Semi-coupled air/water immersed boundary approach for curvilinear dynamic overset grids with application to ship hydrodynamics
For many problems in ship hydrodynamics, the effects of air flow on the water flow are negligible (the frequently called free surface conditions), but the air flow around the ship is still of interest. A method is presented where the water flow is decoupled from the air solution, but the air flow us...
Saved in:
Published in | International journal for numerical methods in fluids Vol. 58; no. 6; pp. 591 - 624 |
---|---|
Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Chichester, UK
John Wiley & Sons, Ltd
30.10.2008
Wiley |
Subjects | |
Online Access | Get full text |
Cover
Loading…
Abstract | For many problems in ship hydrodynamics, the effects of air flow on the water flow are negligible (the frequently called free surface conditions), but the air flow around the ship is still of interest. A method is presented where the water flow is decoupled from the air solution, but the air flow uses the unsteady water flow as a boundary condition. The authors call this a semi‐coupled air/water flow approach. The method can be divided into two steps. At each time step the free surface water flow is computed first with a single‐phase method assuming constant pressure and zero stress on the interface. The second step is to compute the air flow assuming the free surface as a moving immersed boundary (IB). The IB method developed for Cartesian grids (Annu. Rev. Fluid Mech. 2005; 37:239–261) is extended to curvilinear grids, where no‐slip and continuity conditions are used to enforce velocity and pressure boundary conditions for the air flow. The forcing points close to the IB can be computed and corrected under a sharp interface condition, which makes the computation very stable. The overset implementation is similar to that of the single‐phase solver (Comput. Fluids 2007; 36:1415–1433), with the difference that points in water are set as IB points even if they are fringe points. Pressure–velocity coupling through pressure implicit with splitting of operators or projection methods is used for water computations, and a projection method is used for the air. The method on each fluid is a single‐phase method, thus avoiding ill‐conditioned numerical systems caused by large differences of fluid properties between air and water. The computation is only slightly slower than the single‐phase version, with complete absence of spurious velocity oscillations near the free surface, frequently present in fully coupled approaches. Validations are performed for laminar Couette flow over a wavy boundary by comparing with the analytical solution, and for the surface combatant model David Taylor Model Basin (DTMB) 5512 by comparing with Experimental Fluid Dynamics (EFD) and the results of two‐phase level set computations. Complex flow computations are demonstrated for the ONR Tumblehome DTMB 5613 with superstructure subject to waves and wind, including 6DOF motions and broaching in SS7 irregular waves and wind. Copyright © 2008 John Wiley & Sons, Ltd. |
---|---|
AbstractList | For many problems in ship hydrodynamics, the effects of air flow on the water flow are negligible (the frequently called free surface conditions), but the air flow around the ship is still of interest. A method is presented where the water flow is decoupled from the air solution, but the air flow uses the unsteady water flow as a boundary condition. The authors call this a semi‐coupled air/water flow approach. The method can be divided into two steps. At each time step the free surface water flow is computed first with a single‐phase method assuming constant pressure and zero stress on the interface. The second step is to compute the air flow assuming the free surface as a moving immersed boundary (IB). The IB method developed for Cartesian grids (Annu. Rev. Fluid Mech. 2005; 37:239–261) is extended to curvilinear grids, where no‐slip and continuity conditions are used to enforce velocity and pressure boundary conditions for the air flow. The forcing points close to the IB can be computed and corrected under a sharp interface condition, which makes the computation very stable. The overset implementation is similar to that of the single‐phase solver (Comput. Fluids 2007; 36:1415–1433), with the difference that points in water are set as IB points even if they are fringe points. Pressure–velocity coupling through pressure implicit with splitting of operators