Stability ordinates of Adams predictor-corrector methods

Verfasser / Beitragende:
[Michelle Ghrist, Bengt Fornberg, Jonah Reeger]
Ort, Verlag, Jahr:
2015
Enthalten in:
BIT Numerical Mathematics, 55/3(2015-09-01), 733-750
Format:
Artikel (online)
ID: 605496919
LEADER caa a22 4500
001 605496919
003 CHVBK
005 20210128100538.0
007 cr unu---uuuuu
008 210128e20150901xx s 000 0 eng
024 7 0 |a 10.1007/s10543-014-0528-7  |2 doi 
035 |a (NATIONALLICENCE)springer-10.1007/s10543-014-0528-7 
245 0 0 |a Stability ordinates of Adams predictor-corrector methods  |h [Elektronische Daten]  |c [Michelle Ghrist, Bengt Fornberg, Jonah Reeger] 
520 3 |a How far the stability domain of a numerical method for approximating solutions to differential equations extends along the imaginary axis indicates how useful the method is for approximating solutions to wave equations; this maximum extent is termed the imaginary stability boundary, also known as the stability ordinate. It has previously been shown that exactly half of Adams-Bashforth (AB), Adams-Moulton (AM), and staggered Adams-Bashforth methods have nonzero stability ordinates. In this paper, we consider two categories of Adams predictor-corrector methods and prove that they follow a similar pattern. In particular, if $$p$$ p is the order of the method, AB $$p$$ p -AM $$p$$ p methods have nonzero stability ordinate only for $$p = 1, 2, \ 5, 6,\ 9, 10, \ldots $$ p = 1 , 2 , 5 , 6 , 9 , 10 , ... , and AB( $$p-$$ p - 1)-AM $$p$$ p methods have nonzero stability ordinates only for $$p = 3, 4, \ 7, 8, \ 11, 12, \ldots $$ p = 3 , 4 , 7 , 8 , 11 , 12 , ... . 
540 |a Springer Science+Business Media Dordrecht (outside the USA), 2014 
690 7 |a Adams methods  |2 nationallicence 
690 7 |a Predictor-corrector  |2 nationallicence 
690 7 |a Imaginary stability boundary  |2 nationallicence 
690 7 |a Linear multistep methods  |2 nationallicence 
690 7 |a Finite difference methods  |2 nationallicence 
690 7 |a Stability region  |2 nationallicence 
690 7 |a Stability ordinate  |2 nationallicence 
700 1 |a Ghrist  |D Michelle  |u Department of Mathematical Sciences, United States Air Force Academy, 2354 Fairchild, Suite 6D2, 80840, USAF Academy, CO, USA  |4 aut 
700 1 |a Fornberg  |D Bengt  |u Department of Applied Mathematics, University of Colorado, Campus Box 526, 80309, Boulder, CO, USA  |4 aut 
700 1 |a Reeger  |D Jonah  |u Department of Mathematics and Statistics, Air Force Institute of Technology, 2950 Hobson Way, 45433, WPAFB, OH, USA  |4 aut 
773 0 |t BIT Numerical Mathematics  |d Springer Netherlands  |g 55/3(2015-09-01), 733-750  |x 0006-3835  |q 55:3<733  |1 2015  |2 55  |o 10543 
856 4 0 |u https://doi.org/10.1007/s10543-014-0528-7  |q text/html  |z Onlinezugriff via DOI 
898 |a BK010053  |b XK010053  |c XK010000 
900 7 |a Metadata rights reserved  |b Springer special CC-BY-NC licence  |2 nationallicence 
908 |D 1  |a research-article  |2 jats 
949 |B NATIONALLICENCE  |F NATIONALLICENCE  |b NL-springer 
950 |B NATIONALLICENCE  |P 856  |E 40  |u https://doi.org/10.1007/s10543-014-0528-7  |q text/html  |z Onlinezugriff via DOI 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Ghrist  |D Michelle  |u Department of Mathematical Sciences, United States Air Force Academy, 2354 Fairchild, Suite 6D2, 80840, USAF Academy, CO, USA  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Fornberg  |D Bengt  |u Department of Applied Mathematics, University of Colorado, Campus Box 526, 80309, Boulder, CO, USA  |4 aut 
950 |B NATIONALLICENCE  |P 700  |E 1-  |a Reeger  |D Jonah  |u Department of Mathematics and Statistics, Air Force Institute of Technology, 2950 Hobson Way, 45433, WPAFB, OH, USA  |4 aut 
950 |B NATIONALLICENCE  |P 773  |E 0-  |t BIT Numerical Mathematics  |d Springer Netherlands  |g 55/3(2015-09-01), 733-750  |x 0006-3835  |q 55:3<733  |1 2015  |2 55  |o 10543