{"id":28965,"date":"2024-03-10T08:22:33","date_gmt":"2024-03-10T09:22:33","guid":{"rendered":"https:\/\/express24.ir\/d\/product\/%d9%85%d9%82%d8%a7%d9%84%d9%87-%d9%85%d8%a7%d9%87%db%8c%d8%aa-%d8%a8%d8%ad%d8%b1%d8%a7%d9%86%db%8c-%d9%86%d9%85%d8%a7%da%af%d8%b1-%d8%a7%d9%86%d8%af%d8%a7%d8%b2%d9%87-%d9%be%d9%84%db%8c%d9%85%d8%b1\/"},"modified":"2024-03-10T16:05:23","modified_gmt":"2024-03-10T17:05:23","slug":"%d9%85%d9%82%d8%a7%d9%84%d9%87-%d9%85%d8%a7%d9%87%db%8c%d8%aa-%d8%a8%d8%ad%d8%b1%d8%a7%d9%86%db%8c-%d9%86%d9%85%d8%a7%da%af%d8%b1-%d8%a7%d9%86%d8%af%d8%a7%d8%b2%d9%87-%d9%be%d9%84%db%8c%d9%85%d8%b1","status":"publish","type":"product","link":"https:\/\/express24.ir\/d\/product\/%d9%85%d9%82%d8%a7%d9%84%d9%87-%d9%85%d8%a7%d9%87%db%8c%d8%aa-%d8%a8%d8%ad%d8%b1%d8%a7%d9%86%db%8c-%d9%86%d9%85%d8%a7%da%af%d8%b1-%d8%a7%d9%86%d8%af%d8%a7%d8%b2%d9%87-%d9%be%d9%84%db%8c%d9%85%d8%b1\/","title":{"rendered":"\u0645\u0642\u0627\u0644\u0647 \u0645\u0627\u0647\u06cc\u062a \u0628\u062d\u0631\u0627\u0646\u06cc \u0646\u0645\u0627\u06af\u0631 \u0627\u0646\u062f\u0627\u0632\u0647 \u067e\u0644\u06cc\u0645\u0631\u0647\u0627"},"content":{"rendered":"<table class=\"table table-striped table-hover\">\n<tbody>\n<tr>\n<td>\u0639\u0646\u0648\u0627\u0646 \u0645\u0642\u0627\u0644\u0647 \u0628\u0647 \u0627\u0646\u06af\u0644\u06cc\u0633\u06cc <\/td>\n<td>Critical Nature of the Size Exponent of Polymers<\/td>\n<\/tr>\n<tr>\n<td>\u0639\u0646\u0648\u0627\u0646 \u0645\u0642\u0627\u0644\u0647 \u0628\u0647 \u0641\u0627\u0631\u0633\u06cc <\/td>\n<td>\u0645\u0642\u0627\u0644\u0647 \u0645\u0627\u0647\u06cc\u062a \u0628\u062d\u0631\u0627\u0646\u06cc \u0646\u0645\u0627\u06af\u0631 \u0627\u0646\u062f\u0627\u0632\u0647 \u067e\u0644\u06cc\u0645\u0631\u0647\u0627<\/td>\n<\/tr>\n<tr>\n<td>\u0646\u0648\u06cc\u0633\u0646\u062f\u06af\u0627\u0646 <\/td>\n<td>Kazumi Suematsu, Haruo Ogura, Seiichi Inayama, Toshihiko Okamoto<\/td>\n<\/tr>\n<tr>\n<td>\u0632\u0628\u0627\u0646 \u0645\u0642\u0627\u0644\u0647 <\/td>\n<td>\u0627\u0646\u06af\u0644\u06cc\u0633\u06cc<\/td>\n<\/tr>\n<tr>\n<td>\u0641\u0631\u0645\u062a \u0645\u0642\u0627\u0644\u0647: <\/td>\n<td>PDF<\/td>\n<\/tr>\n<tr>\n<td>\u062a\u0639\u062f\u0627\u062f \u0635\u0641\u062d\u0627\u062a<\/td>\n<td>10<\/td>\n<\/tr>\n<tr>\n<td>\u062f\u0633\u062a\u0647 \u0628\u0646\u062f\u06cc \u0645\u0648\u0636\u0648\u0639\u0627\u062a  <\/td>\n<td>Soft Condensed Matter,Chemical Physics,\u0645\u0627\u062f\u0647 \u0645\u062a\u0631\u0627\u06a9\u0645 \u0646\u0631\u0645 , \u0641\u06cc\u0632\u06cc\u06a9 \u0634\u06cc\u0645\u06cc\u0627\u06cc\u06cc ,<\/td>\n<\/tr>\n<tr>\n<td>\u062a\u0648\u0636\u06cc\u062d\u0627\u062a    <\/td>\n<td>Submitted 1 March, 2024; originally announced March 2024. , Comments: 10 pages, 10 figures<\/td>\n<\/tr>\n<tr>\n<td>\u062a\u0648\u0636\u06cc\u062d\u0627\u062a \u0628\u0647 \u0641\u0627\u0631\u0633\u06cc    <\/td>\n<td>\u0627\u0631\u0633\u0627\u0644 1 \u0645\u0627\u0631\u0633 2024 \u061b\u062f\u0631 \u0627\u0628\u062a\u062f\u0627 \u0645\u0627\u0631\u0633 2024 \u0627\u0639\u0644\u0627\u0645 \u0634\u062f \u060c \u0646\u0638\u0631\u0627\u062a: 10 \u0635\u0641\u062d\u0647 \u060c 10 \u0634\u06a9\u0644<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<h2>\u0686\u06a9\u06cc\u062f\u0647<\/h2>\n<p style=\"direction:ltr;\">On the basis of the thermodynamic theory of the excluded volume effects, we show that the size exponent varies abruptly, depending on the change of the segment concentration. For linear polymers, the exponent changes discontinuously from $\u03bd=3\/5$ for the isolated system ($\\bar\u03c6=0$) in good solvents to $\u03bd=1\/2$ in the finite concentration ($0<\\bar\u03c6\\le1$), while for branched polymers having $\u03bd_{0}=1\/4$, the corresponding exponent varies from $\u03bd=1\/2$ ($\\bar\u03c6=0$) to $\u03bd\\cong 1\/3$ ($0<\\bar\u03c6\\le1$).