt and Eringen, 1969;Kumar and Singh, 1998a;Singh and Kumar, 1998b;Tomar et al, 1998;Kumar, 2000;Kumar and Sharma, 2005;Hsia and Cheng, 2006;Hsia et al, 2007;Singh, 2007;Kumar and Rupender, 2008;) investigated the problems of reflection at the free surface of a micropolar elastic half space and micropolar thermoelastic half space.…”
Section: Ksharmamentioning
confidence: 99%
“…The theory of elastic and viscoelastic micropolar liquids was studied by Yeremeyev and Zubov [14]. Hsia and Cheng [15] discussed longitudinal plane waves propagation in elastic micropolar porous media. Hsia et al [16] studied propagation of transverse waves in elastic micropolar porous semispaces.…”
Section: Introductionmentioning
confidence: 99%