{"id":1600,"date":"2021-02-09T09:01:18","date_gmt":"2021-02-09T08:01:18","guid":{"rendered":"https:\/\/us.edu.pl\/instytut\/ich\/?page_id=1600"},"modified":"2025-09-10T14:45:35","modified_gmt":"2025-09-10T12:45:35","slug":"aparatura","status":"publish","type":"page","link":"https:\/\/us.edu.pl\/instytut\/ich\/dzialalnosc-naukowa\/aparatura\/","title":{"rendered":"Aparatura"},"content":{"rendered":"

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Aparatura<\/h3>\r\n
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Analizator DSC TA Instrument (zakres -90 do 600 o<\/sup>C)<\/strong><\/p>\n

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Okre\u015blenie parametr\u00f3w termicznych – przemian fazowych w funkcji zadanego przebiegu temperaturowego. Zakres pracy -90 do 600 o<\/sup>C<\/p>\n

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dr S\u0142awomir Ma\u015blanka<\/a><\/p>\n

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Analizator termograwimetryczny SETARAM Labsys evo<\/strong><\/p>\n

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Aparatura pozwala na badania zwi\u0105zane z charakterystyk\u0105 w\u0142a\u015bciwo\u015bci termicznych materia\u0142\u00f3w. Dost\u0119pna aparatura umo\u017cliwia m.in. badanie post\u0119pu procesu degradacji termicznej materia\u0142\u00f3w, identyfikacj\u0119 temperatur przemian fazowych, a tak\u017ce pomiar \u00a0ciep\u0142a przemian fazowych\u00a0 oraz wyznaczanie\u00a0ciep\u0142a w\u0142a\u015bciwego\u00a0substancji.<\/p>\n

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dr in\u017c. Ewa Pietrasik<\/a><\/p>\n

dr Mariola Bartoszek<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Aparat do pomiaru zawarto\u015bci wody w cieczach, SI Analytics Titroline 750 KF Trace<\/strong><\/p>\n

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S\u0142u\u017cy do szybkiego oznaczania wody metod\u0105 kulometryczn\u0105 Karla Fischera, szczeg\u00f3lnie niskiej jej zawarto\u015bci od 1 ppm do ok. 5% dla pr\u00f3bek ciek\u0142ych.<\/p>\n

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dr hab. Monika Geppert-Rybczy\u0144ska, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Aparatura do pomiaru absorpcji ultrad\u017awi\u0119k\u00f3w w cieczach<\/strong><\/p>\n

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Spektroskopia ultrad\u017awi\u0119kowa w cieczach molekularnych i cieczach jonowych w funkcji temperatury i cz\u0119stotliwo\u015bci<\/p>\n

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dr hab. Edward Zor\u0119bski, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Defektoskop ultrad\u017awi\u0119kowy (Krautkramer USM 36)<\/strong><\/p>\n

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Aparatura s\u0142u\u017cy do wykrywania, lokalizacji oraz okre\u015blania wielko\u015bci wad w materia\u0142ach.<\/p>\n

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dr Marta Kuwik<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Densytometr oscylacyjny do pomiaru g\u0119sto\u015bci cieczy z rozdzielczo\u015bci\u0105 1\u00b710-6 g\/cm3, DMA5000 Anton Paar<\/strong><\/p>\n

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Przeprowadzanie pomiar\u00f3w g\u0119sto\u015bci dyspersji ciecz molekularna\/ciecz jonowa + nanostruktury\u00a0 w funkcji temperatury i wyznaczanie wsp\u00f3\u0142czynnika izobarycznej rozszerzalno\u015bci termicznej.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Densytometr oscylacyjny Anton Paar DMA 5000\u00a0 sprz\u0119\u017cony z uk\u0142adem do wysokich ci\u015bnie\u0144 NOVA SWISS 565.0275, przystawk\u0105 wysokoci\u015bnieniow\u0105 Anton Paar DMA HP i przetwornikiem ci\u015bnieniowym HBM Hottinger Baldwin Messtechnik Scout 55<\/strong><\/p>\n

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Pomiary g\u0119sto\u015bci cieczy (cieczy jonowych, paliw, biopaliw, p\u0142yn\u00f3w roboczych) w funkcji temperatury i ci\u015bnienia oraz w oparciu m.in. o te wyniki wyznaczanie zale\u017cno\u015bci temperaturowej wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci adiabatycznej, wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci izotermicznej, izochorycznej pojemno\u015bci cieplnej, ci\u015bnienia wewn\u0119trznego.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a>
\n\"\"<\/a>\"\"<\/a><\/p>\n

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Densytometr oscylacyjny do pomiaru g\u0119sto\u015bci cieczy z rozdzielczo\u015bci\u0105 1\u00b710-6 g\/cm3, DMA5000M Anton Paar<\/strong><\/p>\n

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Przeprowadzanie pomiar\u00f3w g\u0119sto\u015bci cieczy w funkcji temperatury i wyznaczanie wsp\u00f3\u0142czynnika izobarycznej rozszerzalno\u015bci termicznej.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Dwuwi\u0105zkowy spektrofotometr UV\/Vis Evolution 220<\/strong><\/p>\n

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Przyrz\u0105d umo\u017cliwia ocen\u0119 w\u0142a\u015bciwo\u015bci absorpcyjnych pr\u00f3bek ciek\u0142ych oraz sta\u0142ych w zakresie 190 \u2013 1100 nm promieniowania elektromagnetycznego.<\/p>\n

Mo\u017cliwa jest analiza w kontrolowanych warunkach temperaturowych oraz z wykorzystaniem sfery ca\u0142kuj\u0105cej lub sondy \u015bwiat\u0142owodowej.<\/p>\n