or projection methods is used for water computations, and a projection method is used for the air. The method on each fluid is a single‐phase method, thus avoiding ill‐conditioned numerical systems caused by large differences of fluid properties between air and water. The computation is only slightly slower than the single‐phase version, with complete absence of spurious velocity oscillations near the free surface, frequently present in fully coupled approaches. Validations are performed for laminar Couette flow over a wavy boundary by comparing with the analytical solution, and for the surface combatant model David Taylor Model Basin (DTMB) 5512 by comparing with Experimental Fluid Dynamics (EFD) and the results of two‐phase level set computations. Complex flow computations are demonstrated for the ONR Tumblehome DTMB 5613 with superstructure subject to waves and wind, including 6DOF motions and broaching in SS7 irregular waves and wind. Copyright © 2008 John Wiley & Sons, Ltd. For many problems in ship hydrodynamics, the effects of air flow on the water flow are negligible (the frequently called free surface conditions), but the air flow around the ship is still of interest. A method is presented where the water flow is decoupled from the air solution, but the air flow uses the unsteady water flow as a boundary condition. The authors call this a semi-coupled air/water flow approach. The method can be divided into two steps. At each time step the free surface water flow is computed first with a single-phase method assuming constant pressure and zero stress on the interface. The second step is to compute the air flow assuming the free surface as a moving immersed boundary (IB). The IB method developed for Cartesian grids (Annu. Rev. Fluid Mech. 2005; 37:239-261) is extended to curvilinear grids, where no-slip and continuity conditions are used to enforce velocity and pressure boundary conditions for the air flow. The forcing points close to the IB can be computed and corrected under a sharp interface condition, which makes the computation very stable. The overset implementation is similar to that of the single-phase solver (Comput. Fluids 2007; 36:1415-1433), with the difference that points in water are set as IB points even if they are fringe points. Pressure-velocity coupling through pressure implicit with splitting of operators or projection methods is used for water computations, and a projection method is used for the air. The method on each fluid is a single-phase method, thus avoiding ill-conditioned numerical systems caused by large differences of fluid properties between air and water. The computation is only slightly slower than the single-phase version, with complete absence of spurious velocity oscillations near the free surface, frequently present in fully coupled approaches. Validations are performed for laminar Couette flow over a wavy boundary by comparing with the analytical solution, and for the surface combatant model David Taylor Model Basin (DTMB) 5512 by comparing with Experimental Fluid Dynamics (EFD) and the results of two-phase level set computations. Complex flow computations are demonstrated for the ONR Tumblehome DTMB 5613 with superstructure subject to waves and wind, including 6DOF motions and broaching in SS7 irregular waves and wind. For many problems in ship hydrodynamics, the effects of air flow on the water flow are negligible (the frequently called free surface conditions), but the air flow around the ship is still of interest. A method is presented where the water flow is decoupled from the air solution, but the air flow uses the unsteady water flow as a boundary condition. The authors call this a semi‐coupled air/water flow approach. The method can be divided into two steps. At each time step the free surface water flow is computed first with a single‐phase method assuming constant pressure and zero stress on the interface. The second step is to compute the air flow assuming the free surface as a moving immersed boundary (IB). The IB method developed for Cartesian grids ( Annu. Rev. Fluid Mech . 