Matches in SemOpenAlex for { <https://semopenalex.org/work/W1986125950> ?p ?o ?g. }
- W1986125950 endingPage "195" @default.
- W1986125950 startingPage "173" @default.
- W1986125950 abstract "A two-degree-of-freedom system with a clearance and subjected to harmonic excitation is considered. The correlative relationship and matching law between dynamic performance and system parameters are studied by multi-parameter and multi-performance co-simulation analysis. Two key parameters of the system, the exciting frequency ω and clearance δ, are emphasized to reveal the influence of the main factors on dynamic performance of the system. Diversity and evolution of periodic impact motions are analyzed. The fundamental group of impact motions is defined, which have the period of exciting force and differ by the numbers p and q of impacts occurring at the left and right constraints of the clearance. The occurrence mechanism of chattering-impact vibration of the system is studied. As the clearance δ is small or small enough, the transition from 1–p–p to 1–(p+1)–(p+1) motion (the fundamental group of motions, p≥1) basically goes through the processes as follows: pitchfork bifurcation of symmetric 1–p–p motion, period-doubling bifurcation of asymmetric 1–p–p motion, non-periodic or chaotic motions caused by a succession of period-doubling bifurcations, symmetric 1–(p+1)–(p+1) motion generated by a degeneration of chaos. As for slightly large clearance, a series of grazing bifurcations of periodic symmetrical impact motions occur with decreasing the exciting frequency so that the number p of impacts of the fundamental group of motions increases two by two. As p becomes big enough, the incomplete chattering-impact motion will appear which exhibits a chattering sequence in an excitation period followed by a finite sequence of impacts with successively reduced velocity and reaches the non-sticking region. Finally, the complete chattering-impact motion with sticking will occur with decreasing the exciting frequency ω up to the sliding bifurcation boundary. A series of singular points on the boundaries between existence regions of any adjacent symmetrical impact motions with fundamental period are found, i.e., two different saddle-node bifurcation boundaries of one of them, real-grazing and bare-grazing bifurcation boundaries of the other alternately and mutually cross themselves at the points of intersection and create inevitably two types of transition regions: narrow hysteresis and small tongue-shaped regions. A series of zones of regular periodic and subharmonic impact motions are found to exist in the tongue-shaped regions. Based on the sampling ranges of parameters, the influence of dynamic parameters on impact velocities, existence regions and correlative distribution of different types of periodic-impact motions of the system is emphatically analyzed." @default.
- W1986125950 created "2016-06-24" @default.
- W1986125950 creator A5013245200 @default.
- W1986125950 creator A5015200358 @default.
- W1986125950 creator A5070930365 @default.
- W1986125950 date "2014-10-01" @default.
- W1986125950 modified "2023-10-16" @default.
- W1986125950 title "Vibro-impact dynamics of a two-degree-of freedom periodically-forced system with a clearance: Diversity and parameter matching of periodic-impact motions" @default.
- W1986125950 cites W141067971 @default.
- W1986125950 cites W1968807360 @default.
- W1986125950 cites W1971396077 @default.
- W1986125950 cites W1973207641 @default.
- W1986125950 cites W1976342870 @default.
- W1986125950 cites W1980400741 @default.
- W1986125950 cites W1981848010 @default.
- W1986125950 cites W1982068359 @default.
- W1986125950 cites W1982071062 @default.
- W1986125950 cites W1984838918 @default.
- W1986125950 cites W1985631618 @default.
- W1986125950 cites W1993275372 @default.
- W1986125950 cites W1999621897 @default.
- W1986125950 cites W2001455529 @default.
- W1986125950 cites W2006526220 @default.
- W1986125950 cites W2009303015 @default.
- W1986125950 cites W2010465603 @default.
- W1986125950 cites W2011227277 @default.
- W1986125950 cites W2011261230 @default.
- W1986125950 cites W2012069094 @default.
- W1986125950 cites W2012141200 @default.
- W1986125950 cites W2013145460 @default.
- W1986125950 cites W2015439518 @default.
- W1986125950 cites W2017785162 @default.
- W1986125950 cites W2019981623 @default.
- W1986125950 cites W2022219519 @default.
- W1986125950 cites W2023395984 @default.
- W1986125950 cites W2023583323 @default.
- W1986125950 cites W2024100940 @default.
- W1986125950 cites W2025470515 @default.
- W1986125950 cites W2027856518 @default.
- W1986125950 cites W2030468449 @default.
- W1986125950 cites W2033225924 @default.
- W1986125950 cites W2033564707 @default.
- W1986125950 cites W2036572162 @default.
- W1986125950 cites W2039786400 @default.
- W1986125950 cites W2040522568 @default.
- W1986125950 cites W2042223562 @default.
- W1986125950 cites W2044696154 @default.
- W1986125950 cites W2048889405 @default.
- W1986125950 cites W2049752618 @default.
- W1986125950 cites W2053037136 @default.
- W1986125950 cites W2053979403 @default.
- W1986125950 cites W2057687314 @default.
- W1986125950 cites W2062902686 @default.
- W1986125950 cites W2064003018 @default.
- W1986125950 cites W2066552154 @default.
- W1986125950 cites W2070582878 @default.
- W1986125950 cites W2073578998 @default.
- W1986125950 cites W2077945947 @default.
- W1986125950 cites W2079167716 @default.
- W1986125950 cites W2079644436 @default.
- W1986125950 cites W2080041960 @default.
- W1986125950 cites W2087157925 @default.
- W1986125950 cites W2087424619 @default.
- W1986125950 cites W2090022960 @default.
- W1986125950 cites W2094734627 @default.
- W1986125950 cites W2103902597 @default.
- W1986125950 cites W2111319451 @default.
- W1986125950 cites W2119721925 @default.
- W1986125950 cites W2132384949 @default.
- W1986125950 cites W2134056441 @default.
- W1986125950 cites W2141264251 @default.
- W1986125950 cites W2144249884 @default.
- W1986125950 cites W2145669299 @default.
- W1986125950 cites W2159609028 @default.
- W1986125950 cites W2326250702 @default.
- W1986125950 doi "https://doi.org/10.1016/j.ijnonlinmec.2014.04.013" @default.
- W1986125950 hasPublicationYear "2014" @default.
- W1986125950 type Work @default.
- W1986125950 sameAs 1986125950 @default.
- W1986125950 citedByCount "40" @default.
- W1986125950 countsByYear W19861259502015 @default.
- W1986125950 countsByYear W19861259502016 @default.
- W1986125950 countsByYear W19861259502017 @default.
- W1986125950 countsByYear W19861259502018 @default.
- W1986125950 countsByYear W19861259502019 @default.
- W1986125950 countsByYear W19861259502020 @default.
- W1986125950 countsByYear W19861259502021 @default.
- W1986125950 countsByYear W19861259502022 @default.
- W1986125950 countsByYear W19861259502023 @default.
- W1986125950 crossrefType "journal-article" @default.
- W1986125950 hasAuthorship W1986125950A5013245200 @default.
- W1986125950 hasAuthorship W1986125950A5015200358 @default.
- W1986125950 hasAuthorship W1986125950A5070930365 @default.
- W1986125950 hasBestOaLocation W19861259502 @default.
- W1986125950 hasConcept C104114177 @default.
- W1986125950 hasConcept C121332964 @default.
- W1986125950 hasConcept C134306372 @default.
- W1986125950 hasConcept C154945302 @default.