Self-propelled particle in an external potential: existence of an effective temperature
We study a stationary state of a single self-propelled, athermal particle in linear and quadratic external potentials. The self-propulsion is modeled as a fluctuating internal driving force evolving according to the Ornstein-Uhlenbeck process, independently of the state of the particle. Without an e...
Saved in:
Published in | Physical review. E, Statistical, nonlinear, and soft matter physics Vol. 90; no. 1; p. 012111 |
---|---|
Main Author | |
Format | Journal Article |
Language | English |
Published |
United States
14.07.2014
|
Subjects | |
Online Access | Get more information |
Cover
Loading…
Abstract | We study a stationary state of a single self-propelled, athermal particle in linear and quadratic external potentials. The self-propulsion is modeled as a fluctuating internal driving force evolving according to the Ornstein-Uhlenbeck process, independently of the state of the particle. Without an external potential, in the long time limit, the self-propelled particle moving in a viscous medium performs diffusive motion, which allows one to identify an effective temperature. We show that in the presence of a linear external potential the stationary state distribution has an exponential form with the sedimentation length determined by the effective temperature of the free self-propelled particle. In the presence of a quadratic external potential the stationary state distribution has a Gaussian form. However, in general, this distribution is not determined by the effective temperature of the free self-propelled particle. |
---|---|
AbstractList | We study a stationary state of a single self-propelled, athermal particle in linear and quadratic external potentials. The self-propulsion is modeled as a fluctuating internal driving force evolving according to the Ornstein-Uhlenbeck process, independently of the state of the particle. Without an external potential, in the long time limit, the self-propelled particle moving in a viscous medium performs diffusive motion, which allows one to identify an effective temperature. We show that in the presence of a linear external potential the stationary state distribution has an exponential form with the sedimentation length determined by the effective temperature of the free self-propelled particle. In the presence of a quadratic external potential the stationary state distribution has a Gaussian form. However, in general, this distribution is not determined by the effective temperature of the free self-propelled particle. |
Author | Szamel, Grzegorz |
Author_xml | – sequence: 1 givenname: Grzegorz surname: Szamel fullname: Szamel, Grzegorz organization: Department of Chemistry, Colorado State University, Fort Collins, Colorado 80525, USA |
BackLink | https://www.ncbi.nlm.nih.gov/pubmed/25122255$$D View this record in MEDLINE/PubMed |
BookMark | eNo1j9tKxDAYhIMo7kFfwAvJC3RN_jRt6p0srgoLXqh4ueTwBytpG9Ls4r69xcPFMHzDMDALctoPPRJyxdmKcyZu4sdxTHjAVcNWjAPn_ITMuZSsAFFXM7IYx0_GBAhVnpMZSA4AUs7J-wsGX8Q0RAwBHY065dYGpG1PdU_xK2PqdaBxyNjnVofbKWvHCSzSwf90vEeb2wPSjF3EpPM-4QU58zqMePnnS_K2uX9dPxbb54en9d22sCVXuTCmYiBs5XxjsKyNbJwxsmocTFJiggpro73hpdNGW6GQlcZxCQZUrRQsyfXvbtybDt0uprbT6bj7fwjfQUBW6g |