2005; 37 :239–261) is extended to curvilinear grids, where no‐slip and continuity conditions are used to enforce velocity and pressure boundary conditions for the air flow. The forcing points close to the IB can be computed and corrected under a sharp interface condition, which makes the computation very stable. The overset implementation is similar to that of the single‐phase solver ( Comput. Fluids 2007; 36 :1415–1433), with the difference that points in water are set as IB points even if they are fringe points. Pressure–velocity coupling through pressure implicit with splitting of operators or projection methods is used for water computations, and a projection method is used for the air. The method on each fluid is a single‐phase method, thus avoiding ill‐conditioned numerical systems caused by large differences of fluid properties between air and water. The computation is only slightly slower than the single‐phase version, with complete absence of spurious velocity oscillations near the free surface, frequently present in fully coupled approaches. Validations are performed for laminar Couette flow over a wavy boundary by comparing with the analytical solution, and for the surface combatant model David Taylor Model Basin (DTMB) 5512 by comparing with Experimental Fluid Dynamics (EFD) and the results of two‐phase level set computations. Complex flow computations are demonstrated for the ONR Tumblehome DTMB 5613 with superstructure subject to waves and wind, including 6DOF motions and broaching in SS7 irregular waves and wind. Copyright © 2008 John Wiley & Sons, Ltd. |
Author | Stern, Frederick Carrica, Pablo M. Huang, Juntao |
Author_xml | – sequence: 1 givenname: Juntao surname: Huang fullname: Huang, Juntao organization: IIHR-Hydroscience and Engineering, The University of Iowa, Iowa City, IA 52242, U.S.A – sequence: 2 givenname: Pablo M. surname: Carrica fullname: Carrica, Pablo M. organization: IIHR-Hydroscience and Engineering, The University of Iowa, Iowa City, IA 52242, U.S.A – sequence: 3 givenname: Frederick surname: Stern fullname: Stern, Frederick email: frederick-stern@uiowa.edu organization: IIHR-Hydroscience and Engineering, The University of Iowa, Iowa City, IA 52242, U.S.A |
BackLink | http://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=20751175$$DView record in Pascal Francis |
BookMark | eNp1kU2P0zAQhi20SHQXJH6CLyAu6fojiZ0j2qULosAB0B6tqe1QgxMH29nSC78dlxYkEJxGGj3PSO-85-hsDKNF6DElS0oIu-y9WVLRyHtoQUknKsJbfoYWhAlaMdLRB-g8pc-EkI5JvkDf39vBVTrMk7cGg4uXO8g2YjcMNqay2oR5NBD3GKYpBtBb3IeI9RzvnHejhYjNfoTBaRzuDkbGn6IzCe9c3h4c7zRkF0acA05bN-Ht3sRwctJDdL8Hn-yj07xAH1cvPly9rNbvbl5dPV9Xmre1rCjwlslaAtQMSC8FN7wt6TZCauC8EZxb0xrDO0I3tW2lZG1d15ueFrwxml-gp8e7JcPX2aasBpe09R5GG-akeENbybqugE9OICQNvo8wapfUFN1QnqAYEQ0t7y3c8sjpGFKKtlfa5Z9BcwTnFSXqUIcqdahDHUV49pfw6-Y_0OqI7py3-_9yarW-_pN3Kdtvv3mIX1QruGjU7dsb9Ubcvu7q9bVa8R_zKaw3 |
CODEN | IJNFDW |
CitedBy_id | crossref_primary_10_1007_s40722_022_00255_w crossref_primary_10_1007_s00158_017_1775_4 crossref_primary_10_1002_fld_2517 crossref_primary_10_1016_j_compfluid_2020_104627 crossref_primary_10_1016_j_marstruc_2022_103256 crossref_primary_10_1177_1077546317722897 crossref_primary_10_1007_s40722_022_00243_0 crossref_primary_10_1016_j_compfluid_2018_01_006 crossref_primary_10_1115_1_4042752 crossref_primary_10_1016_j_compfluid_2011_10_002 crossref_primary_10_1115_1_4041229 crossref_primary_10_1016_j_oceaneng_2022_113235 crossref_primary_10_1016_j_oceaneng_2023_115511 crossref_primary_10_1016_j_oceaneng_2019_04_082 crossref_primary_10_3233_ISP_180147 crossref_primary_10_1016_j_oceaneng_2015_10_039 crossref_primary_10_1007_s00366_021_01375_x crossref_primary_10_1016_j_apor_2015_04_007 crossref_primary_10_1016_j_apor_2020_102060 crossref_primary_10_1016_j_oceaneng_2022_111607 crossref_primary_10_1007_s00773_008_0022_5 crossref_primary_10_1115_1_4064971 crossref_primary_10_1016_S1001_6058_15_60452_8 crossref_primary_10_1016_j_oceaneng_2021_109081 crossref_primary_10_1115_1_4041372 crossref_primary_10_1016_j_oceaneng_2019_03_025 crossref_primary_10_1016_j_oceaneng_2021_109725 crossref_primary_10_1002_fld_2499 crossref_primary_10_1016_j_oceaneng_2021_109600 crossref_primary_10_3390_math8040546 crossref_primary_10_1063_5_0122257 crossref_primary_10_1177_1094342010394887 crossref_primary_10_1016_j_oceaneng_2019_106277 crossref_primary_10_1016_j_renene_2011_06_029 crossref_primary_10_1016_j_renene_2016_09_070 crossref_primary_10_3390_jmse12111979 crossref_primary_10_1016_j_oceaneng_2010_09_016 crossref_primary_10_1007_s10439_022_02902_7 crossref_primary_10_1080_10618562_2016_1234043 crossref_primary_10_1002_fld_5066 crossref_primary_10_1002_acs_3835 crossref_primary_10_1016_j_apor_2015_08_008 crossref_primary_10_1016_j_oceaneng_2022_112047 crossref_primary_10_1016_j_oceaneng_2019_05_064 crossref_primary_10_1016_j_renene_2014_11_014 crossref_primary_10_1016_j_renene_2016_05_061 crossref_primary_10_1016_j_apor_2016_04_006 crossref_primary_10_1016_j_oceaneng_2025_120312 crossref_primary_10_1007_s11831_014_9138_4 crossref_primary_10_1016_j_oceaneng_2016_02_019 crossref_primary_10_1080_0305215X_2014_895340 crossref_primary_10_1016_j_oceaneng_2017_07_053 crossref_primary_10_1007_s11831_022_09808_6 crossref_primary_10_1016_j_oceaneng_2019_106685 crossref_primary_10_1016_j_oceaneng_2022_113529 |
