{"id":3003011,"date":"2013-05-21T00:00:00","date_gmt":"2018-01-22T00:00:00","guid":{"rendered":""},"modified":"2025-08-12T07:23:34","modified_gmt":"2025-08-12T06:23:34","slug":"p613-specyficzne-ladunki-elektronow-leybold","status":"publish","type":"product","link":"https:\/\/merazet.pl\/en\/product\/p613-specyficzne-ladunki-elektronow-leybold\/","title":{"rendered":"P6.1.3 Specyficzne \u0142adunki elektron\u00f3w – Leybold"},"content":{"rendered":"

\n\t <\/p>\n\n\n\n
\n

\n\t\t\t\t\tP6.1.3.1 Okre\u015blanie specyficznych \u0142adunk\u00f3w wi\u0105zki elektron\u00f3w<\/a><\/p>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

\n\t <\/div>\n
\n\n\n\n
\n\n\n\n
\n

\n\t\t\t\t\t\t\t\t\t\tMasa me elektronu jest niezwykle trudna do wyznaczenia w do\u015bwiadczeniu. \u0141atwiej jest wyznaczy\u0107 \u0142adunek w\u0142a\u015bciwy elektronu<\/p>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

\n\t\t\t\t\t\t <\/div>\n\n\n\n
\n

\n\t\t\t\t\t\t\t\t\t\te =e<\/span><\/p>\n

\n\t\t\t\t\t\t\t\t\t\t     me<\/p>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

\n\n\n\n
\n

\n\t\t\t\t\t\t\t\t\t\t\tz kt\u00f3rego mo\u017cemy obliczy\u0107 mas\u0119 me dla danego \u0142adunku elektronu e.<\/p>\n

\n\t\t\t\t\t\t\t\t\t\t\tW do\u015bwiadczeniu P6.1.3.1, \u015bci\u015ble powi\u0105zane wi\u0105zki elektron\u00f3w s\u0105 odchylane w zamkni\u0119t\u0105 \u015bcie\u017ck\u0119 ko\u0142ow\u0105 za pomoc\u0105 jednorodnego pola magnetycznego w celu wyznaczenia \u0142adunku w\u0142a\u015bciwego elektronu. Pole magnetyczne B odchylaj\u0105ce elektrony w drog\u0119 o danym promieniu r jest wyznaczane w funkcji napi\u0119cia przyspieszaj\u0105cego U. Si\u0142a Lorentza wywo\u0142ana przez pole magnetyczne dzia\u0142a jako si\u0142a do\u015brodkowa. Zale\u017cy od pr\u0119dko\u015bci elektron\u00f3w, kt\u00f3ra jest wyznaczana przez napi\u0119cie przyspieszaj\u0105ce. Tym samym mo\u017cna wyznaczy\u0107 \u0142adunek w\u0142a\u015bciwy elektronu z wielko\u015bci pomiarowych U, B i r zgodnie ze wzroem<\/p>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

\n\t\t\t\t\t\t\t <\/div>\n<\/p><\/div>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n
\n\t\t <\/div>\n<\/div>\n

\n\t <\/p>","protected":false},"excerpt":{"rendered":"

  P6.1.3.1 Okre\u015blanie specyficznych \u0142adunk\u00f3w wi\u0105zki elektron\u00f3w   Masa […]<\/p>\n","protected":false},"featured_media":3405630,"template":"","meta":{"_acf_changed":false,"_members_access_role":[],"_members_access_error":""},"product_brand":[3022459],"product_cat":[3001922],"product_tag":[3015969,3016041,3007212,3008082,3015809],"class_list":["post-3003011","product","type-product","status-publish","has-post-thumbnail","product_brand-leybold","product_cat-fizyka-atomowa-i-jadrowa","product_tag-fizyka","product_tag-fizyka-atomowa-i-jadrowa","product_tag-ld-didactic","product_tag-specyficzne-ladunki-elektronow","product_tag-zestawy-edukacyjne-stoly-elektrotechniczne","first","onbackorder","taxable","shipping-taxable","product-type-simple"],"acf":[],"yoast_head":"\nP6.1.3 Specyficzne \u0142adunki elektron\u00f3w - Leybold - Merazet<\/title>\n<meta name=\"description\" content=\"P6.1.3 Specyficzne \u0142adunki elektron\u00f3w - Leybold. 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