CitedBy_id | crossref_primary_10_1016_j_physa_2019_121574 crossref_primary_10_21468_SciPostPhys_13_3_065 crossref_primary_10_1103_PhysRevE_106_014605 crossref_primary_10_1103_PhysRevE_103_052602 crossref_primary_10_1103_PhysRevLett_126_208102 crossref_primary_10_1103_PhysRevResearch_6_013190 crossref_primary_10_1088_1742_5468_aaa78c crossref_primary_10_1103_PhysRevE_103_052603 crossref_primary_10_1103_PhysRevE_95_052608 crossref_primary_10_1103_PhysRevApplied_14_054042 crossref_primary_10_1088_1742_5468_ab7e2e crossref_primary_10_1103_PhysRevE_98_020604 crossref_primary_10_1063_1_5110262 crossref_primary_10_1103_PhysRevE_109_024124 crossref_primary_10_1063_1_5048698 crossref_primary_10_1103_PhysRevE_103_062415 crossref_primary_10_1088_1674_1056_aba60d crossref_primary_10_1088_1742_5468_ad5435 crossref_primary_10_1088_1742_5468_ab14dd crossref_primary_10_1103_PhysRevResearch_2_023207 crossref_primary_10_1088_1361_648X_ab3e90 crossref_primary_10_1088_1742_5468_ac3d37 crossref_primary_10_1088_1367_2630_aa914e crossref_primary_10_1016_j_cocis_2022_101603 crossref_primary_10_1103_PhysRevE_106_054617 crossref_primary_10_1103_PhysRevE_108_064205 crossref_primary_10_1063_1_5085752 crossref_primary_10_1103_PhysRevE_99_012145 crossref_primary_10_1209_0295_5075_133_60002 crossref_primary_10_1088_1367_2630_aa9b4d crossref_primary_10_1140_epje_i2018_11739_y crossref_primary_10_3390_sym13010081 crossref_primary_10_1088_1751_8121_ab9cf3 crossref_primary_10_1103_PhysRevResearch_2_043262 crossref_primary_10_1103_PhysRevE_107_024112 crossref_primary_10_1088_1751_8121_acfc09 crossref_primary_10_1103_PhysRevE_108_054607 crossref_primary_10_1103_PhysRevE_108_054606 crossref_primary_10_1063_1_5080537 crossref_primary_10_1103_PhysRevLett_123_238003 crossref_primary_10_1140_epje_s10189_022_00176_4 crossref_primary_10_1103_PhysRevLett_131_158302 crossref_primary_10_1103_PhysRevE_109_014103 crossref_primary_10_1088_1367_2630_ac44e6 crossref_primary_10_1088_1742_5468_acf70c crossref_primary_10_7554_eLife_76406 crossref_primary_10_1103_PhysRevE_107_054130 crossref_primary_10_1039_D0SM00687D crossref_primary_10_1088_1402_4896_acc289 crossref_primary_10_1016_j_physa_2022_128342 crossref_primary_10_1103_PhysRevLett_129_178001 crossref_primary_10_1103_PhysRevE_95_050103 crossref_primary_10_1039_D1SM01648B crossref_primary_10_1088_1367_2630_aae732 crossref_primary_10_1103_PhysRevE_102_052405 crossref_primary_10_1039_D0SM00711K crossref_primary_10_1039_D0SM02273J crossref_primary_10_1103_PhysRevE_96_062608 crossref_primary_10_1103_PhysRevE_102_042605 crossref_primary_10_1103_PhysRevE_99_062608 crossref_primary_10_1039_D4SM00338A crossref_primary_10_1063_1_4991731 crossref_primary_10_1103_PhysRevE_100_032123 crossref_primary_10_1039_C8SM01840E crossref_primary_10_1088_1742_5468_abefe2 crossref_primary_10_1103_PhysRevLett_123_260602 crossref_primary_10_1063_5_0049239 crossref_primary_10_1088_0953_8984_28_25_253001 crossref_primary_10_1103_PhysRevE_98_062610 crossref_primary_10_1103_PhysRevLett_129_138002 crossref_primary_10_1103_PhysRevE_107_054602 crossref_primary_10_1103_PhysRevE_101_022608 crossref_primary_10_1007_s10955_021_02787_1 