Finite-correlation-time effects in the kinematic dynamo problem
Most of the theoretical results on the kinematic amplification of small-scale magnetic fluctuations by turbulence have been confined to the model of white-noise-like (δ-correlated in time) advecting turbulent velocity field. In this work, the statistics of the passive magnetic field in the diffusion...
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| Format: | Journal article |
| Language: | English |
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2001
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| _version_ | 1826297003861082112 |
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| author | Schekochihin, A Kulsrud, R |
| author_facet | Schekochihin, A Kulsrud, R |
| author_sort | Schekochihin, A |
| collection | OXFORD |
| description | Most of the theoretical results on the kinematic amplification of small-scale magnetic fluctuations by turbulence have been confined to the model of white-noise-like (δ-correlated in time) advecting turbulent velocity field. In this work, the statistics of the passive magnetic field in the diffusion-free regime are considered for the case when the advecting flow is finite-time correlated. A new method is developed that allows one to systematically construct the correlation-time expansion for statistical characteristics of the field such as its probability density function or the complete set of its moments. The expansion is valid provided the velocity correlation time is smaller than the characteristic growth time of the magnetic fluctuations. This expansion is carried out up to first order in the general case of a d-dimensional arbitrarily compressible advecting flow. The growth rates for all moments of the magnetic-field strength are derived. The effect of the first-order corrections due to the finite correlation time is to reduce these growth rates. It is shown that introducing a finite correlation time leads to the loss of the small-scale statistical universality, which was present in the limit of the δ-correlated velocity field. Namely, the shape of the velocity time-correlation profile and the large-scale spatial structure of the flow become important. The latter is a new effect, that implies, in particular, that the approximation of a locally-linear shear flow does not fully capture the effect of nonvanishing correlation time. Physical applications of this theory include the small-scale kinematic dynamo in the interstellar medium and protogalactic plasmas. © 2001 American Institute of Physics. |
| first_indexed | 2024-03-07T04:25:00Z |
| format | Journal article |
| id | oxford-uuid:cc4fe11e-8c4d-4485-b490-559a2e96f3f3 |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-07T04:25:00Z |
| publishDate | 2001 |
| record_format | dspace |
| spelling | oxford-uuid:cc4fe11e-8c4d-4485-b490-559a2e96f3f32022-03-27T07:21:03ZFinite-correlation-time effects in the kinematic dynamo problemJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:cc4fe11e-8c4d-4485-b490-559a2e96f3f3EnglishSymplectic Elements at Oxford2001Schekochihin, AKulsrud, RMost of the theoretical results on the kinematic amplification of small-scale magnetic fluctuations by turbulence have been confined to the model of white-noise-like (δ-correlated in time) advecting turbulent velocity field. In this work, the statistics of the passive magnetic field in the diffusion-free regime are considered for the case when the advecting flow is finite-time correlated. A new method is developed that allows one to systematically construct the correlation-time expansion for statistical characteristics of the field such as its probability density function or the complete set of its moments. The expansion is valid provided the velocity correlation time is smaller than the characteristic growth time of the magnetic fluctuations. This expansion is carried out up to first order in the general case of a d-dimensional arbitrarily compressible advecting flow. The growth rates for all moments of the magnetic-field strength are derived. The effect of the first-order corrections due to the finite correlation time is to reduce these growth rates. It is shown that introducing a finite correlation time leads to the loss of the small-scale statistical universality, which was present in the limit of the δ-correlated velocity field. Namely, the shape of the velocity time-correlation profile and the large-scale spatial structure of the flow become important. The latter is a new effect, that implies, in particular, that the approximation of a locally-linear shear flow does not fully capture the effect of nonvanishing correlation time. Physical applications of this theory include the small-scale kinematic dynamo in the interstellar medium and protogalactic plasmas. © 2001 American Institute of Physics. |
| spellingShingle | Schekochihin, A Kulsrud, R Finite-correlation-time effects in the kinematic dynamo problem |
| title | Finite-correlation-time effects in the kinematic dynamo problem |
| title_full | Finite-correlation-time effects in the kinematic dynamo problem |
| title_fullStr | Finite-correlation-time effects in the kinematic dynamo problem |
| title_full_unstemmed | Finite-correlation-time effects in the kinematic dynamo problem |
| title_short | Finite-correlation-time effects in the kinematic dynamo problem |
| title_sort | finite correlation time effects in the kinematic dynamo problem |
| work_keys_str_mv | AT schekochihina finitecorrelationtimeeffectsinthekinematicdynamoproblem AT kulsrudr finitecorrelationtimeeffectsinthekinematicdynamoproblem |