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dr Joanna Orze\u0142<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Dyfraktometr rentgenowski Gemini A Ultra<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Dyfraktometr rentgenowski Gemini A Ultra firmy Oxford Diffraction o pe\u0142nej geometrii kappa, wyposa\u017cony w dwa automatycznie prze\u0142\u0105czalne \u017ar\u00f3d\u0142a rentgenowskie dla promieniowania Mo K alfa i Cu K alfa i przystawk\u0119 CryoJet do utrzymania sta\u0142ej temperatury pr\u00f3bki w zakresie pracy od 90 do 490K.<\/p>\n

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prof. dr hab. Jan G. Ma\u0142ecki<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Edukacyjne aparaty rentgenowskie z lampami: wolframow\u0105 i molibdenow\u0105 PHYWE<\/strong><\/p>\n

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Edukacyjny aparat rentgenowski firmy PHYWE jest niezb\u0119dny do nauki i zrozumienia podstawowych zastosowa\u0144 promieniowania rentgenowskiego. Urz\u0105dzenie jest wykorzystywane przez student\u00f3w chemii i technologii chemicznej na II stopniu kszta\u0142cenia.<\/p>\n

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dr Anna \u015awitlicka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Fotometr p\u0142omieniowy BWB XP (BWB Technologies UK Ltd, Newbury, England).<\/strong><\/p>\n

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R\u00f3wnoczesne oznaczanie Na, K, Li, Ca i Ba w pr\u00f3bkach ciek\u0142ych. Granice wykrywalno\u015bci rz\u0119du mg L-1 (ppm).<\/p>\n

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dr Karina Kocot<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Goniometr (analizator kszta\u0142tu kropli) DSA100 Kr\u00fcss<\/strong><\/p>\n

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Aparat s\u0142u\u017cy do pomiaru napi\u0119cia powierzchniowego\/ mi\u0119dzyfazowego metod\u0105 wisz\u0105cej kropli oraz do pomiar\u00f3w k\u0105ta zwil\u017cania i do wyznaczania energii powierzchniowej. Umo\u017cliwia badanie zjawisk adsorpcji\u00a0 zwi\u0105zk\u00f3w powierzchniowo-czynnych na granicach faz.<\/p>\n

Zakres pracy od -5 \u00b0C do\u00a0 + 120\u00b0C.<\/p>\n

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dr hab. Monika Geppert-Rybczy\u0144ska, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Kamera spektralna wysokiej rozdzielczo\u015bci: High Speed and High Res VISNIR Spectral Camera FX10 – zakres spektralny min. 400 do 1000 nm
\n<\/strong><\/p>\n

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Kamera umo\u017cliwia rejestracj\u0119 obraz\u00f3w hiperspektralnych pr\u00f3bek. W ka\u017cdym z pikseli, zawartych w zarejestrowanym obrazie, znajduje si\u0119 widmo spektralne z wybranego przez u\u017cytkownika zakresu Vis- NIR (400 \u2013 1000 nm). Wysoka rozdzielczo\u015b\u0107 uk\u0142adu optycznego umo\u017cliwia rejestrowanie obraz\u00f3w o bardzo dobrej jako\u015bci.<\/p>\n

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prof. dr hab. Micha\u0142 Daszykowski<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Miernik przewodnictwa cieplnego\u00a0 Thermtest THW-L2 w uk\u0142adzie z sond\u0105 pomiarow\u0105 60 mm typu hot-wire oraz \u0142a\u017ani\u0105 such\u0105 oraz komputerem<\/strong><\/p>\n

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Pomiary przewodnictwa cieplnego cieczy, nnaofluid\u00f3w i ionanofluid\u00f3w.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a><\/p>\n

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Mikrokalorymetr DSC SETARAM CALVET sprz\u0119\u017cony z komputerem i kriostatem SETARAM<\/strong><\/p>\n

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Uk\u0142ad do pomiaru izobarycznej pojemno\u015bci cieplnej faz skondensowanych w zakresie temp. 5 \u2013 120o<\/sup>C<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

dr hab. Edward Zor\u0119bski, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Piec rurowy tr\u00f3jstrefowy<\/strong><\/p>\n

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W piecu jest mo\u017cliwo\u015b\u0107 zaprogramowania trzech stref grzejnych o r\u00f3\u017cnych temperaturach. W takich piecach prowadzona jest synteza materia\u0142\u00f3w metod\u0105 gazowego transportu chemicznego, w kt\u00f3rej wymagany jest gradient temperatury.<\/p>\n

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dr hab. Izabela Jendrzejewska, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Piece komorowe<\/strong><\/p>\n