crossref_primary_10_1063_1_5090104 crossref_primary_10_1103_PhysRevLett_119_258001 crossref_primary_10_1088_1751_8121_ac96db crossref_primary_10_1103_PhysRevE_93_012603 crossref_primary_10_1103_PhysRevE_107_034110 crossref_primary_10_1209_0295_5075_acc96a crossref_primary_10_1063_5_0051315 crossref_primary_10_1039_D0SM00006J crossref_primary_10_1088_1361_648X_aceba9 crossref_primary_10_1103_PhysRevE_106_034608 crossref_primary_10_1103_PhysRevLett_124_248003 crossref_primary_10_1103_PhysRevX_5_011004 crossref_primary_10_1209_0295_5075_127_34003 crossref_primary_10_1063_5_0084213 crossref_primary_10_1103_PhysRevE_99_012118 crossref_primary_10_1039_D3SM00793F crossref_primary_10_1146_annurev_conmatphys_031218_013554 crossref_primary_10_1038_s41467_023_42713_5 crossref_primary_10_1088_1742_5468_abe29e crossref_primary_10_1038_nphys3435 crossref_primary_10_1039_D3SM00358B crossref_primary_10_1103_PhysRevE_108_024605 crossref_primary_10_1016_j_physa_2018_07_055 crossref_primary_10_1103_PhysRevE_108_024602 crossref_primary_10_1103_PhysRevResearch_2_033518 crossref_primary_10_1103_PhysRevE_91_062124 crossref_primary_10_1039_C6SM01322H crossref_primary_10_1103_PhysRevE_94_052602 crossref_primary_10_1103_PhysRevE_107_014604 crossref_primary_10_1007_s40042_023_00797_8 crossref_primary_10_1073_pnas_2318106121 crossref_primary_10_1021_acs_macromol_3c02488 crossref_primary_10_1103_PhysRevE_96_052605 crossref_primary_10_1063_5_0138256 crossref_primary_10_1063_5_0056506 crossref_primary_10_1039_C7SM01648D crossref_primary_10_1088_1742_5468_abffce crossref_primary_10_1103_PhysRevE_92_032301 crossref_primary_10_1103_PhysRevLett_131_057101 crossref_primary_10_1103_PhysRevE_97_032604 crossref_primary_10_1088_1361_648X_accd36 crossref_primary_10_1063_5_0173374 crossref_primary_10_1140_epjs_s11734_024_01188_1 crossref_primary_10_1063_5_0097863 crossref_primary_10_1039_C7SM01504F crossref_primary_10_1142_S021947751940008X crossref_primary_10_1088_1742_5468_abc7b7 crossref_primary_10_1134_S1811238218020108 crossref_primary_10_1088_1751_8121_aa546b crossref_primary_10_1063_5_0030940 crossref_primary_10_1088_1742_5468_aa8c1f crossref_primary_10_1063_5_0131080 crossref_primary_10_1103_PhysRevE_105_034113 crossref_primary_10_1103_PhysRevE_90_062304 crossref_primary_10_1140_epjst_e2015_02457_0 crossref_primary_10_1039_C6SM00889E crossref_primary_10_1088_1742_5468_abe6fd crossref_primary_10_1103_PhysRevLett_125_208001 crossref_primary_10_1038_s41598_018_36824_z crossref_primary_10_1073_pnas_2101964118 crossref_primary_10_1103_PhysRevE_100_012601 crossref_primary_10_1103_PhysRevLett_125_208003 crossref_primary_10_1140_epjb_e2016_70359_0 crossref_primary_10_1088_1742_5468_aa8c37 crossref_primary_10_1088_1367_2630_ac1d37 crossref_primary_10_1080_00268976_2020_1867250 crossref_primary_10_1039_D0SM02162H crossref_primary_10_1088_1742_5468_abee22 crossref_primary_10_1103_PhysRevE_90_052130 crossref_primary_10_1209_0295_5075_112_28004 crossref_primary_10_1038_s42005_024_01540_w crossref_primary_10_1063_5_0074072 crossref_primary_10_1039_D2SM01421A crossref_primary_10_1209_0295_5075_111_60006 crossref_primary_10_1088_1361_648X_aad14f crossref_primary_10_1103_PhysRevE_108_024121 