2010
DOI: 10.1016/j.jappmathmech.2010.11.005
|View full text |Cite
|
Sign up to set email alerts
|

The stability and stabilization of non-linear, non-stationary mechanical systems

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2014
2014
2022
2022

Publication Types

Select...
4
1

Relationship

0
5

Authors

Journals

citations
Cited by 8 publications
(1 citation statement)
references
References 3 publications
0
1
0
Order By: Relevance
“…This assumption formulates the same properties as Assumption 1, considering nonlinear potential forces and linear dissipative ones (in Assumption 1 the potential forces are linear). Then the system equation can be rewritten as follows: truex¨+𝕎truex˙+Gfalse(xfalse)x=d, and using the approach proposed in Reference 14, let us select a LF in the form: V=h()12truex˙truex˙+Gfalse(xfalse)+12x𝕎x+xtruex˙, where h>0$$ h>0 $$ is a design parameter, then trueV˙=prefix−truex˙()h𝕎prefix−Itruex˙prefix−xGfalse(xfalse)x. Hence, (6) is GSLF for a sufficiently big value of h$$ h $$ for the system (2) under Assumption 2. Let us demonstrate that a mild modification is needed to get ISS:…”
Section: Iss Analysis For the First Systemmentioning
confidence: 99%
“…This assumption formulates the same properties as Assumption 1, considering nonlinear potential forces and linear dissipative ones (in Assumption 1 the potential forces are linear). Then the system equation can be rewritten as follows: truex¨+𝕎truex˙+Gfalse(xfalse)x=d, and using the approach proposed in Reference 14, let us select a LF in the form: V=h()12truex˙truex˙+Gfalse(xfalse)+12x𝕎x+xtruex˙, where h>0$$ h>0 $$ is a design parameter, then trueV˙=prefix−truex˙()h𝕎prefix−Itruex˙prefix−xGfalse(xfalse)x. Hence, (6) is GSLF for a sufficiently big value of h$$ h $$ for the system (2) under Assumption 2. Let us demonstrate that a mild modification is needed to get ISS:…”
Section: Iss Analysis For the First Systemmentioning
confidence: 99%