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Piece laboratoryjne komorowe pozwalaj\u0105 na wygrzewanie pr\u00f3bek w wysokich temperaturach. Piec typu FCF 22HM z maksymaln\u0105 temperatur\u0105 grzania 1300o<\/sup>C i piec typu FCF 22M z maksymaln\u0105 temperatur\u0105 grzania 1150o<\/sup>C. Du\u017ce komory wewn\u0119trzne (22 dm3<\/sup>) pozwalaj\u0105 na umieszczenie znacznej ilo\u015bci pr\u00f3bek jednocze\u015bnie. Stabilizacja temperatury zawiera si\u0119 w zakresie do 3\u00b0C a rozk\u0142ad temperatury w komorze roboczej pieca do 5\u00b0C. Sterowanie piecami odbywa si\u0119 za pomoc\u0105 programowanego mikroprocesorowego regulatora temperatury z wy\u015bwietlaczem cyfrowym, umo\u017cliwiaj\u0105cym realizacj\u0119 10 program\u00f3w po 10 cykli w ka\u017cdym programie, pozwalaj\u0105cy na ustawienie op\u00f3\u017anionego czasu startu (do 100 godzin), przyrostu temperatury w odpowiednim czasie, czasu wygrzewania i czasu ch\u0142odzenia.
\nPiece rurowo-strefowe PRS – 55HM i PRS – 55HMpp to elektryczne, oporowe, przelotowe, komorowe piece \u015bredniotemperaturowe z metalowymi przewodami grzejnymi. Maksymalna temperatura pracy ci\u0105g\u0142ej 1200o<\/sup>C, z dok\u0142adno\u015bci\u0105 do 1o<\/sup>C. Piece te s\u0105 wykorzystywane do otrzymywania monokryszta\u0142\u00f3w metod\u0105 gazowego transportu chemicznego, poniewa\u017c mo\u017cliwe jest ustalenie automatyczne dowolnego gradientu temperatur pomi\u0119dzy dwoma ko\u0144cami ampu\u0142y reakcyjnej. W piecu PRS – 55HMpp s\u0105 trzy programatory temperatury co umo\u017cliwia prowadzenie r\u00f3wnocze\u015bnie dw\u00f3ch syntez, natomiast w piecu PRS – 55HM s\u0105 dwa programatory temperatury i tylko jedna reakcja mo\u017ce przebiega\u0107 w danym okresie czasu. Piece te pozwalaj\u0105 na \u015bcis\u0142e zaprogramowanie przebiegu procesu: czasu rozgrzewania do zadanej temperatury, czasu wygrzewania oraz stopniowego ch\u0142odzenia reaktora.<\/span><\/p>\n

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dr hab. Izabela Jendrzejewska, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a>
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Potencjostat AUTOLAB <\/strong>PGSTAT128N serii N<\/strong><\/p>\n

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Niskoszumowy potencjostat\/galwanostat PGSTAT 128N zdolny do mierzenia pr\u0105d\u00f3w si\u0119gaj\u0105cych 800 mA, przy napi\u0119ciu WE-CE do 12 V. Znajduje zastosowanie do prowadzenia zaawansowanych pomiar\u00f3w na niedu\u017cych elektrodach.<\/p>\n

\u00a0<\/span><\/p>\n

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dr Agata Sz\u0142apa-Kula<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Refraktometr METRICON Model 2010\/M Prism Coupler z zestawem 5 laser\u00f3w<\/strong><\/p>\n

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Aparatura umo\u017cliwia wyznaczenie wsp\u00f3\u0142czynnika za\u0142amania \u015bwiat\u0142a dla badanych materia\u0142\u00f3w sta\u0142ych.<\/p>\n

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prof. dr hab. in\u017c. Joanna Pisarska<\/a><\/p>\n

dr Marta Kuwik<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Refraktometr RL3\u00a0 PZO sprz\u0119\u017cony z lamp\u0105 i zasilaczem<\/strong><\/p>\n

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Pomiary wsp\u00f3\u0142czynnika za\u0142amania \u015bwiat\u0142a cieczy w celu potwierdzenia czysto\u015bci pr\u00f3bek wykorzystywanych w badaniach.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Sonikatory ultrad\u017awi\u0119kowe SONICS Vibracell VCX 130 i VCX 500 z sonotrod\u0105 CV18 i komor\u0105 d\u017awi\u0119koch\u0142onn\u0105<\/strong><\/p>\n

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Przygotowywanie dyspersji cieczy jonowych\/molekularnych z nanocz\u0105stkami.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofluorymetr Edinburgh Instruments FLS 980<\/strong><\/p>\n

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Aparat umo\u017cliwia pomiary stacjonarne pr\u00f3bek w ciele sta\u0142ym lub w roztworze oraz\u00a0 pomiary czas\u00f3w \u017cycia w zakresie 15ps do 10s. Wyposa\u017cony jest w bezozonow\u0105 lamp\u0119 ksenonow\u0105 w zakresie 230-1000nm oraz lampy mikrosekundow\u0105 i nanosekundow\u0105 do pomiar\u00f3w czas\u00f3w \u017cycia. Zestaw pulsowych diod LED i laser\u00f3w diodowych pozwala na wzbudzanie pr\u00f3bek w zakresie od 200 do 900nm. Aparat dodatkowo wyposa\u017cony jest w kriostat azotowy do pomiar\u00f3w luminescencji roztwor\u00f3w w zakresie temperatur 77-300K oraz w sfer\u0119 ca\u0142kuj\u0105c\u0105 pozwalaj\u0105c\u0105 na pomiary wydajno\u015bci kwantowej luminescencji w roztworach oraz w ciele sta\u0142ym.<\/p>\n

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dr Anna Maro\u0144<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofluorymetr femtosekundowy z bramkowaniem optycznym FOG 100-DX<\/strong><\/p>\n

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Aparat wyposa\u017cony jest w femtosekundowy oscylator tytanowo-szafirowy zaopatrzony w laser pompuj\u0105cy oraz spektrometr wraz z uk\u0142adem podwajania cz\u0119stotliwo\u015bci (SHG) do wzbudzenia pr\u00f3bki drug\u0105 harmoniczn\u0105 oscylatora Ti:sapp oraz generatorem trzeciej harmonicznej (THG) wsp\u00f3\u0142pracuj\u0105cym z uk\u0142adem podwajania cz\u0119stotliwo\u015bci. Maksymalny zakres pomiaru fluorescencji wynosi 320 – 1600 nm natomiast cz\u0119stotliwo\u015b\u0107 repetycji puls\u00f3w jest\u00a0 w zakresie od 100 kHz do 100 MHz natomiast krok pulsu bramkuj\u0105cego wynosi 2 fs.<\/p>\n