crossref_primary_10_1088_1361_648X_ac2c3f crossref_primary_10_1038_s41598_019_52420_1 crossref_primary_10_1088_1742_5468_abffd4 crossref_primary_10_1039_D1SM01798E crossref_primary_10_1103_PhysRevLett_117_038103 crossref_primary_10_1103_PhysRevE_94_022612 crossref_primary_10_3389_fphy_2020_00229 crossref_primary_10_3390_e26060439 crossref_primary_10_1039_D1SM01163D crossref_primary_10_1103_PhysRevResearch_5_033208 crossref_primary_10_1103_PhysRevX_9_021009 crossref_primary_10_1039_C8CP04419H crossref_primary_10_3389_fphy_2020_582992 crossref_primary_10_1103_PhysRevLett_131_228202 crossref_primary_10_1140_epje_i2020_11992_5 crossref_primary_10_1016_j_physa_2017_12_137 crossref_primary_10_1039_D0SM00339E crossref_primary_10_1039_D2CP01313D crossref_primary_10_1103_PhysRevLett_127_278002 crossref_primary_10_1063_1_5093240 crossref_primary_10_1039_C7SM00852J crossref_primary_10_1142_S0217979223502077 crossref_primary_10_1103_PhysRevE_100_050603 crossref_primary_10_1103_PhysRevE_105_014415 crossref_primary_10_1039_C8SM02492H crossref_primary_10_1103_PhysRevE_107_024609 crossref_primary_10_1103_PhysRevE_102_012609 crossref_primary_10_1209_0295_5075_ac9c28 crossref_primary_10_1103_PhysRevE_102_022607 crossref_primary_10_3390_e19070356 crossref_primary_10_1088_1367_2630_aa9d4b crossref_primary_10_1088_1751_8121_ad02cc crossref_primary_10_1103_PhysRevE_91_062304 crossref_primary_10_1103_PhysRevE_101_032131 crossref_primary_10_1039_C7SM00613F crossref_primary_10_1103_PhysRevE_97_012601 crossref_primary_10_1063_5_0029710 crossref_primary_10_1103_PhysRevE_97_012602 crossref_primary_10_1103_PhysRevE_95_022606 crossref_primary_10_1103_PhysRevE_108_044603 crossref_primary_10_1103_PhysRevE_105_044603 crossref_primary_10_1038_s42254_021_00406_2 crossref_primary_10_1039_C6SM01898J crossref_primary_10_1063_1_5086390 crossref_primary_10_1209_0295_5075_114_68004 crossref_primary_10_3390_e19050193 crossref_primary_10_1016_j_chaos_2021_111500 crossref_primary_10_1103_PhysRevLett_124_118002 crossref_primary_10_1063_5_0179375 crossref_primary_10_1103_PhysRevE_103_032607 crossref_primary_10_1103_PhysRevE_95_012115 crossref_primary_10_1063_1_5086152 crossref_primary_10_1209_0295_5075_117_50010 crossref_primary_10_1039_D3SM00034F crossref_primary_10_1103_PhysRevLett_127_150602 crossref_primary_10_1038_s42005_022_00886_3 crossref_primary_10_1103_PhysRevE_105_044610 crossref_primary_10_1063_5_0096710 crossref_primary_10_1103_PhysRevResearch_6_013156 crossref_primary_10_1103_PhysRevLett_129_048002 |
ContentType | Journal Article |
DBID | CGR CUY CVF ECM EIF NPM |
DOI | 10.1103/physreve.90.012111 |
DatabaseName | Medline MEDLINE MEDLINE (Ovid) MEDLINE MEDLINE PubMed |
DatabaseTitle | MEDLINE Medline Complete MEDLINE with Full Text PubMed MEDLINE (Ovid) |
DatabaseTitleList | MEDLINE |
Database_xml | – sequence: 1 dbid: NPM name: PubMed url: https://proxy.k.utb.cz/login?url=http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed sourceTypes: Index Database – sequence: 2 dbid: EIF name: MEDLINE url: https://proxy.k.utb.cz/login?url=https://www.webofscience.com/wos/medline/basic-search sourceTypes: Index Database |
DeliveryMethod | no_fulltext_linktorsrc |
Discipline | Physics |
EISSN | 1550-2376 |