<\/p>\n<h2>\u0686\u06a9\u06cc\u062f\u0647 \u0628\u0647 \u0641\u0627\u0631\u0633\u06cc (\u062a\u0631\u062c\u0645\u0647 \u0645\u0627\u0634\u06cc\u0646\u06cc)<\/h2>\n<p>\u0628\u0631 \u0627\u0633\u0627\u0633 \u0646\u0638\u0631\u06cc\u0647 \u062a\u0631\u0645\u0648\u062f\u06cc\u0646\u0627\u0645\u06cc\u06a9\u06cc \u0627\u062b\u0631\u0627\u062a \u062d\u062c\u0645 \u062d\u0630\u0641 \u0634\u062f\u0647 \u060c \u0645\u0627 \u0646\u0634\u0627\u0646 \u0645\u06cc \u062f\u0647\u06cc\u0645 \u06a9\u0647 \u0646\u0645\u0627\u06cc\u0646\u062f\u06af\u06cc \u0627\u0646\u062f\u0627\u0632\u0647 \u0628\u0633\u062a\u0647 \u0628\u0647 \u062a\u063a\u06cc\u06cc\u0631 \u063a\u0644\u0638\u062a \u0642\u0637\u0639\u0647 \u0628\u0647 \u0637\u0648\u0631 \u0646\u0627\u06af\u0647\u0627\u0646\u06cc \u0645\u062a\u0641\u0627\u0648\u062a \u0627\u0633\u062a.\u0628\u0631\u0627\u06cc \u067e\u0644\u06cc\u0645\u0631\u0647\u0627\u06cc \u062e\u0637\u06cc \u060c \u0646\u0645\u0627\u06cc\u0646\u062f\u0647 \u0628\u0647 \u0637\u0648\u0631 \u0646\u0627\u067e\u06cc\u0648\u0633\u062a\u0647 \u0627\u0632 $ \u03bd = 3\/5 $ \u0628\u0631\u0627\u06cc \u0633\u06cc\u0633\u062a\u0645 \u062c\u062f\u0627 \u0634\u062f\u0647 ($ \\ bar\u03c6 = 0 $) \u062f\u0631 \u062d\u0644\u0627\u0644 \u0647\u0627\u06cc \u062e\u0648\u0628 \u0628\u0647 $ \u03bd = 1\/2 $ \u062f\u0631 \u063a\u0644\u0638\u062a \u0645\u062d\u062f\u0648\u062f (0 $ <\\ bar\u03c6 \\ le1 \u062a\u063a\u06cc\u06cc\u0631 \u0645\u06cc \u06a9\u0646\u062f.$) \u060c \u062f\u0631 \u062d\u0627\u0644\u06cc \u06a9\u0647 \u0628\u0631\u0627\u06cc \u067e\u0644\u06cc\u0645\u0631\u0647\u0627\u06cc \u0634\u0627\u062e\u0647 \u062f\u0627\u0631 \u06a9\u0647 \u062f\u0627\u0631\u0627\u06cc $ \u03bd_ {0} = 1\/4 $ \u0647\u0633\u062a\u0646\u062f \u060c \u0645\u0623\u0645\u0648\u0631 \u0645\u0631\u0628\u0648\u0637\u0647 \u0627\u0632 $ \u03bd = 1\/2 $ ($ \\ bar\u03c6 = 0 $) \u062a\u0627 $ \u03bd \\ cong 1\/3 $ \u0645\u062a\u0641\u0627\u0648\u062a \u0627\u0633\u062a (0 $ 0 $<\\ bar\u03c6 \\ le1 $).\n\n\n\n\n\n[sc name=\"paperTranslation2\"][\/sc]\n<\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u0639\u0646\u0648\u0627\u0646 \u0645\u0642\u0627\u0644\u0647 \u0628\u0647 \u0627\u0646\u06af\u0644\u06cc\u0633\u06cc Critical Nature of the Size Exponent of Polymers \u0639\u0646\u0648\u0627\u0646 \u0645\u0642\u0627\u0644\u0647 \u0628\u0647 \u0641\u0627\u0631\u0633\u06cc \u0645\u0642\u0627\u0644\u0647 \u0645\u0627\u0647\u06cc\u062a \u0628\u062d\u0631\u0627\u0646\u06cc \u0646\u0645\u0627\u06af\u0631 [&hellip;]<\/p>\n","protected":false},"featured_media":27,"comment_status":"open","ping_status":"closed","template":"","meta":{"pmpro_default_level":"","site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"default","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center 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