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dr Anna Maro\u0144<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofluorymetr Hitachi F-7000<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Aparat jest szybko skanuj\u0105cym spektrofotometrem fluorescencyjnym (60.000 nm\/min) umo\u017cliwiaj\u0105cym wykonywanie pomiar\u00f3w luminescencji roztwor\u00f3w oraz pr\u00f3bek sta\u0142ych. Dodatkowo mo\u017cliwe jest wykonywanie pomiar\u00f3w czasu \u017cycia fosforescencji do 1 ms. Wyposa\u017cony jest w przystawk\u0119 do pomiar\u00f3w w temperaturze ciek\u0142ego azotu oraz dwa monochromatory pozwalaj\u0105ce na ci\u0105g\u0142y wyb\u00f3r d\u0142ugo\u015bci fali wzbudzenia i emisji fluorescencyjnej.<\/p>\n

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dr Anna Maro\u0144<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofluorymetr Varian<\/strong><\/p>\n

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Przyrz\u0105d rejestruje sygna\u0142 emisyjny (z zakresu UV-Vis) generowany przez sk\u0142adniki pr\u00f3bki na skutek wzbudzenia fal\u0105 elektromagnetyczn\u0105 o wybranej energii (d\u0142ugo\u015bci z zakresu 220 \u2013 800 nm).<\/p>\n

Aparatura umo\u017cliwia badanie w\u0142a\u015bciwo\u015bci spektralnych pr\u00f3bek ciek\u0142ych oraz sta\u0142ych zar\u00f3wno w postaci pojedynczych widm emisyjnych jak i widm ca\u0142kowitej fluorescencji (z ang. Excitation-Emission Matrices \u2013 EEM). Mo\u017cliwa jest analiza w kontrolowanych warunkach temperaturowych oraz z wykorzystaniem mikrop\u0142ytek lub sondy fluorescencyjnej.<\/p>\n

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dr Joanna Orze\u0142<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofotometr UV-Vis (JASCO V-530, Jasco, Japan)<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Dwuwi\u0105zkowy spektrofotometr o zakresie d\u0142ugo\u015bci fal od 190 do 1100 nm wyposa\u017cony w lamp\u0119 deuterow\u0105(D2) do pomiar\u00f3w w zakresie UV oraz halogenow\u0105(WI) do pomiar\u00f3w w zakresie VIS\/NIR.<\/p>\n

Mo\u017cliwo\u015b\u0107 wykonania analizy ilo\u015bciowej, jako\u015bciowej oraz kinetycznej w oparciu o pomiary spektrofotometryczne wybranych zwi\u0105zk\u00f3w organicznych i nieorganicznych.<\/p>\n

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dr hab. Katarzyna Pytlakowska, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofotometr UV-vis <\/strong>Lambda 35 Perkin Elmer<\/strong><\/p>\n

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Aparatura s\u0142u\u017cy do pomiar\u00f3w absorbcji promieniowania elektromagnetycznego z zakresu widzialnego i nadfioletu w pr\u00f3bkach ciek\u0142ych. Pomiary spektrofotometryczne znajduj\u0105 zastosowanie w analizie ilo\u015bciowej, m.in. do oznaczania ca\u0142kowitej zawarto\u015bci polifenoli oraz ca\u0142kowitej pojemno\u015bci antyoksydacyjnej.<\/p>\n

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dr Justyna Polak<\/a><\/p>\n

dr Mariola Bartoszek<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofotometr UV-VIS do mikroobj\u0119to\u015bci – NanoDrop OneC<\/strong><\/p>\n

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Aparat umo\u017cliwia pomiary bezpo\u015brednio w pr\u00f3bce o obj\u0119to\u015bci ju\u017c od 0,5 \u03bcl bez konieczno\u015bci rozcie\u0144czania i zag\u0119szczania pr\u00f3bki jak r\u00f3wnie\u017c w kuwecie. Zakres skanowania 190-850 nm. Zakres st\u0119\u017ce\u0144: dsDNA od 2 do 27,500 ng\/ul; BSA od 0,06 do 820 mg\/ml. Powtarzalno\u015b\u0107 i wiarygodno\u015b\u0107 pomiar\u00f3w zapewnia system kontroli d\u0142ugo\u015bci drogi optycznej.<\/p>\n

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dr Anna \u015awitlicka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofotometr UV-VIS-NIR Nicolet iS50<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Modu\u0142 UV-Vis pozwala na pomiary absorbancji pr\u00f3bek ciek\u0142ych oraz reflektancji pr\u00f3bek proszkowych w zakresie 200-1100 nm, natomiast modu\u0142 NIR pozwala na pomiary pr\u00f3bek sta\u0142ych w\u00a0 zakresie spektralnym 770-3500 nm.<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr Anna \u015awitlicka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrofotometry UV-Vis Lab Aliance 8500 oraz Jasco V630<\/strong><\/p>\n