Cites_doi | 10.1016/j.compfluid.2007.01.007 10.21236/ADA458092 10.1016/0021-9991(81)90145-5 10.2514/3.12149 10.5957/jsr.2003.47.1.63 10.1016/0021-9991(88)90002-2 10.1016/S0045-7930(99)00033-X 10.1002/fld.1499 10.1007/s003480100293 10.1080/10618560310001634159 10.1017/S0022112099006965 10.1002/fld.1406 10.1002/fld.1279 10.2514/6.1991-1560 10.1016/0021-9991(72)90065-4 10.5957/jsr.1988.32.4.246 10.5957/jsr.2005.49.1.55 10.1016/j.compfluid.2004.12.005 10.1017/S0022112059000568 10.1146/annurev.fluid.37.061903.175743 |
ContentType | Journal Article |
Copyright | Copyright © 2008 John Wiley & Sons, Ltd. 2008 INIST-CNRS |
Copyright_xml | – notice: Copyright © 2008 John Wiley & Sons, Ltd. – notice: 2008 INIST-CNRS |
DBID | BSCLL AAYXX CITATION IQODW 7SC 7TB 7U5 8FD FR3 H8D JQ2 KR7 L7M L~C L~D |
DOI | 10.1002/fld.1758 |
DatabaseName | Istex CrossRef Pascal-Francis Computer and Information Systems Abstracts Mechanical & Transportation Engineering Abstracts Solid State and Superconductivity Abstracts Technology Research Database Engineering Research Database Aerospace Database ProQuest Computer Science Collection Civil Engineering Abstracts Advanced Technologies Database with Aerospace Computer and Information Systems Abstracts Academic Computer and Information Systems Abstracts Professional |
DatabaseTitle | CrossRef Aerospace Database Civil Engineering Abstracts Technology Research Database Computer and Information Systems Abstracts – Academic Mechanical & Transportation Engineering Abstracts ProQuest Computer Science Collection Computer and Information Systems Abstracts Solid State and Superconductivity Abstracts Engineering Research Database Advanced Technologies Database with Aerospace Computer and Information Systems Abstracts Professional |
DatabaseTitleList | Aerospace Database CrossRef |
DeliveryMethod | fulltext_linktorsrc |
Discipline | Applied Sciences Engineering Physics |
EISSN | 1097-0363 |
EndPage | 624 |
ExternalDocumentID | 20751175 10_1002_fld_1758 FLD1758 ark_67375_WNG_M7WK94LD_F |
Genre | article |
GrantInformation_xml | – fundername: ONR funderid: N00014‐01‐1‐0073; N00014‐06‐1‐0420 |
GroupedDBID | -~X .3N .GA .Y3 05W 0R~ 10A 1L6 1OB 1OC 1ZS 31~ 33P 3SF 3WU 4.4 4ZD 50Y 50Z 51W 51X 52M 52N 52O 52P 52S 52T 52U 52W 52X 5GY 5VS 66C 702 7PT 8-0 8-1 8-3 8-4 8-5 8UM 930 A03 AAESR AAEVG AAHHS AANLZ AAONW AASGY AAXRX AAZKR ABCQN ABCUV ABIJN ABJNI ACAHQ ACBWZ ACCFJ ACCZN ACGFS ACIWK ACPOU ACXBN ACXQS ADBBV ADEOM ADIZJ ADKYN ADMGS ADOZA ADZMN ADZOD AEEZP AEIGN AEIMD AENEX AEQDE AEUQT AEUYR AFBPY AFFPM AFGKR AFPWT AFRAH AFZJQ AHBTC AITYG AIURR AIWBW AJBDE AJXKR ALAGY ALMA_UNASSIGNED_HOLDINGS ALUQN AMBMR AMYDB ASPBG ATUGU AUFTA AVWKF AZBYB AZFZN AZVAB BAFTC BDRZF BFHJK BHBCM BMNLL BMXJE BNHUX BROTX BRXPI BSCLL BY8 CS3 D-E D-F DCZOG DPXWK DR2 DRFUL DRSTM DU5 EBS EJD F00 F01 F04 FEDTE G-S G.N GBZZK GNP GODZA H.T H.X HBH HGLYW HHY HVGLF HZ~ IX1 J0M JPC KQQ LATKE LAW LC2 LC3 LEEKS LH4 LITHE LOXES LP6 LP7 LUTES LW6 LYRES MEWTI MK4 MRFUL MRSTM MSFUL MSSTM MXFUL MXSTM N04 N05 NF~ O66 O9- OIG P2P P2W P2X P4D Q.N Q11 QB0 QRW R.K ROL RWI RWS RX1 RYL SUPJJ TN5 UB1 V2E W8V W99 WBKPD WIB WIH WIK WLBEL WOHZO WQJ WRC WXSBR WYISQ XG1 XPP XV2 ZZTAW ~02 ~IA ~WT AAHQN AAMNL AANHP AAYCA ACRPL ACYXJ ADNMO AFWVQ ALVPJ AAYXX AEYWJ AGQPQ AGYGG CITATION 6TJ AAMMB ABEML ACSCC AEFGJ AGHNM AGXDD AI. AIDQK AIDYY AMVHM HF~ IQODW M6O PALCI RIWAO RJQFR SAMSI TUS VH1 VOH ZY4 ~A~ 7SC 7TB 7U5 8FD FR3 H8D JQ2 KR7 L7M L~C L~D |
ID | FETCH-LOGICAL-c3648-1a362848aa42a0f873d36097b78ca335733ed6dd3901b4e68826444bf12a05dc3 |
IEDL.DBID | DR2 |
ISSN | 0271-2091 |
IngestDate | Thu Jul 10 23:12:49 EDT 2025 Mon Jul 21 09:13:47 EDT 2025 Thu Apr 24 22:57:22 EDT 2025 Tue Jul 01 02:08:29 EDT 2025 Wed Jan 22 17:06:16 EST 2025 Wed Oct 30 09:53:14 EDT 2024 |
IsPeerReviewed | true |
IsScholarly | true |
Issue | 6 |
Keywords | Computational fluid dynamics ship hydrodynamics Computation code Hydrodynamics Air water interface Modeling Curvilinear coordinate immersed boundary curvilinear and dynamic overset grids Parallel processing Free surface flow Numerical simulation level set method Shipbuilding Ship free surface flows Mesh generation semi-coupled method |
