Updated lyx doc
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lrftubes.bib
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lrftubes.bib
@ -31,7 +31,7 @@
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journaltitle = {Journal of Sound and Vibration},
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author = {Beltman, W. M.},
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urldate = {2011-07-20},
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date = {1999-10-28},
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date = {1999},
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keywords = {Printed},
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file = {BELTMAN - 1999 - VISCOTHERMAL WAVE PROPAGATION INCLUDING ACOUSTO-EL.pdf:/home/anne/.literature/storage/VUEH48TH/BELTMAN - 1999 - VISCOTHERMAL WAVE PROPAGATION INCLUDING ACOUSTO-EL.pdf:application/pdf;ScienceDirect Snapshot:/home/anne/.literature/storage/7RZVXTAA/S0022460X99923556.html:text/html}
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}
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@ -112,6 +112,17 @@ The full solution of the problem has been obtained by Kirchhoff (1868) in the fo
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file = {ingentaconnect An Efficient Finite Element Model for Viscothermal Acoustics:/home/anne/.literature/storage/68KJ2IVT/art00009.html:text/html;Kampinga et al. - 2011 - An Efficient Finite Element Model for Viscothermal.pdf:/home/anne/.literature/storage/QRGF9MR6/Kampinga et al. - 2011 - An Efficient Finite Element Model for Viscothermal.pdf:application/pdf}
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}
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@book{bird_transport_2007,
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location = {New York, {NY}, {USA}},
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edition = {2nd},
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title = {Transport phenomena},
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isbn = {978-0-470-11539-8},
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series = {Wiley International edition},
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publisher = {J. Wiley},
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author = {Bird, R.B. and Stewart, W.E. and Lightfoot, E.N.},
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date = {2007}
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}
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@article{bossart_hybrid_2003,
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title = {Hybrid numerical and analytical solutions for acoustic boundary problems in thermo-viscous fluids},
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volume = {263},
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@ -179,6 +190,21 @@ The full solution of the problem has been obtained by Kirchhoff (1868) in the fo
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file = {Ward e.a. - 2017 - DeltaEC Users Guide version 6.4b2.7.pdf:/home/anne/.literature/storage/MQKGHJ9I/Ward e.a. - 2017 - DeltaEC Users Guide version 6.4b2.7.pdf:application/pdf}
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}
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@article{licht_variation_1944,
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title = {The Variation of the Viscosity of Gases and Vapors with Temperature.},
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volume = {48},
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issn = {0092-7325},
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doi = {10.1021/j150433a004},
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pages = {23--47},
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number = {1},
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journaltitle = {The Journal of Physical Chemistry},
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shortjournal = {J. Phys. Chem.},
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author = {Licht, William and Stechert, Dietrich G.},
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urldate = {2015-01-08},
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date = {1944},
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file = {ACS Full Text Snapshot:/home/anne/.literature/storage/4JAIZ6VC/j150433a004.html:text/html;Licht and Stechert - 1944 - The Variation of the Viscosity of Gases and Vapors.pdf:/home/anne/.literature/storage/MKPFZ6SN/Licht and Stechert - 1944 - The Variation of the Viscosity of Gases and Vapors.pdf:application/pdf}
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}
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@thesis{van_der_eerden_noise_2000,
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location = {Enschede, The Netherlands},
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title = {Noise reduction with coupled prismatic tubes},
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@ -205,7 +231,6 @@ The full solution of the problem has been obtained by Kirchhoff (1868) in the fo
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title = {Numerical modeling of thermoacoustic systems},
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rights = {All rights reserved},
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url = {http://doc.utwente.nl/96275/},
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abstract = {The subject of this thesis is a relatively new class of heat engines and refrigerators, called thermoacoustic ({TA}) systems. {TA} systems have gained commercial interest due to their low number of moving parts and potentially high efficiency. In the case of a {TA} engine, heat is converted to acoustic power. This power can subsequently be converted to electricity using a ?reversed? loudspeaker, called a linear alternator. In a {TA} refrigerator, a speaker or linear alternator is used to generate a strong acoustic wave, which is used to pump heat. To achieve competitive power densities, thermoacoustic systems are generally run at such high amplitudes, that performance deteriorating nonlinear effects can no longer be neglected. To accu- rately predict performance in the nonlinear regime, nonlinear models are required. This thesis describes two contributions to the field of thermoacoustic system modeling. Firstly, a one-dimensional heat transfer model has been developed. This model can be used to estimate the performance of often used parallel-plate heat exchangers for thermoacoustic systems. These heat exchangers are located close to the stack or regenerator of a {TA} system and are responsible for the heat in/output required to let the system execute its thermodynamic cycle. The results of the model show a good match with a different heat transfer model from the literature, and the model provides guidelines for future heat exchanger design. Secondly, a nonlinear frequency domain method is developed with which the initial transient start-up process can be skipped in the simulations. The method can be used to directly simulate a {TA} system in its periodic steady-state. This significantly reduces computational cost, since the initial transient regime often involves several hundred oscillation cycles. The method is applied to a one-dimensional nonlinear model of {TA} systems. The model is used to simulate an experimental standing wave thermoacoustic engine from the literature. The obtained results are in agreement with literature results.},