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Dwuwi\u0105zkowe spektrofotometry UV-Vis Lab Aliance 8500 oraz Jasco V630 umo\u017cliwiaj\u0105ce pomiary absorpcji promieniowania elektromagnetycznego pr\u00f3bek ciek\u0142ych i sta\u0142ych w zakresie od 1100 do 190 nm. Rozdzielczo\u015b\u0107 aparat\u00f3w jest na poziomie 2 nm. Urz\u0105dzenia s\u0105 przystosowane do pomiar\u00f3w kinetycznych w zakresie 0,5, 1, 6, 30 i 60 sekund. Szybko\u015b\u0107 skanowania d\u0142ugo\u015bci fali od 60 do 3,2 nm na minut\u0119. Dane pomiarowe zbierane i prezentowane s\u0105 komputerowo, co umo\u017cliwia ich dalsz\u0119 obr\u00f3bk\u0119.<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr Anna \u015awitlicka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr AAS (iCE 3300, Thermo Scientific)<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Spektrometr atomowej absorpcji z atomizerem p\u0142omieniowym FAAS wyposa\u017cony w palnik tytanowy, uniwersalny, 50 mm, automatycznie regulowany w wi\u0105zce \u015bwiat\u0142a przystosowany do pracy z p\u0142omieniami acetylen\/powietrze oraz podtlenek azotu\/acetylen.<\/p>\n

Oznaczanie jon\u00f3w metali w wodach i pr\u00f3bkach sta\u0142ych po mineralizacji (oznaczanie danego pierwiastka wymaga zastosowania odpowiedniej lampy z katod\u0105 wn\u0119kow\u0105). Granice wykrywalno\u015bci w zakresie 10 \u2013 10000 ng mL-1<\/sup>.<\/p>\n

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dr hab. Barbara Feist, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr AAS (iCE 3500Z, Thermo Scientific)<\/strong><\/p>\n

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Dwukomorowy spektrometr atomowej absorpcji AAS z atomizerem p\u0142omieniowym FAAS oraz piecem grafitowym GFAAS. Wyposa\u017cony w palnik tytanowy, uniwersalny, 50 mm, automatycznie regulowany w wi\u0105zce \u015bwiat\u0142a przystosowany do pracy z p\u0142omieniami acetylen\/powietrze oraz podtlenek azotu\/acetylen, lampy z katod\u0105 wn\u0119kow\u0105 oraz podw\u00f3jn\u0105 korekcj\u0119 t\u0142a: deuterow\u0105 i Zeemana.<\/p>\n

Pozwala na oznaczanie jon\u00f3w metali w wodach i pr\u00f3bkach sta\u0142ych po mineralizacji (oznaczanie danego pierwiastka wymaga zastosowania odpowiedniej lampy z katod\u0105 wn\u0119kow\u0105). Granice wykrywalno\u015bci w zakresie 10 \u2013 10000 ng mL-1<\/sup> dla atomizacji p\u0142omieniowej oraz w zakresie 0,01 \u2013 1 ng mL-1<\/sup> dla atomizacji elektrotermicznej.<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr hab. Barbara Feist, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr absorpcji przej\u015bciowej Ultrafast Helios Fire wraz ze strojonym laserem femtosekundowym Astrella-TOPAS<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Zestaw z\u0142o\u017cony jest z uk\u0142adu laserowego, opartego na laserze pompuj\u0105cym Revolution, kt\u00f3ry jest zintegrowany z zestawem ultraszybkich oscylator\u00f3w Ti:S typu Vitara firmy Coherent generuj\u0105cych femtosekundowe impulsy. Przestrajalny uk\u0142ad tytanowo-szafirowych laser\u00f3w umo\u017cliwia pomiary w ca\u0142ym zakresie widma UV-VIS-NIR.<\/p>\n

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dr Anna Maro\u0144<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr EDXRF (Epsilon3, PANalytical, Holandia)<\/strong><\/p>\n

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Rentgenowski spektrometr fluorescencyjny z dyspersj\u0105 energii EDXRF wyposa\u017cony w lamp\u0119 z anod\u0105 rodow\u0105 o maksymalnej mocy 9 W i detektor\u00a0 SDD.<\/p>\n

Wielopierwiastkowa analiza pr\u00f3bek sta\u0142ych (materia\u0142y lite i proszkowe). Zakres oznaczanych pierwiastk\u00f3w od sodu do uranu. Granice wykrywalno\u015bci na poziomie mg kg-1<\/sup> (ppm) dla pierwiastk\u00f3w o \u015brednich liczbach atomowych.<\/p>\n

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prof. dr hab. Rafa\u0142 Sitko<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr Elektronowego Rezonansu Paramagnetycznego (EPR), Bruker<\/strong><\/p>\n

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Aparatura pozwala na jako\u015bciowe i ilo\u015bciowe badania substancji, zawieraj\u0105cych niesparowane elektrony. Urz\u0105dzenie to pozwala na badanie w\u0142a\u015bciwo\u015bci antyoksydacyjnych \u00a0produkt\u00f3w spo\u017cywczych oraz badanie proces\u00f3w humifikacji w osadach i glebach. Ponadto spektrometr EPR jest wykorzystywany do badania materia\u0142\u00f3w domieszkowanych metalami przej\u015bciowymi i ziem rzadkich.<\/p>\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr Justyna Polak<\/a><\/p>\n

dr Mariola Bartoszek<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr FT-IR Nicolet iS5<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Spektrometr FTIR Nicolet iS5 o zakresie spektralnym 7800-350cm-1<\/sup> i rozdzielczo\u015bci spektralnej lepszej ni\u017c 0,8cm-1<\/sup>.<\/p>\n

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dr Anna \u015awitlicka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr FT-IR Nicolet is50<\/strong><\/p>\n

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Aparatura umo\u017cliwia badania obejmuj\u0105ce charakterystyk\u0119 strukturaln\u0105 pr\u00f3bek sta\u0142ych oraz ciek\u0142ych. Pozwala na badanie przemian strukturalnych materia\u0142\u00f3w w efekcie zmian temperatury, \u015bledzenie post\u0119pu reakcji, wykrywanie zanieczyszcze\u0144, a tak\u017ce przeprowadzenie analizy jako\u015bciowej oraz ilo\u015bciowej badanych substancji.<\/p>\n