Language | English |
License | http://onlinelibrary.wiley.com/termsAndConditions#vor CC BY 4.0 |
LinkModel | DirectLink |
MergedId | FETCHMERGED-LOGICAL-c3648-1a362848aa42a0f873d36097b78ca335733ed6dd3901b4e68826444bf12a05dc3 |
Notes | istex:44CB2145AACBF6D0CE9453EEBE5B1043F18742C3 ArticleID:FLD1758 ark:/67375/WNG-M7WK94LD-F ONR - No. N00014-01-1-0073; No. N00014-06-1-0420 ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
PQID | 35168299 |
PQPubID | 23500 |
PageCount | 34 |
ParticipantIDs | proquest_miscellaneous_35168299 pascalfrancis_primary_20751175 crossref_citationtrail_10_1002_fld_1758 crossref_primary_10_1002_fld_1758 wiley_primary_10_1002_fld_1758_FLD1758 istex_primary_ark_67375_WNG_M7WK94LD_F |
ProviderPackageCode | CITATION AAYXX |
PublicationCentury | 2000 |
PublicationDate | 30 October 2008 |
PublicationDateYYYYMMDD | 2008-10-30 |
PublicationDate_xml | – month: 10 year: 2008 text: 30 October 2008 day: 30 |
PublicationDecade | 2000 |
PublicationPlace | Chichester, UK |
PublicationPlace_xml | – name: Chichester, UK – name: Chichester |
PublicationTitle | International journal for numerical methods in fluids |
PublicationTitleAlternate | Int. J. Numer. Meth. Fluids |
PublicationYear | 2008 |
Publisher | John Wiley & Sons, Ltd Wiley |
Publisher_xml | – name: John Wiley & Sons, Ltd – name: Wiley |
References | Syms GF. Numerical simulation of frigate airwakes. International Journal of Computational Fluid Dynamics 2004; 18:199-207. Gui L, Longo J, Stern F. Towing tank PIV measurement system, data and uncertainty assessment for DTMB model 5512. Experiments in Fluids 2001; 31:336-346. Wilson RV, Carrica PM, Stern F. Simulation of a ship breaking bow wave and induced vortices and scars. International Journal for Numerical Methods in Fluids 2007; 54(4):419-451. Reddy KR, Toffoletto R, Jones KRW. Numerical simulation of ship airwakes. Computers and Fluids 2000; 29:451-465. Peskin CS. Flow patterns around heart valves: a numerical method. Journal of Computational Physics 1972; 10:252-271. Wilson RV, Carrica PM, Stern F. Unsteady RANS method for ship motions with application to roll for a surface combatant. Computers and Fluids 2006; 35:501-524. Sullivan PP, McWilliams JC, Moeng CH. Simulation of turbulent flow over idealized water waves. Journal of Fluid Mechanics 2000; 404:47-85. Hirt CW, Nichols BD. Volume of fluid (VOF) method for dynamics of free boundaries. Journal of Computational Physics 1981; 39:201-225. Larsson L, Stern F, Bertram V. Benchmarking of computational fluid dynamics for ship flows: the Gothenburg 2000 Workshop. Journal of Ship Research 2003; 47:63-81. Thompson JF, Warsi ZUA, Mastin JW. Numerical Grid Generation. North-Holland: Amsterdam, 1985. Carrica PM, Wilson RV, Stern F. Ship motions using single-phase level set with dynamic overset grids. Computers and Fluids 2007; 36:1415-1433. Benjamin TB. Shearing flow over a wavy boundary. Journal of Fluid Mechanics 1959; 6:161-205. Carrica PM, Wilson RV, Stern F. An unsteady single-phase level set method for viscous free surface flows. International Journal for Numerical Methods in Fluids 2007; 53(2):229-256. Longo J, Stern F. Uncertainty assessment for towing tank tests with example for surface combatant DTMB model 5512. Journal of Ship Research 2005; 49:55-68. Lewis E (ed.). Principles of Naval Architecture, vol. III. SNAME: Jersey City, NJ, 1989; 28. Mittal R, Iaccarino G. Immersed boundary methods. Annual Review of Fluid Mechanics 2005; 37:239-261. Menter FR. Two-equation eddy viscosity turbulence models for engineering applications. AIAA Journal 1994; 32:1598-1605. Osher S, Sethian JA. Fronts propagating with curvature-dependent speed: algorithms based on Hamilton-Jacobi formulations. Journal of Computational Physics 1988; 79:12-49. Huang JT, Carrica PM, Stern F. Coupled ghost fluid/two-phase level set method for curvilinear body fitted grids. International Journal for Numerical Methods in Fluids 2007; 55(8):867-897. Stern F, Kim HT, Patel VC, Chen HC. A viscous-flow approach to the computation of propeller-hull interaction. Journal of Ship Research 1988; 32(4):246-262. 2000; 29 2004; 18 2006; 35 2000; 404 1988; 32 2003; 47 1985 1988; 79 1972; 10 1981; 39 1982 2003 1989; III 2007; 53 2005; 37 2007; 54 2005; 49 2007; 55 2007; 36 1994; 32 1959; 6 2001; 31 Lewis E (e_1_2_1_19_2) 1989 e_1_2_1_22_2 e_1_2_1_23_2 e_1_2_1_20_2 e_1_2_1_26_2 e_1_2_1_27_2 e_1_2_1_24_2 Stern F (e_1_2_1_21_2) 1988; 32 e_1_2_1_29_2 Larsson L (e_1_2_1_25_2) 2003; 47 Youngs DL (e_1_2_1_10_2) 1982 e_1_2_1_6_2 e_1_2_1_30_2 e_1_2_1_7_2 e_1_2_1_4_2 e_1_2_1_5_2 e_1_2_1_2_2 e_1_2_1_11_2 Longo J (e_1_2_1_28_2) 2005; 49 e_1_2_1_3_2 e_1_2_1_12_2 e_1_2_1_15_2 e_1_2_1_13_2 Thompson JF (e_1_2_1_16_2) 1985 e_1_2_1_14_2 e_1_2_1_8_2 e_1_2_1_17_2 e_1_2_1_9_2 e_1_2_1_18_2 |
