The immediate impulse-response of a confined incompressible fluid
is characterized by inertance. For a vessel with inlet and outlet, this
is a single quantity; for multiple ports the generalization is a singular
reciprocal inertance matrix, acting on the port-impulses to give the
corresponding inflows. The coefficients are defined by the boundaryfluxes of potential flows. Green’s identity converts these to domain
integrals of kinetic energy. If the system is discretized with finite
elements, a third method is proposed which requires only the stiffness
matrix and the solution vectors and no numerical differentiation.
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%0 Journal Article
%1 noauthororeditor
%A McBain, G. D.
%A Mallinson, S. G.
%A Brown, B. R.
%A Gustafsson, Tom
%D 2019
%J The ANZIAM Journal
%K 65n30-pdes-bvps-finite-elements 76-04-fluid-mechanics-explicit-machine-computation-and-programs 76b99-incompressible-inviscid-fluids-none-of-the-above 76m10-finite-element-methods-in-fluid-mechanics
%P C140–C155
%R 10.21914/anziamj.v60i0.14058
%T Three Ways to Compute Multiport Inertance
%U https://journal.austms.org.au/ojs/index.php/ANZIAMJ/article/view/14058
%V 60
%X The immediate impulse-response of a confined incompressible fluid
is characterized by inertance. For a vessel with inlet and outlet, this
is a single quantity; for multiple ports the generalization is a singular
reciprocal inertance matrix, acting on the port-impulses to give the
corresponding inflows. The coefficients are defined by the boundaryfluxes of potential flows. Green’s identity converts these to domain
integrals of kinetic energy. If the system is discretized with finite
elements, a third method is proposed which requires only the stiffness
matrix and the solution vectors and no numerical differentiation.
@article{noauthororeditor,
abstract = {The immediate impulse-response of a confined incompressible fluid
is characterized by inertance. For a vessel with inlet and outlet, this
is a single quantity; for multiple ports the generalization is a singular
reciprocal inertance matrix, acting on the port-impulses to give the
corresponding inflows. The coefficients are defined by the boundaryfluxes of potential flows. Green’s identity converts these to domain
integrals of kinetic energy. If the system is discretized with finite
elements, a third method is proposed which requires only the stiffness
matrix and the solution vectors and no numerical differentiation.
},
added-at = {2019-06-19T01:59:43.000+0200},
author = {McBain, G. D. and Mallinson, S. G. and Brown, B. R. and Gustafsson, Tom},
biburl = {https://www.bibsonomy.org/bibtex/29b74a40a002b074e456c5b74aab3f1c8/gdmcbain},
doi = {10.21914/anziamj.v60i0.14058},
interhash = {e69e2059e6bcc28cb70b2574799b763d},
intrahash = {9b74a40a002b074e456c5b74aab3f1c8},
issn = {1446-8735},
journal = {The ANZIAM Journal},
keywords = {65n30-pdes-bvps-finite-elements 76-04-fluid-mechanics-explicit-machine-computation-and-programs 76b99-incompressible-inviscid-fluids-none-of-the-above 76m10-finite-element-methods-in-fluid-mechanics},
language = {en},
pages = {C140–C155},
timestamp = {2019-09-30T01:37:21.000+0200},
title = {Three Ways to Compute Multiport Inertance},
url = {https://journal.austms.org.au/ojs/index.php/ANZIAMJ/article/view/14058},
volume = 60,
year = 2019
}