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dr Marta Kuwik<\/a><\/p>\n

dr Natalia \u017bak<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr FT-IR, SpectrumOne, Perkin Elmer<\/strong><\/p>\n

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dr S\u0142awomir Ma\u015blanka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr ICP-MS (iCAP RQ, Thermo Scientific)<\/strong><\/p>\n

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Kwadrupolowy spektrometr nas iCAP RQ ICP-MS umo\u017cliwia pomiar wszystkich analit\u00f3w w jednym trybie He \u2013 dyskryminacji energii kinetycznej (He KED). Jest wyposa\u017cony w p\u00f3\u0142przewodnikowy, cyfrowy\u00a0 generator RF o cz\u0119stotliwo\u015bci 27,12 MHz ch\u0142odzony cieczowo. Uk\u0142ad wprowadzania pr\u00f3bki zawiera pomp\u0119 perystaltyczn\u0105, szklany rozpylacz koncentryczny, stabilizowan\u0105 temperaturowo kwarcow\u0105 komor\u0119 mgieln\u0105 ch\u0142odzon\u0105 termoelektrycznie uk\u0142adem Peltiera oraz semi-rozbieralny palnik kwarcowy z centraln\u0105 rurk\u0105 wtryskiwacza o \u015brednicy 2,5 mm, z mo\u017cliwo\u015bci\u0105 stosowania rurek o r\u00f3\u017cnych \u015brednicach.<\/p>\n

Pozwala na oznaczanie jon\u00f3w metali w wodach i pr\u00f3bkach sta\u0142ych po mineralizacji. Granice wykrywalno\u015bci rz\u0119du ng L-1<\/sup> (ppt).<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr hab. Barbara Feist, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr ICP-OES (SpectroBlue, Spectro Analytical Instruments GmbH)<\/strong><\/p>\n

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Optyczny spektrometr emisyjny ze wzbudzeniem w plazmie sprz\u0119\u017conej indukcyjnie ICP-OES wyposa\u017cony w generator ch\u0142odzony powietrzem o cz\u0119stotliwo\u015bci 27,12 MHz i mocy 0,7-1,7 kW, polichromator (165-770 nm) oraz nebulizer typu cross-flow.<\/p>\n

Nieorganiczna analiza jako\u015bciowa i ilo\u015bciowa pr\u00f3bek ciek\u0142ych lub sta\u0142ych po ich wcze\u015bniejszej mineralizacji. Mo\u017cliwo\u015b\u0107 oznaczania ponad 70 pierwiastk\u00f3w, w bardzo szerokim zakresie st\u0119\u017ce\u0144: od 1 ng L-1<\/sup> do 1 g L-1<\/sup>. Granice wykrywalno\u015bci rz\u0119du \u00b5g L-1<\/sup> (ppb).<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr hab. Barbara Feist, prof. U\u015a<\/a><\/p>\n

dr Marzena Dabioch<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr Ramana DXRxi<\/strong><\/p>\n

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Aparatura umo\u017cliwia badania obejmuj\u0105ce charakterystyk\u0119 strukturaln\u0105 pr\u00f3bek sta\u0142ych oraz ciek\u0142ych. Pozwala na badanie przemian strukturalnych materia\u0142\u00f3w w efekcie zmian temperatury, \u015bledzenie post\u0119pu reakcji, wykrywanie zanieczyszcze\u0144, a tak\u017ce przeprowadzenie analizy jako\u015bciowej oraz ilo\u015bciowej badanych substancji.<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr Marta Kuwik<\/a><\/p>\n

dr Natalia \u017bak<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr TXRF (S4T-STAR, Bruker, Niemcy)<\/strong><\/p>\n

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Rentgenowski spektrometr fluorescencyjny z ca\u0142kowitym odbiciem promieniowania TXRF<\/p>\n

wyposa\u017cony w lamp\u0119 z anod\u0105 molibdenow\u0105 o maksymalnej mocy 50 W i detektor \u00a0SDD.<\/p>\n

Ultra\u015bladowa analiza nieorganiczna mikro-pr\u00f3bek ciek\u0142ych. Mo\u017cliwo\u015b\u0107 prowadzenia analizy wielopierwiastkowej; granice wykrywalno\u015bci na poziomie ng mL-1<\/sup> (ppb) zale\u017cne od oznaczanego pierwiastka.<\/p>\n

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prof. dr hab. Rafa\u0142 Sitko<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Spektrometr UV-Vis Lambda Bio 40 z przystawk\u0105 temperaturow\u0105 PTP-1 (zakres: 5-80 o<\/sup>C), Perkin Elmer<\/strong><\/p>\n

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Dwuwi\u0105zkowe spektrofotometr UV-Vis umo\u017cliwiaj\u0105cy pomiary absorpcji promieniowania elektromagnetycznego pr\u00f3bek ciek\u0142ych w zakresie od 1100 do 190 nm.<\/p>\n

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dr S\u0142awomir Ma\u015blanka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Termograwimetr TG, Pyris-1, Perkin\u00a0 Elmer<\/strong><\/p>\n

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Analiza termograwimetryczna oparta na detekcji zmiany masy pr\u00f3bki\u00a0 i zmiany temperatury w funkcji zadanego przebiegu temperaturowego. Zakres pracy aparatu 25 – 900 0<\/sup>C<\/p>\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr S\u0142awomir Ma\u015blanka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Termograwimetr TG, TA Instrument<\/strong><\/p>\n