References_xml | – reference: Hirt CW, Nichols BD. Volume of fluid (VOF) method for dynamics of free boundaries. Journal of Computational Physics 1981; 39:201-225. – reference: Sullivan PP, McWilliams JC, Moeng CH. Simulation of turbulent flow over idealized water waves. Journal of Fluid Mechanics 2000; 404:47-85. – reference: Carrica PM, Wilson RV, Stern F. Ship motions using single-phase level set with dynamic overset grids. Computers and Fluids 2007; 36:1415-1433. – reference: Thompson JF, Warsi ZUA, Mastin JW. Numerical Grid Generation. North-Holland: Amsterdam, 1985. – reference: Syms GF. Numerical simulation of frigate airwakes. International Journal of Computational Fluid Dynamics 2004; 18:199-207. – reference: Osher S, Sethian JA. Fronts propagating with curvature-dependent speed: algorithms based on Hamilton-Jacobi formulations. Journal of Computational Physics 1988; 79:12-49. – reference: Lewis E (ed.). Principles of Naval Architecture, vol. III. SNAME: Jersey City, NJ, 1989; 28. – reference: Benjamin TB. Shearing flow over a wavy boundary. Journal of Fluid Mechanics 1959; 6:161-205. – reference: Longo J, Stern F. Uncertainty assessment for towing tank tests with example for surface combatant DTMB model 5512. Journal of Ship Research 2005; 49:55-68. – reference: Peskin CS. Flow patterns around heart valves: a numerical method. Journal of Computational Physics 1972; 10:252-271. – reference: Mittal R, Iaccarino G. Immersed boundary methods. Annual Review of Fluid Mechanics 2005; 37:239-261. – reference: Stern F, Kim HT, Patel VC, Chen HC. A viscous-flow approach to the computation of propeller-hull interaction. Journal of Ship Research 1988; 32(4):246-262. – reference: Larsson L, Stern F, Bertram V. Benchmarking of computational fluid dynamics for ship flows: the Gothenburg 2000 Workshop. Journal of Ship Research 2003; 47:63-81. – reference: Reddy KR, Toffoletto R, Jones KRW. Numerical simulation of ship airwakes. Computers and Fluids 2000; 29:451-465. – reference: Huang JT, Carrica PM, Stern F. Coupled ghost fluid/two-phase level set method for curvilinear body fitted grids. International Journal for Numerical Methods in Fluids 2007; 55(8):867-897. – reference: Menter FR. Two-equation eddy viscosity turbulence models for engineering applications. AIAA Journal 1994; 32:1598-1605. – reference: Wilson RV, Carrica PM, Stern F. Simulation of a ship breaking bow wave and induced vortices and scars. International Journal for Numerical Methods in Fluids 2007; 54(4):419-451. – reference: Gui L, Longo J, Stern F. Towing tank PIV measurement system, data and uncertainty assessment for DTMB model 5512. Experiments in Fluids 2001; 31:336-346. – reference: Wilson RV, Carrica PM, Stern F. Unsteady RANS method for ship motions with application to roll for a surface combatant. Computers and Fluids 2006; 35:501-524. – reference: Carrica PM, Wilson RV, Stern F. An unsteady single-phase level set method for viscous free surface flows. International Journal for Numerical Methods in Fluids 2007; 53(2):229-256. – volume: 37 start-page: 239 year: 2005 end-page: 261 article-title: Immersed boundary methods publication-title: Annual Review of Fluid Mechanics – year: 1985 – volume: 18 start-page: 199 year: 2004 end-page: 207 article-title: Numerical simulation of frigate airwakes publication-title: International Journal of Computational Fluid Dynamics – volume: 53 start-page: 229 issue: 2 year: 2007 end-page: 256 article-title: An unsteady single‐phase level set method for viscous free surface flows publication-title: International Journal for Numerical Methods in Fluids – volume: 47 start-page: 63 year: 2003 end-page: 81 article-title: Benchmarking of computational fluid dynamics for ship flows: the Gothenburg 2000 Workshop publication-title: Journal of Ship Research – volume: 32 start-page: 1598 year: 1994 end-page: 1605 article-title: Two‐equation eddy viscosity turbulence models for engineering applications publication-title: AIAA Journal – volume: 49 start-page: 55 year: 2005 end-page: 68 article-title: Uncertainty assessment for towing tank tests with example for surface combatant DTMB model 