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institution = {Universiteit Twente},
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type = {phdthesis},
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author = {De Jong, J.A.},
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@ -339,3 +364,21 @@ The full solution of the problem has been obtained by Kirchhoff (1868) in the fo
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author = {Welch, Peter},
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date = {1967}
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}
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@article{kino_investigation_2009,
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title = {Investigation of non-acoustical parameters of compressed melamine foam materials},
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volume = {70},
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issn = {0003682X},
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url = {https://linkinghub.elsevier.com/retrieve/pii/S0003682X08001497},
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doi = {10.1016/j.apacoust.2008.07.002},
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abstract = {A series of careful non-acoustical parameters measurements using 5 ‘Illtec’ melamine foam and 10 ‘Basotect {TG}’ melamine foam samples have been made. Flow resistivity, tortuosity, porosity, viscous characteristic length and thermal characteristic length of two types of compressed melamine foam materials with different foam magnifications have been investigated. It has been found that a relationship between the flow resistivity, fibre equivalent diameter and bulk density exists for each of the compressed melamine foam materials.},
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pages = {595--604},
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number = {4},
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journaltitle = {Applied Acoustics},
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shortjournal = {Applied Acoustics},
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author = {Kino, Naoki and Ueno, Takayasu and Suzuki, Yasuhiro and Makino, Hiroshi},
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urldate = {2019-11-28},
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date = {2009-04},
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langid = {english},
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file = {Kino et al. - 2009 - Investigation of non-acoustical parameters of comp.pdf:/home/anne/.literature/storage/I9P5SZAE/Kino et al. - 2009 - Investigation of non-acoustical parameters of comp.pdf:application/pdf}
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}
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lrftubes.lyx
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lrftubes.lyx
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\usepackage{xcolor}
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% If we use non-tex fonts we need this for biblatex
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% \usepackage{polyglossia}
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% \setdefaultlanguage{english}
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\usepackage[%
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giveninits=true,
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%% natbib=true,
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%% date=year,
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bibencoding=utf8,
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% style=numeric-comp,
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backend=biber,
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% refsection=chapter, % If we want bibliographies per chapter
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]{biblatex}
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% \usepackage[%
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% %% natbib=true,
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% %% date=year,
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% bibencoding=utf8,
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% backend=biber,
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% % refsection=chapter, % If we want bibliographies per chapter
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% ]{biblatex}
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\DeclareFieldFormat*{url}{}
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\DeclareFieldFormat[misc]{url}{\mkbibacro{URL}\addcolon\space\url{#1}}
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\DeclareFieldFormat[report]{url}{\mkbibacro{URL}\addcolon\space\url{#1}}
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\DeclareFieldFormat*{urldate}{}
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\DeclareFieldFormat[misc]{urldate}{\mkbibparens{\bibstring{urlseen}\space#1}}
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\DeclareFieldFormat[report]{urldate}{\mkbibparens{\bibstring{urlseen}\space#1}}
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\renewbibmacro{in:}{}
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% We need absolute path to the bibliography here, or it should be in
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% the same directory
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\addbibresource{lrftubes.bib}
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% \DeclareFieldFormat*{url}{}
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% \DeclareFieldFormat[misc]{url}{\mkbibacro{URL}\addcolon\space\url{#1}}
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% \DeclareFieldFormat[report]{url}{\mkbibacro{URL}\addcolon\space\url{#1}}
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% \DeclareFieldFormat*{urldate}{}
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% \DeclareFieldFormat[misc]{urldate}{\mkbibparens{\bibstring{urlseen}\space#1}}
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% \DeclareFieldFormat[report]{urldate}{\mkbibparens{\bibstring{urlseen}\space#1}}
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% \renewbibmacro{in:}{}
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% Separate the items in the bibliography somewhat
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% \setlength{\bibsep}{4pt}
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\newcommand{\lrftubes}{\textbf{\texttt{LRFTubes}}}
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\newcommand{\lrftubes}{\texttt{LRFTubes}}
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\newcommand{\lrftubess}{\lrftubes\ }
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% Customize the caption of the figures and tables
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\usepackage[margin=10pt,font={footnotesize},labelfont=bf,labelsep=endash]{caption}
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