Results 1 to 10 of about 13 (13)
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2023
Ð Ñ Ð¾Ð´Ðµ данной вÑпÑÑкной квалиÑикаÑионной ÑабоÑÑ Ð±Ñл пÑоведен анализ ÑазлиÑнÑÑ Â Ð¿Ð¾Ð´Ñ Ð¾Ð´Ð¾Ð² к опÑеделениÑ ÑÑÑноÑÑи и ÑодеÑÐ¶Ð°Ð½Ð¸Ñ Ð¿Ñавового ÑÑаÑÑÑа адвокаÑа. ÐзÑÑÐµÐ½Ñ Ð¾ÑобенноÑÑи ноÑмаÑивно-пÑ
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Ð Ñ Ð¾Ð´Ðµ данной вÑпÑÑкной квалиÑикаÑионной ÑабоÑÑ Ð±Ñл пÑоведен анализ ÑазлиÑнÑÑ Â Ð¿Ð¾Ð´Ñ Ð¾Ð´Ð¾Ð² к опÑеделениÑ ÑÑÑноÑÑи и ÑодеÑÐ¶Ð°Ð½Ð¸Ñ Ð¿Ñавового ÑÑаÑÑÑа адвокаÑа. ÐзÑÑÐµÐ½Ñ Ð¾ÑобенноÑÑи ноÑмаÑивно-пÑ
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2023
This work is devoted to the numerical simulation of free convective stationary laminar and non-stationary transient flow of molten iron in a square cavity and a cubic cavity with and without the influence of an external magnetic field. The main results lie in the flow fields presented in the paper and in the dependences of the Nusselt number on ...
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This work is devoted to the numerical simulation of free convective stationary laminar and non-stationary transient flow of molten iron in a square cavity and a cubic cavity with and without the influence of an external magnetic field. The main results lie in the flow fields presented in the paper and in the dependences of the Nusselt number on ...
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2021
ÐбÑекÑом иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ ÑвлÑеÑÑÑ Ð¸ÑÑледование меÑодов повÑÑÐµÐ½Ð¸Ñ ÐºÐ°ÑеÑÑва ÑаÑÐ¿Ð¾Ð·Ð½Ð°Ð²Ð°Ð½Ð¸Ñ Ð´Ð»Ñ ÑадиолокаÑионнÑÑ Ð´ÐµÑекÑоÑов в задаÑÐ°Ñ Ð¿Ð¾ÑÑобÑабоÑки Ñигналов. ÐÑедмеÑом иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ ÑвлÑеÑÑÑ Ñади
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ÐбÑекÑом иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ ÑвлÑеÑÑÑ Ð¸ÑÑледование меÑодов повÑÑÐµÐ½Ð¸Ñ ÐºÐ°ÑеÑÑва ÑаÑÐ¿Ð¾Ð·Ð½Ð°Ð²Ð°Ð½Ð¸Ñ Ð´Ð»Ñ ÑадиолокаÑионнÑÑ Ð´ÐµÑекÑоÑов в задаÑÐ°Ñ Ð¿Ð¾ÑÑобÑабоÑки Ñигналов. ÐÑедмеÑом иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ ÑвлÑеÑÑÑ Ñади
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2021
ÐÐ°Ð½Ð½Ð°Ñ ÑабоÑа поÑвÑÑена ÑÐ¾Ð·Ð´Ð°Ð½Ð¸Ñ Ð¿ÑогÑаммно-аппаÑаÑного имиÑаÑоÑа Ð´Ð»Ñ Ð¿ÑовеÑки ÑабоÑÑ ÑадиолокаÑионнÑÑ ÑиÑÑем Ñ ÐºÐ»Ð°ÑÑиÑикаÑией движÑÑегоÑÑ Ð¾Ð±ÑекÑа.
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ÐÐ°Ð½Ð½Ð°Ñ ÑабоÑа поÑвÑÑена ÑÐ¾Ð·Ð´Ð°Ð½Ð¸Ñ Ð¿ÑогÑаммно-аппаÑаÑного имиÑаÑоÑа Ð´Ð»Ñ Ð¿ÑовеÑки ÑабоÑÑ ÑадиолокаÑионнÑÑ ÑиÑÑем Ñ ÐºÐ»Ð°ÑÑиÑикаÑией движÑÑегоÑÑ Ð¾Ð±ÑекÑа.