5512 publication-title: Journal of Ship Research – volume: 6 start-page: 161 year: 1959 end-page: 205 article-title: Shearing flow over a wavy boundary publication-title: Journal of Fluid Mechanics – volume: 35 start-page: 501 year: 2006 end-page: 524 article-title: Unsteady RANS method for ship motions with application to roll for a surface combatant publication-title: Computers and Fluids – volume: 32 start-page: 246 issue: 4 year: 1988 end-page: 262 article-title: A viscous‐flow approach to the computation of propeller–hull interaction publication-title: Journal of Ship Research – volume: 55 start-page: 867 issue: 8 year: 2007 end-page: 897 article-title: Coupled ghost fluid/two‐phase level set method for curvilinear body fitted grids publication-title: International Journal for Numerical Methods in Fluids – year: 2003 – volume: III start-page: 28 year: 1989 – volume: 404 start-page: 47 year: 2000 end-page: 85 article-title: Simulation of turbulent flow over idealized water waves publication-title: Journal of Fluid Mechanics – volume: 36 start-page: 1415 year: 2007 end-page: 1433 article-title: Ship motions using single‐phase level set with dynamic overset grids publication-title: Computers and Fluids – volume: 29 start-page: 451 year: 2000 end-page: 465 article-title: Numerical simulation of ship airwakes publication-title: Computers and Fluids – volume: 54 start-page: 419 issue: 4 year: 2007 end-page: 451 article-title: Simulation of a ship breaking bow wave and induced vortices and scars publication-title: International Journal for Numerical Methods in Fluids – start-page: 24 end-page: 27 – volume: 79 start-page: 12 year: 1988 end-page: 49 article-title: Fronts propagating with curvature‐dependent speed: algorithms based on Hamilton–Jacobi formulations publication-title: Journal of Computational Physics – volume: 10 start-page: 252 year: 1972 end-page: 271 article-title: Flow patterns around heart valves: a numerical method publication-title: Journal of Computational Physics – volume: 39 start-page: 201 year: 1981 end-page: 225 article-title: Volume of fluid (VOF) method for dynamics of free boundaries publication-title: Journal of Computational Physics – volume: 31 start-page: 336 year: 2001 end-page: 346 article-title: Towing tank PIV measurement system, data and uncertainty assessment for DTMB model 5512 publication-title: Experiments in Fluids – start-page: 273 year: 1982 end-page: 285 – ident: e_1_2_1_3_2 doi: 10.1016/j.compfluid.2007.01.007 – ident: e_1_2_1_11_2 – start-page: 273 volume-title: Numerical Methods for Fluid Dynamics year: 1982 ident: e_1_2_1_10_2 – ident: e_1_2_1_17_2 doi: 10.21236/ADA458092 – ident: e_1_2_1_9_2 doi: 10.1016/0021-9991(81)90145-5 – ident: e_1_2_1_18_2 doi: 10.2514/3.12149 – volume: 47 start-page: 63 year: 2003 ident: e_1_2_1_25_2 article-title: Benchmarking of computational fluid dynamics for ship flows: the Gothenburg 2000 Workshop publication-title: Journal of Ship Research doi: 10.5957/jsr.2003.47.1.63 – ident: e_1_2_1_30_2 – ident: e_1_2_1_8_2 doi: 10.1016/0021-9991(88)90002-2 – ident: e_1_2_1_6_2 doi: 10.1016/S0045-7930(99)00033-X – ident: e_1_2_1_13_2 doi: 10.1002/fld.1499 – ident: e_1_2_1_27_2 doi: 10.1007/s003480100293 – ident: e_1_2_1_7_2 doi: 10.1080/10618560310001634159 – volume-title: Numerical Grid Generation year: 1985 ident: e_1_2_1_16_2 – start-page: 28 volume-title: Principles of Naval Architecture year: 1989 ident: e_1_2_1_19_2 – ident: e_1_2_1_20_2 doi: 10.1017/S0022112099006965 – ident: e_1_2_1_22_2 doi: 10.1002/fld.1406 – ident: e_1_2_1_5_2 doi: 10.1002/fld.1279 – ident: e_1_2_1_23_2 doi: 10.2514/6.1991-1560 – ident: e_1_2_1_14_2 doi: 10.1016/0021-9991(72)90065-4 – volume: 32 start-page: 246 issue: 4 year: 1988 ident: e_1_2_1_21_2 article-title: A viscous‐flow approach to the computation of propeller–hull interaction publication-title: Journal of Ship Research doi: 10.5957/jsr.1988.32.4.246 – volume: 49 start-page: 55 year: 2005 ident: e_1_2_1_28_2 article-title: Uncertainty assessment for towing tank tests with example for surface combatant DTMB model 5512 publication-title: Journal of Ship Research doi: 10.5957/jsr.2005.49.1.55 – ident: e_1_2_1_29_2 – ident: e_1_2_1_26_2 – ident: e_1_2_1_2_2 doi: 10.1016/j.compfluid.2004.12.005 – ident: e_1_2_1_12_2 – ident: e_1_2_1_24_2 doi: 10.1017/S0022112059000568 – ident: e_1_2_1_4_2 – ident: e_1_2_1_15_2 doi: 10.1146/annurev.fluid.37.061903.175743 |
SSID | ssj0009283 |
Score | 2.2226553 |