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Analiza termograwimetryczna oparta na detekcji zmiany masy pr\u00f3bki\u00a0 i zmiany temperatury w funkcji zadanego przebiegu temperaturowego. Zakres pracy aparatu 25 – 900 0<\/sup>C<\/p>\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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dr S\u0142awomir Ma\u015blanka<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Tranzycjometr \u2013 kalorymetr ci\u015bnieniowy<\/strong><\/p>\n

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Kalorymetr umo\u017cliwia r\u00f3wnoczesn\u0105 rejestracj\u0119 przep\u0142ywu ciep\u0142a i zmian obj\u0119to\u015bci badanej substancji wraz z mo\u017cliwo\u015bci\u0105 \u015bledzenia ewolucji przej\u015b\u0107 fazowych i proces\u00f3w b\u0119d\u0105cych wynikiem ci\u0105g\u0142ych zmian temperatury, ci\u015bnienia lub obj\u0119to\u015bci badanej pr\u00f3bki.<\/p>\n

Zakres parametr\u00f3w pracy:
\nT: -70 o<\/sup>C – +400 o<\/sup>C
\nP: pr\u00f3\u017cnia – 500 MPa<\/p>\n

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dr hab. Miros\u0142aw Chor\u0105\u017cewski, prof. U\u015a<\/a><\/p>\n

dr Alexander Rowland Lowe<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a><\/p>\n

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Uk\u0142ad do kalibracji i badania wsp\u00f3\u0142mierno\u015bci termometr\u00f3w:
\n<\/u>2-termostaty po\u0142\u0105czone kaskadowo\/ UT-2\/77 Horyzont, UTU-4 Horyzont
\n– supertermometr FLUKE 1594A
\n– sonda FLUKE Hart Scientific 5628- zasilacz Cobrabid KB-60-01<\/strong><\/p>\n

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Temperatura jest podstawow\u0105 zmienn\u0105 w wszelkich pomiarach fizykochemicznych, dok\u0142adno\u015b\u0107 oraz wsp\u00f3\u0142mierno\u015b\u0107 u\u017cywanych termometr\u00f3w jest kluczowa dla wszelkich bada\u0144. A zatem, w praktyce uk\u0142ad jest zwi\u0105zany z wszystkimi badaniami dotycz\u0105cymi w\u0142a\u015bciwo\u015bci fizykochemicznych faz skondensowanych.<\/p>\n

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dr hab. Edward Zor\u0119bski, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a><\/p>\n

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Uk\u0142ad do pomiaru lepko\u015bci:
\n– termostat w\u0142a\u015bciwy UTU-4 Horyzont z komor\u0105 pozwalaj\u0105c\u0105 na obserwacj\u0119 przep\u0142ywu cieczy przez kapilar\u0119 podczas pomiaru
\n– kontroler temperatury UNIPAN 660
\n– termometr Ertco Hart 850\u00a0 z sond\u0105 platynow\u0105 (400952)<\/strong><\/p>\n

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Prowadzenie pomiar\u00f3w lepko\u015bci w funkcji temperatury<\/p>\n

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dr hab. Edward Zor\u0119bski, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a>
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Uk\u0142ad do pomiaru pr\u0119dko\u015bci propagacji fali ultrad\u017awi\u0119kowej metod\u0105 Pulse Echo Overlap<\/strong><\/p>\n

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Pomiary pr\u0119dko\u015bci propagacji ultrad\u017awi\u0119k\u00f3w w o\u015brodkach ciek\u0142ych ( ciecze molekularne , ciecze jonowe, paliwa, p\u0142yny robocze) pod ci\u015bnieniem atmosferycznym w funkcji temperatury (5-50 o<\/sup>C) oraz w oparciu m.in. o te wyniki wyznaczanie zale\u017cno\u015bci temperaturowej wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci adiabatycznej, wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci izotermicznej, izochorycznej pojemno\u015bci cieplnej, ci\u015bnienia wewn\u0119trznego.<\/p>\n

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dr hab. Edward Zor\u0119bski, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a>
\n\"\"<\/a>\"\"<\/a><\/p>\n

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Uk\u0142ad do pomiaru pr\u0119dko\u015bci ultrad\u017awi\u0119k\u00f3w w cieczach w zakresie temperatury od 10 do 50 o<\/sup>C i ci\u015bnienia do 1000 atm.<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Pomiary pr\u0119dko\u015bci ultrad\u017awi\u0119k\u00f3w cieczy (cieczy jonowych, paliw, biopaliw, p\u0142yn\u00f3w roboczych) pod wysokimi ci\u015bnieniami do 1000 atm. w funkcji temperatury (15-50 o<\/sup>C) oraz wyznaczanie zale\u017cno\u015bci temperaturowej i ci\u015bnieniowej g\u0119sto\u015bci, izobarycznej pojemno\u015bci cieplnej, izochorycznej pojemno\u015bci cieplnej, wsp\u00f3\u0142czynnika izobarycznej rozszerzalno\u015bci termicznej, wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci adiabatycznej, wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci izotermicznej, ci\u015bnienia wewn\u0119trznego.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

dr hab. Miros\u0142aw Chor\u0105\u017cewski, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Uk\u0142ad do pomiaru pr\u0119dko\u015bci ultrad\u017awi\u0119k\u00f3w w cieczach w zakresie temperatury od 10 do 50 o<\/sup>C metod\u0105 Pulse Echo Overlap
\n<\/strong><\/p>\n

