{"title":"博恩霍尔姆深底边界层涡动扩散系数的估计","authors":"V. Paka, V. Zhurbas","doi":"10.1109/BALTIC.2008.4625548","DOIUrl":null,"url":null,"abstract":"Reliable estimate of eddy diffusivity in the bottom boundary layer (BBL) of the Bornholm Deep is the issue of practical importance because it would control dispersion of the chemical warfare agents dumped in the Deep after WW II [Helcom, 1994]. The most common way to arrive at an estimate of the eddy diffusivity, K is to apply a well-known parameterization of mixing in the Baltic halocline due to internal wave instability suggested by [A. Stigebrandt, 1987] K = min(K<sub>max</sub>, alpha/N), where K<sub>max</sub> is the maximum value of K, N is the buoyancy frequency, and alpha =1times10<sup>-7</sup> m<sup>2</sup> s<sup>-2</sup> [H.E.M. Meier, 2007] or alpha = 0.87times10<sup>-7</sup> m<sup>2</sup> s<sup>-2</sup> [H.-U. Lass, 2003] is the empirical constant. Taking N<sub>BBL</sub> =0.02 s<sup>-1</sup> for near-bottom layer and N<sub>halocline</sub> =0.03 s<sup>-1</sup> for the halocline in the Bornholm Deep [J. Elken, 1996] one obtains K<sub>BBL</sub>= 0.5times10<sup>-5</sup> m<sup>2</sup> s<sup>-1</sup> and K<sub>halocline</sub> = 0.33times10<sup>-5</sup> m<sup>2</sup> s<sup>-1</sup>. However, the above estimate of K<sub>BBL</sub> does not take into account the possibility of enhancement of eddy diffusivity in BBL due shear instability of the near-bottom current and a variety of mechanisms of boundary mixing [J.H. Reissmann, 2007]. Numerical simulations based on the Princeton Ocean Model with a second and a half moment turbulence closure by Mellor and Yamada [1982] embedded brought for eddy diffusivity in the Bornholm Deep BBL and the BBL thickness the values of K<sub>BBL1</sub>= 2.5times10<sup>-4</sup> m<sup>2</sup> s<sup>-1</sup> and h<sub>BBL1</sub> = 2 m respectively. Eddy diffusivity in the Bornholm Deep BBL can be also estimated using data of tow-yo CTD profiling in a near-bottom layer performed aboard R/V Shelf in Summer 2006.","PeriodicalId":6307,"journal":{"name":"2008 IEEE/OES US/EU-Baltic International Symposium","volume":"58 1","pages":"1-3"},"PeriodicalIF":0.0000,"publicationDate":"2008-05-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Estimates of eddy diffusivity in bottom boundary layer of the Bornholm Deep\",\"authors\":\"V. Paka, V. Zhurbas\",\"doi\":\"10.1109/BALTIC.2008.4625548\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Reliable estimate of eddy diffusivity in the bottom boundary layer (BBL) of the Bornholm Deep is the issue of practical importance because it would control dispersion of the chemical warfare agents dumped in the Deep after WW II [Helcom, 1994]. The most common way to arrive at an estimate of the eddy diffusivity, K is to apply a well-known parameterization of mixing in the Baltic halocline due to internal wave instability suggested by [A. Stigebrandt, 1987] K = min(K<sub>max</sub>, alpha/N), where K<sub>max</sub> is the maximum value of K, N is the buoyancy frequency, and alpha =1times10<sup>-7</sup> m<sup>2</sup> s<sup>-2</sup> [H.E.M. Meier, 2007] or alpha = 0.87times10<sup>-7</sup> m<sup>2</sup> s<sup>-2</sup> [H.-U. Lass, 2003] is the empirical constant. Taking N<sub>BBL</sub> =0.02 s<sup>-1</sup> for near-bottom layer and N<sub>halocline</sub> =0.03 s<sup>-1</sup> for the halocline in the Bornholm Deep [J. Elken, 1996] one obtains K<sub>BBL</sub>= 0.5times10<sup>-5</sup> m<sup>2</sup> s<sup>-1</sup> and K<sub>halocline</sub> = 0.33times10<sup>-5</sup> m<sup>2</sup> s<sup>-1</sup>. However, the above estimate of K<sub>BBL</sub> does not take into account the possibility of enhancement of eddy diffusivity in BBL due shear instability of the near-bottom current and a variety of mechanisms of boundary mixing [J.H. Reissmann, 2007]. Numerical simulations based on the Princeton Ocean Model with a second and a half moment turbulence closure by Mellor and Yamada [1982] embedded brought for eddy diffusivity in the Bornholm Deep BBL and the BBL thickness the values of K<sub>BBL1</sub>= 2.5times10<sup>-4</sup> m<sup>2</sup> s<sup>-1</sup> and h<sub>BBL1</sub> = 2 m respectively. Eddy diffusivity in the Bornholm Deep BBL can be also estimated using data of tow-yo CTD profiling in a near-bottom layer performed aboard R/V Shelf in Summer 2006.\",\"PeriodicalId\":6307,\"journal\":{\"name\":\"2008 IEEE/OES US/EU-Baltic International Symposium\",\"volume\":\"58 1\",\"pages\":\"1-3\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-05-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2008 IEEE/OES US/EU-Baltic International Symposium\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/BALTIC.2008.4625548\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2008 IEEE/OES US/EU-Baltic International Symposium","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/BALTIC.2008.4625548","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Estimates of eddy diffusivity in bottom boundary layer of the Bornholm Deep
Reliable estimate of eddy diffusivity in the bottom boundary layer (BBL) of the Bornholm Deep is the issue of practical importance because it would control dispersion of the chemical warfare agents dumped in the Deep after WW II [Helcom, 1994]. The most common way to arrive at an estimate of the eddy diffusivity, K is to apply a well-known parameterization of mixing in the Baltic halocline due to internal wave instability suggested by [A. Stigebrandt, 1987] K = min(Kmax, alpha/N), where Kmax is the maximum value of K, N is the buoyancy frequency, and alpha =1times10-7 m2 s-2 [H.E.M. Meier, 2007] or alpha = 0.87times10-7 m2 s-2 [H.-U. Lass, 2003] is the empirical constant. Taking NBBL =0.02 s-1 for near-bottom layer and Nhalocline =0.03 s-1 for the halocline in the Bornholm Deep [J. Elken, 1996] one obtains KBBL= 0.5times10-5 m2 s-1 and Khalocline = 0.33times10-5 m2 s-1. However, the above estimate of KBBL does not take into account the possibility of enhancement of eddy diffusivity in BBL due shear instability of the near-bottom current and a variety of mechanisms of boundary mixing [J.H. Reissmann, 2007]. Numerical simulations based on the Princeton Ocean Model with a second and a half moment turbulence closure by Mellor and Yamada [1982] embedded brought for eddy diffusivity in the Bornholm Deep BBL and the BBL thickness the values of KBBL1= 2.5times10-4 m2 s-1 and hBBL1 = 2 m respectively. Eddy diffusivity in the Bornholm Deep BBL can be also estimated using data of tow-yo CTD profiling in a near-bottom layer performed aboard R/V Shelf in Summer 2006.