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2021
ÐÐ°Ð½Ð½Ð°Ñ ÑабоÑа поÑвÑÑена иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ ÑилÑÑÑов ÑиÑÑем ÑÐ»ÐµÐ¶ÐµÐ½Ð¸Ñ Ð·Ð° кодом и неÑÑÑей в пÑиÑмнике Ñигналов ÑпÑÑниковÑÑ Ð½Ð°Ð²Ð¸Ð³Ð°ÑионнÑÑ ÑиÑÑем пÑи ÑазлиÑной динамике ÑиÑÑÐµÐ¼Ñ ÑпÑÑник-пÑиÑмник. Ð ÑÑед
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ÐÐ°Ð½Ð½Ð°Ñ ÑабоÑа поÑвÑÑена иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ ÑилÑÑÑов ÑиÑÑем ÑÐ»ÐµÐ¶ÐµÐ½Ð¸Ñ Ð·Ð° кодом и неÑÑÑей в пÑиÑмнике Ñигналов ÑпÑÑниковÑÑ Ð½Ð°Ð²Ð¸Ð³Ð°ÑионнÑÑ ÑиÑÑем пÑи ÑазлиÑной динамике ÑиÑÑÐµÐ¼Ñ ÑпÑÑник-пÑиÑмник. Ð ÑÑед
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2019
The work for the master's degree is devoted to the study of the temperature dependence of the Nernst-Ettingshausen effect in lightly doped samples of bismuth HTSCs in the Bi-2212 system. The first chapter of this work is a brief review of the literature containing information necessary for carrying out the work about high-temperature superconductors ...
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The work for the master's degree is devoted to the study of the temperature dependence of the Nernst-Ettingshausen effect in lightly doped samples of bismuth HTSCs in the Bi-2212 system. The first chapter of this work is a brief review of the literature containing information necessary for carrying out the work about high-temperature superconductors ...
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2019
The master's thesis is devoted to the study of the possibility of reducing the program execution time for simulating the spin polarization of alkali metal atoms through the use of sparse matrix technologies. A program with a significantly shorter simulation time has been developed. Functionality of the Intel MKL library was used.
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The master's thesis is devoted to the study of the possibility of reducing the program execution time for simulating the spin polarization of alkali metal atoms through the use of sparse matrix technologies. A program with a significantly shorter simulation time has been developed. Functionality of the Intel MKL library was used.
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2018
Ð¦ÐµÐ»Ñ Ð´Ð°Ð½Ð½Ð¾Ð¹ ÑабоÑÑ â полÑÑение инÑоÑмаÑии о ÑнеÑгеÑиÑеÑком ÑпекÑÑе ÑиÑÑÐµÐ¼Ñ Y_(1-x) ãCa_x Baã_2 Cu_2.8 Zn_0.2 O_y пÑÑем анализа ÑемпеÑаÑÑÑнÑÑ Ð·Ð°Ð²Ð¸ÑимоÑÑей коÑÑÑиÑÐ¸ÐµÐ½Ñ Ð° ÐеÑнÑÑа в ÑÐ°Ð¼ÐºÐ°Ñ Ð¼Ð¾Ð´ÐµÐ»Ð¸ Ñзкой зонÑ.
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Ð¦ÐµÐ»Ñ Ð´Ð°Ð½Ð½Ð¾Ð¹ ÑабоÑÑ â полÑÑение инÑоÑмаÑии о ÑнеÑгеÑиÑеÑком ÑпекÑÑе ÑиÑÑÐµÐ¼Ñ Y_(1-x) ãCa_x Baã_2 Cu_2.8 Zn_0.2 O_y пÑÑем анализа ÑемпеÑаÑÑÑнÑÑ Ð·Ð°Ð²Ð¸ÑимоÑÑей коÑÑÑиÑÐ¸ÐµÐ½Ñ Ð° ÐеÑнÑÑа в ÑÐ°Ð¼ÐºÐ°Ñ Ð¼Ð¾Ð´ÐµÐ»Ð¸ Ñзкой зонÑ.
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2017
ÐакалавÑÑÐºÐ°Ñ ÑабоÑа поÑвÑÑена иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ Ð¾Ð´Ð½Ð¾Ð³Ð¾ из наиболее акÑÑалÑнÑÑ Ð²Ð¾Ð¿ÑоÑов: повÑÑÐµÐ½Ð¸Ñ Ð¿Ð¾Ð¶Ð°Ñной безопаÑноÑÑи обÑекÑа ÑоÑиалÑного назнаÑениÑ, в ÑаÑÑноÑÑи.
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ÐакалавÑÑÐºÐ°Ñ ÑабоÑа поÑвÑÑена иÑÑÐ»ÐµÐ´Ð¾Ð²Ð°Ð½Ð¸Ñ Ð¾Ð´Ð½Ð¾Ð³Ð¾ из наиболее акÑÑалÑнÑÑ Ð²Ð¾Ð¿ÑоÑов: повÑÑÐµÐ½Ð¸Ñ Ð¿Ð¾Ð¶Ð°Ñной безопаÑноÑÑи обÑекÑа ÑоÑиалÑного назнаÑениÑ, в ÑаÑÑноÑÑи.
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