\u00a0<\/strong><\/p>\n

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Pomiary pr\u0119dko\u015bci ultrad\u017awi\u0119k\u00f3w cieczy (cieczy jonowych, paliw, biopaliw, p\u0142yn\u00f3w roboczych) w funkcji temperatury (15-50 o<\/sup>C) oraz w oparciu m.in. o te wyniki wyznaczanie zale\u017cno\u015bci temperaturowej wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci adiabatycznej, wsp\u00f3\u0142czynnika \u015bci\u015bliwo\u015bci izotermicznej, izochorycznej pojemno\u015bci cieplnej, ci\u015bnienia wewn\u0119trznego.\u00a0 Skonstruowany w Zak\u0142adzie Chemii Fizycznej Uniwersytetu \u015al\u0105skiego w Katowicach.<\/p>\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

dr hab. Miros\u0142aw Chor\u0105\u017cewski, prof. U\u015a<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a><\/p>\n

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Waga analityczna Sartorius MSA 225S-100-DU<\/strong><\/p>\n

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Odwa\u017canie sk\u0142adnik\u00f3w dyspersji ciecz molekularna + nanocz\u0105stki, mieszanin, roztwor\u00f3w, przygotowywanie pr\u00f3bek do pomiar\u00f3w np. kalorymetrycznych.<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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prof. dr hab. Marzena Dzida<\/a><\/p>\n

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\"\"<\/a><\/p>\n

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Zestaw laserowy do pomiar\u00f3w luminescencji: spektrofluorymetr PTI QuantaMaster QM40 z detektorami UVVIS PMT R928 oraz NIR Hamamatsu H10330B-75, laser Nd:YAG (Opotek Opolette 355 LD), laser femtosekundowy Chameleon<\/strong><\/p>\n

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Aparatura pozwala na badanie w\u0142a\u015bciwo\u015bci luminescencyjnych materia\u0142\u00f3w. Umo\u017cliwia rejestrowanie widm emisyjnych zar\u00f3wno dla pr\u00f3bek sta\u0142ych jak i ciek\u0142ych. Dodatkowo, mo\u017cna wykona\u0107 analiz\u0119 kinetyki zaniku luminescencji materia\u0142\u00f3w.<\/p>\n

\n<\/div>\r\n <\/div>\r\n <\/div>[\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”]\r\n

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prof. dr hab. in\u017c. Joanna Pisarska<\/a><\/p>\n

dr Marta Kuwik<\/a><\/p>\n

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\"\"<\/a>\"\"<\/a><\/p>\n

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I am text block. Click edit button to change this text. Lorem ipsum dolor sit amet, consectetur adipiscing elit. Ut elit tellus, luctus nec ullamcorper mattis, pulvinar dapibus leo.<\/p>\n

[\/vc_column_text]<\/p>","protected":false},"excerpt":{"rendered":"

[vc_row][vc_column][vc_column_text][\/vc_column_text][\/vc_column][\/vc_row][vc_row][vc_column][vc_column_text][\/vc_column_text][\/vc_column][\/vc_row][vc_row][vc_column][vc_column_text][\/vc_column_text][\/vc_column][\/vc_row][vc_row][vc_column][vc_column_text][\/vc_column_text][\/vc_column][\/vc_row][vc_row][vc_column][vc_column_text][\/vc_column_text][\/vc_column][\/vc_row][vc_row][vc_column][vc_column_text][\/vc_column_text][\/vc_column][\/vc_row][vc_row][vc_column][\/vc_column][\/vc_row][vc_row gap=”20″ equal_height=”yes” content_placement=”middle”][vc_column width=”1\/12″][\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1611856745023{background-color: #ebebeb !important;}”][\/vc_column][vc_column width=”3\/12″ css=”.vc_custom_1611856838340{background-color: #ebebeb !important;}”][\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1612855036491{border-top-width: 1px !important;border-right-width: 1px !important;border-bottom-width: 1px !important;border-left-width: 1px !important;background-color: #ebebeb !important;border-left-color: #ebebeb !important;border-left-style: solid !important;border-right-color: #ebebeb !important;border-right-style: solid !important;border-top-color: #ebebeb !important;border-top-style: solid !important;border-bottom-color: #ebebeb !important;border-bottom-style: solid !important;}”][\/vc_column][vc_column width=”3\/12″][\/vc_column][vc_column width=”1\/12″][\/vc_column][\/vc_row][vc_row][vc_column][vc_separator el_width=”70″][\/vc_column][\/vc_row][vc_row gap=”20″ equal_height=”yes” content_placement=”middle”][vc_column width=”1\/12″][\/vc_column][vc_column width=”2\/12″ css=”.vc_custom_1611856745023{background-color: #ebebeb !important;}”][\/vc_column][vc_column width=”3\/12″ css=”.vc_custom_1611856838340{background-color: #ebebeb […]<\/p>\n

Read More…<\/a><\/p>\n","protected":false},"author":99,"featured_media":0,"parent":123,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_expiration-date-status":"","_expiration-date":0,"_expiration-date-type":"","_expiration-date-categories":[],"_expiration-date-options":[]},"acf":[],"_links":{"self":[{"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/pages\/1600"}],"collection":[{"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/users\/99"}],"replies":[{"embeddable":true,"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/comments?post=1600"}],"version-history":[{"count":10,"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/pages\/1600\/revisions"}],"predecessor-version":[{"id":3602,"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/pages\/1600\/revisions\/3602"}],"up":[{"embeddable":true,"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/pages\/123"}],"wp:attachment":[{"href":"https:\/\/us.edu.pl\/instytut\/ich\/wp-json\/wp\/v2\/media?parent=1600"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}