2021
DOI: 10.1103/physreve.103.042601
|View full text |Cite
|
Sign up to set email alerts
|

Time-dependent inertia of self-propelled particles: The Langevin rocket

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
48
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
6
3

Relationship

5
4

Authors

Journals

citations
Cited by 44 publications
(54 citation statements)
references
References 105 publications
1
48
0
Order By: Relevance
“…( 10 ) to obtain which yields As a result, the leading asymptotic behavior of is determined by the first term involving a scaling behavior of the MD in . This is remarkably slow compared to typical behavior of a Brownian particle in a harmonic potential or of active Brownian motion where the MD reaches its asymptotic value exponentially in time [ 57 59 ] thus constituting an example of a very slow relaxation as induced by space-dependent noise.…”
Section: Free Particle Casementioning
confidence: 99%
“…( 10 ) to obtain which yields As a result, the leading asymptotic behavior of is determined by the first term involving a scaling behavior of the MD in . This is remarkably slow compared to typical behavior of a Brownian particle in a harmonic potential or of active Brownian motion where the MD reaches its asymptotic value exponentially in time [ 57 59 ] thus constituting an example of a very slow relaxation as induced by space-dependent noise.…”
Section: Free Particle Casementioning
confidence: 99%
“…In Newtonian fluids, the effective selfpropulsion force is proportional and instantaneous in the orientation, and thus the delay function equates to zero for all time. In a similar manner, the inertial delay function was previously defined for macroscopic active particles which measured the mismatch between the particle velocity ṙ(t) and the particle orientation n(t) [5,70,71]. In our overdamped system, this inertial delay function is always zero since the average velocity is aligned with the orientation.…”
Section: General Resultsmentioning
confidence: 92%
“…Our model can be extended to higher spatial dimensions [69], to harmonic confinement [86][87][88][89], to external fields [90,91], and to include inertia [5,70,71,[92][93][94][95] where an analytical solution seems to be in reach as well. Moreover different combinations of friction and memory kernel as well as colored noise can be considered for future work [96][97][98][99][100], for instance, Mittag-Leffler noise [101,102] or power-law memory [103,104].…”
Section: Discussionmentioning
confidence: 99%
“…In conclusion, the PAM both unifies ABPs and AOUPs and provides a crucial step towards more realistic modeling of overdamped (dry) active motion in general, which should in future work be employed to provide an improved fit of experimental swim-velocity distributions. Investigating the effect of the swim-velocity fluctuations could represent an interesting perspective for circle swimming [92][93][94][95][96][97] , systems with spatial-dependent swim velocity [98][99][100][101][102][103] , and inertial dynamics [104][105][106][107][108] even affecting the orientational degrees of freedom 109,110 . The generalization of PAM to these cases could be responsible for new intriguing phenomena which will be investigated in future works.…”
Section: Parental Active Modelmentioning
confidence: 99%