ExternalDocumentID | 25122255 |
Genre | Research Support, U.S. Gov't, Non-P.H.S Research Support, Non-U.S. Gov't Journal Article |
GroupedDBID | --- -~X 123 2-P 29O 3MX 6TJ 8NH ACGFO AENEX AEQTI AFDAS AFFNX AFGMR AGDNE AJQPL ALMA_UNASSIGNED_HOLDINGS AUAIK CGR CS3 CUY CVF DU5 EBS ECM EIF EJD F5P MVM NPBMV NPM OHT P2P RNS S7W TN5 WH7 XFK XJT YNT ZPR |
ID | FETCH-LOGICAL-c418t-bb6023c6df9be47b59dbb569d269d83dbb6e7bafb14dabac38e04bd152b287882 |
IngestDate | Thu May 23 23:19:57 EDT 2024 |
IsPeerReviewed | true |
IsScholarly | true |
Issue | 1 |
Language | English |
LinkModel | OpenURL |
MergedId | FETCHMERGED-LOGICAL-c418t-bb6023c6df9be47b59dbb569d269d83dbb6e7bafb14dabac38e04bd152b287882 |
PMID | 25122255 |
ParticipantIDs | pubmed_primary_25122255 |
PublicationCentury | 2000 |
PublicationDate | 2014-07-14 |
PublicationDateYYYYMMDD | 2014-07-14 |
PublicationDate_xml | – month: 07 year: 2014 text: 2014-07-14 day: 14 |
PublicationDecade | 2010 |
PublicationPlace | United States |
PublicationPlace_xml | – name: United States |
PublicationTitle | Physical review. E, Statistical, nonlinear, and soft matter physics |
PublicationTitleAlternate | Phys Rev E Stat Nonlin Soft Matter Phys |
PublicationYear | 2014 |
SSID | ssj0032384 |
Score | 2.6199975 |
Snippet | We study a stationary state of a single self-propelled, athermal particle in linear and quadratic external potentials. The self-propulsion is modeled as a... |
SourceID | pubmed |
SourceType | Index Database |
StartPage | 012111 |
SubjectTerms | Models, Theoretical Motion Temperature |
Title | Self-propelled particle in an external potential: existence of an effective temperature |
URI | https://www.ncbi.nlm.nih.gov/pubmed/25122255 |
Volume | 90 |
hasFullText | |
inHoldings | 1 |
isFullTextHit | |
isPrint | |
link | http://utb.summon.serialssolutions.com/2.0.0/link/0/eLvHCXMwnV1LS8QwEA4-ELyI77fk4G1Jbbdpt_Um4gNBEXRxb0umTUBwu0X3IPvrnWna2t1VfBy2bJtQQr7JZGY684Wx47YBg9uyJ-hsbSG9xBVxEPkCdIw7hG-iJKRq5Nu78Lorb3pBr_HFlKpLRuAk4y_rSv6DKj5DXKlK9g_I1i_FB_gf8cUrIozXX2H8oF-MyCmcjt5_2srLLhTDUETebwmeW_lwRDlB6qU4huedgKXlTBkAWZnQQflDxFJVUiw3Tdb7Cklb5eK0Lmx2GJVFFIFwus0s44aqs0HfUL23BgV5Zxk9qY33h7Ea2NyAq9cxVciMm6EHT1JM05Z8OrpUl4ErKK-mqU_t8Z8TcmOVY0En532tt13ij6DhEHGVE7vObGeco3xQIEk2Geqh4OfWKS7tqmmezXci0od3FNux-7aPxousyqpc_2R2MEQcXb5gygkpjJHHVbZSehH8zOK9xuZ0ts6WLFJvG-xpUjB4JRj8OeMq49VoeS0Yp7wWCz40RZ9KLHhDLDZZ9_Li8fxalCdoiER60UgAhLjikjA1MWjZgSBOAYIwTtv4i3y8CXUHlAFPpgpU4kfalZCiTQfoSaPztcUWUID0DuOAZkzb7WipvViaJI3aEKVhoiQo8NDO3GXbdkb6uaVJ6Vdztfdtyz5b_hSrA7ZocF3qQzTyRnBUYPMB5E5Vwg |
link.rule.ids | 786 |
linkProvider | National Library of Medicine |
openUrl | ctx_ver=Z39.88-2004&ctx_enc=info%3Aofi%2Fenc%3AUTF-8&rfr_id=info%3Asid%2Fsummon.serialssolutions.com&rft_val_fmt=info%3Aofi%2Ffmt%3Akev%3Amtx%3Ajournal&rft.genre=article&rft.atitle=Self-propelled+particle+in+an+external+potential%3A+existence+of+an+effective+temperature&rft.jtitle=Physical+review.+E%2C+Statistical%2C+nonlinear%2C+and+soft+matter+physics&rft.au=Szamel%2C+Grzegorz&rft.date=2014-07-14&rft.eissn=1550-2376&rft.volume=90&rft.issue=1&rft.spage=012111&rft_id=info:doi/10.1103%2Fphysreve.90.012111&rft_id=info%3Apmid%2F25122255&rft_id=info%3Apmid%2F25122255&rft.externalDocID=25122255 |