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ON THE THIRD ORDER SOLUTION OF KdV EQUATION BY USING HOMOTOPY PERTURBATION METHOD

BAREKENG: Jurnal Ilmu Matematika dan Terapan · Vol. 17 No. 2 (2023) · pp. 0609–0614

DOI
10.30598/barekengvol17iss2pp0609-0614
ISSN
2615-3017, 1978-7227
Published
2023-06-11
Publisher
PATTIMURA UNIVERSITY
Language
eng
License
creativecommons.org/licenses/by-sa/4.0

Abstract

In this research we discussed about the solution of the KdV equation using Homotopy Perturbation method. The KdV equation that describing water wave equation solved by using the mixing method between Homotopy and Perturbation method. Homotopy was built with embedding parameter p∈[0,1] which undergoes a deformation process from linear problems to nonlinear problems and the assumed solution of the KdV equation is expressed in the form of a power series p up to the third order. The result show that in each order solution we obtained resonance term. for handling the condition, we used Lindsteadt-Poincare method.the wave number k2 and dispersion relation can be obtained in the second order solution as the effect of using Lindsteadt-Poincare method.

Collaboration network of the authors

40 authors · 114 co-authorship links · 1 across different organisations · showing the 40 most connected

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  • State University of Semarang
  • Ministry of Religious Affairs
  • Muhammadiyah University of Makassar
  • Affiliation unknown
  • Different organisations
  • Same organisation
  • Affiliation unknown
  • Thicker line = more joint articles · bigger circle = more articles
Show as table
Co-authorOrganisationJoint articles
Rahayu Budhiati VeronicaAffiliation unknown6
Amin SuyitnoAffiliation unknown4
Mulyono MulyonoAffiliation unknown3
Arief AgoestantoAffiliation unknown3
Muhammad KharisAffiliation unknown3
Hardi SuyitnoAffiliation unknown3
Rochmad RochmadAffiliation unknown3
Putriaji HendikawatiAffiliation unknown3
Kristina WijayantiAffiliation unknown3
Sriati UsmanAffiliation unknown2
Anjar Kusuma DewiAffiliation unknown2
Nadrun NadrunAffiliation unknown2
Darmawan DarmawanAffiliation unknown2
Masrukan MasrukanState University of Semarang2
Riza ArifudinState University of Semarang2
St. Budi WaluyaAffiliation unknown2
Muhammad Zuhair ZahidAffiliation unknown2
Naila Zulfatur RohmahAffiliation unknown2
Detalia Noriza MunahefiAffiliation unknown2
Dewi Putri Tuah SusilaAffiliation unknown1
Abd. KamarrudinAffiliation unknown1
Moh. Abraham Akbar EisenringAffiliation unknown1
Mochtar MarhumAffiliation unknown1
Khusnul KhusnulAffiliation unknown1
Mawardin MawardinAffiliation unknown1
Dela ZahraAffiliation unknown1
Nur FajriaAffiliation unknown1
Budi BudiAffiliation unknown1
Sindi KlodiaAffiliation unknown1
Maf'ulah Maf'ulahAffiliation unknown1
Mulky Satria KamalAffiliation unknown1
Rahmat Agung WibowoAffiliation unknown1
Desrin LebagiAffiliation unknown1
Tresia Hartati UpeAffiliation unknown1
Ratnasari RamlanAffiliation unknown1
Muhajir MuhajirMinistry of Religious Affairs1
Nirwana NirwanaMuhammadiyah University of Makassar1

Affiliations come from OpenAlex; journal OAI-PMH metadata carries none. Authors without an OpenAlex ID are matched by name, which can merge or split people.

Metadata source: OAI-PMH (metadata jurnal) https://ojs3.unpatti.ac.id/index.php/barekeng/oai, first harvested 5 Nov 2026, last seen 5 Nov 2026.
Original metadata (oai_dc)
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	<dc:title xml:lang="en-US">ON THE THIRD ORDER SOLUTION OF KdV EQUATION BY USING HOMOTOPY PERTURBATION METHOD</dc:title>
	<dc:creator>Mashuri, Mashuri</dc:creator>
	<dc:creator>Zakiyah, Yayah</dc:creator>
	<dc:creator>Reorita, Rina</dc:creator>
	<dc:description xml:lang="en-US">In this research we discussed about the solution of the KdV equation using Homotopy Perturbation method. The KdV equation that describing water wave equation solved&amp;nbsp; by using the mixing method between Homotopy and Perturbation method. Homotopy was built with embedding parameter p∈[0,1] which undergoes a deformation process&amp;nbsp; from linear problems to nonlinear problems and the assumed solution of the KdV equation is expressed in the form of a power series p up to the third order. The result show that in each order solution &amp;nbsp;we obtained resonance term. for handling the condition, we used Lindsteadt-Poincare method.the wave number k2 and dispersion relation &amp;nbsp;can be obtained in the second order solution as the effect of using Lindsteadt-Poincare method.</dc:description>
	<dc:publisher xml:lang="en-US">PATTIMURA UNIVERSITY</dc:publisher>
	<dc:date>2023-06-11</dc:date>
	<dc:type>info:eu-repo/semantics/article</dc:type>
	<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
	<dc:format>application/pdf</dc:format>
	<dc:identifier>https://ojs3.unpatti.ac.id/index.php/barekeng/article/view/6597</dc:identifier>
	<dc:identifier>10.30598/barekengvol17iss2pp0609-0614</dc:identifier>
	<dc:source xml:lang="en-US">BAREKENG: Jurnal Ilmu Matematika dan Terapan; Vol 17 No 2 (2023): BAREKENG: Journal of Mathematics and Its Applications; 0609-0614</dc:source>
	<dc:source>2615-3017</dc:source>
	<dc:source>1978-7227</dc:source>
	<dc:source>10.30598/barekengvol17iss2year2023</dc:source>
	<dc:language>eng</dc:language>
	<dc:relation>https://ojs3.unpatti.ac.id/index.php/barekeng/article/view/6597/5921</dc:relation>
	<dc:rights xml:lang="en-US">Copyright (c) 2023 Mashuri Mashuri, Yayah Zakiyah, Rina Reorita</dc:rights>
	<dc:rights xml:lang="en-US">http://creativecommons.org/licenses/by-sa/4.0</dc:rights>
</oai_dc:dc>