Snippet | For many problems in ship hydrodynamics, the effects of air flow on the water flow are negligible (the frequently called free surface conditions), but the air... |
SourceID | proquest pascalfrancis crossref wiley istex |
SourceType | Aggregation Database Index Database Enrichment Source Publisher |
StartPage | 591 |
SubjectTerms | Applied sciences Computational methods in fluid dynamics curvilinear and dynamic overset grids Exact sciences and technology Fluid dynamics free surface flows Fundamental areas of phenomenology (including applications) Ground, air and sea transportation, marine construction immersed boundary level set method Marine construction Physics semi-coupled method ship hydrodynamics |
Title | Semi-coupled air/water immersed boundary approach for curvilinear dynamic overset grids with application to ship hydrodynamics |
URI | https://api.istex.fr/ark:/67375/WNG-M7WK94LD-F/fulltext.pdf https://onlinelibrary.wiley.com/doi/abs/10.1002%2Ffld.1758 https://www.proquest.com/docview/35168299 |
Volume | 58 |
hasFullText | 1 |
inHoldings | 1 |
isFullTextHit | |
isPrint | |
link | http://utb.summon.serialssolutions.com/2.0.0/link/0/eLvHCXMwnV1Lb9QwEB6hcikHCgXE0lKMhOC0u0mc5xFRthW0PQBVK3Gw_EqJus1WeahdTv0J_EZ-CTN5bHcRSIhTpGicOM6M_c14_A3AK8_noStlOtQ6iNFBSdxhIh2JXkqCtwNlnaYc0OFRuH_sfzgNTrusSjoL0_JDLAJuZBnNfE0GLlU5viUNTadmhGsfnfOlVC3CQ59umaMSr2Xg9CIXFSFxe95Zxxv3DVdWors0qNeUGSlLHJy0rWqxAjuXwWuz-kw24Gvf7zbp5HxUV2qkv_9G6fh_H_YA7neglL1ttegh3LH5Jmx0AJV15l9uwr0l9sJHcPPZXmQ_b37oWX05RTmZFeMrhK4Fy5poON5STdGmYs566nKGGJnpGucn6qcsmJnn8iLTjDJJS1uxsyIzJaPoMFvaW2fVjFFaGfs2Nzjjt23Kx3A8ef_l3f6wK-gw1Dz00VuVuFzGfiyl70knjSNueOgkkYpiLTknakZrQmMoDqN8GyL6R7jmq9RF8cBo_gTW8llunwJDn55bdO2jmJhMFT4rJKp-FSTodKeRHsCb_ucK3bGdU9GNqWh5mj2BwyxomAfwciF52TJ8_EHmdaMfCwFZnFNGXBSIk6M9cRidfEz8g10xGcDOigItGngIzYgVdQAveo0SaMi0OyNzO6tLwQM3jBEc4Lsa7fhrZ8TkYJeuz_5VcAvWvY7FlzvbsFYVtX2OUKpSO43R_AJv7RzC |
linkProvider | Wiley-Blackwell |
linkToHtml | http://utb.summon.serialssolutions.com/2.0.0/link/0/eLvHCXMwnV1Lb9NAEB6V9gA9UCigpkC7SAhOSWyvn-KEKCHQJAdo1R6QVuv1mlpNncoPteHUn8Bv5Jcw40eaIJAQJ0urWXs9nt39Znb8DcBLy-auKWXcVcrx0UEJzG4gDYleSoDNTqiNqhzQeOIOj-1Pp87pGrxp_4Wp-SEWATeaGdV6TROcAtL9W9bQeBr1cPPz78AGFfSu_KnPt9xRgVVzcFqeiaYQmC3zrGH1254re9EGqfWaciNljuqJ67oWK8BzGb5W-89gC762I6_TTs57ZRH21PffSB3_89UewP0Gl7K3tSE9hDWdbsNWg1FZswLk27C5RGD4CG6-6Ivk580PNSsvpygnk6x_heg1Y0kVEMemsKrblM1Zy17OECYzVeISRQOVGYvmqbxIFKNk0lwX7FuWRDmjADFbOl5nxYxRZhk7m0e46Nd98sdwPHh_9G7YbWo6dBV3bXRYJe6Yvu1LaVvSiH2PR9w1Ai_0fCU5J3ZGHblRRKGY0NYuOgCI2OwwNlHciRR_AuvpLNU7wNCt5xq9e88nMtMQ7-USW3_oBOh3x57qwOv26wrVEJ5T3Y2pqKmaLYFqFqTmDrxYSF7WJB9_kHlVGchCQGbnlBTnOeJk8kGMvZPDwB4diEEH9lYsaNHBQnRGxKgd2G9NSuBcpgMamepZmQvumK6P-ACfVZnHXwcjBqMDuu7-q-A-3B0ejUdi9HFy-BTuWQ2pLzeewXqRlfo5Iqsi3Ktm0C8XoiDd |
linkToPdf | http://utb.summon.serialssolutions.com/2.0.0/link/0/eLvHCXMwnV1Lb9NAEB5BKyE4UCggwqNdJASnJLbXzyMimELTCAFVK3FYrXfXEDV1Ij8E4dSfwG_klzDjR5ogkBAnS6tZe72e2f1mdvwNwFPH5b4tZdpXygvRQYnsfiQtiV5KhM1eYqy6HNDRxD84dt-eeqdtViX9C9PwQ6wCbmQZ9XpNBr7Q6fCSNDSd6QHufeFV2HZ9KySNHr2_pI6KnIaC0wls1ITI7ohnLWfY9dzYirZpVr9RaqQscHbSpqzFBu5cR6_19hPvwKdu4E3WydmgKpOB-v4bp-P_vdktuNmiUvaiUaPbcMVku7DTIlTW2n-xCzfW6AvvwMUHcz79efFDzavFDOXkNB9-Reyas2kdDsempK7alC9Zx13OECQzVeECReOUOdPLTJ5PFaNU0sKU7HM-1QWj8DBbO1xn5ZxRXhn7stS45Dd9irtwHL_6-PKg31Z06Cvuu-iuStwvQzeU0nWklYYB19y3oiAJQiU5J25Go32tKRCTuMZH-I94zU1SG8U9rfg92MrmmbkPDJ16btC3D0KiMk3wXj5x9SdehF53GqgePO8-rlAt3TlV3ZiJhqjZETjNgqa5B09WkouG4uMPMs9q_VgJyPyMUuICT5xMXouj4OQwcscjEfdgb0OBVh0cxGZEi9qD_U6jBFoyHc_IzMyrQnDP9kNEB_isWjv-OhgRj0d0ffCvgvtw7d0oFuM3k8OHcN1pGX259Qi2yrwyjxFWlclebT-_AMYcH5U |
openUrl | ctx_ver=Z39.88-2004&ctx_enc=info%3Aofi%2Fenc%3AUTF-8&rfr_id=info%3Asid%2Fsummon.serialssolutions.com&rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Ajournal&rft.genre=article&rft.atitle=Semi-coupled+air%2Fwater+immersed+boundary+approach+for+curvilinear+dynamic+overset+grids+with+application+to+ship+hydrodynamics&rft.jtitle=International+journal+for+numerical+methods+in+fluids&rft.au=Huang%2C+Juntao&rft.au=Carrica%2C+Pablo+M&rft.au=Stern%2C+Frederick&rft.date=2008-10-30&rft.issn=0271-2091&rft.volume=58&rft.issue=6&rft.spage=591&rft.epage=624&rft_id=info:doi/10.1002%2Ffld.1758&rft.externalDBID=NO_FULL_TEXT |
thumbnail_l | http://covers-cdn.summon.serialssolutions.com/index.aspx?isbn=/lc.gif&issn=0271-2091&client=summon |
thumbnail_m | http://covers-cdn.summon.serialssolutions.com/index.aspx?isbn=/mc.gif&issn=0271-2091&client=summon |
thumbnail_s | http://covers-cdn.summon.serialssolutions.com/index.aspx?isbn=/sc.gif&issn=0271-2091&client=summon |