{"text_format":"1","workbook":"xlsx","n_sheets":3,"sheets":["Cover","Wandtemperatur","Kreisprozesse"],"not_rendered":{"charts":0,"images":0,"macros":1,"external_links":0,"defined_names":0,"comments":0,"pivot_tables":0},"unopened":[],"bounds":{"document_bytes":16777216,"sheet_cells":100000,"rows_first":2000,"rows_last":500,"rows_between":2000,"halvings":0,"cell_chars":16384,"cell_head_chars":4096},"cells_cut":0,"cells_raw":0,"read":"whole","date_system":"1900"}

{"sheet":"Cover","index":0,"n_rows":20,"n_cols":3,"rows_kept":20,"cut":false,"hidden":false,"merged":[]}
[]
[]
[null,"Excel + VBA"]
[]
[]
[null,"Kapitel",9]
[null,"Thema","Berechnungen aus der Thermodynamik"]
[]
[null,"Inhalt","Nichtstationäre Wärmeströmung durch eine Wand"]
[null,null,"Zustandsänderungen idealer Gase und Kreisprozesse"]
[]
[]
[]
[]
[null,"Autor","Harald Nahrstedt"]
[null,"Datum","2017-03-01"]
[null,"Version","5.0"]
[]
[]
[null,"Springer Vieweg Verlag"]

{"sheet":"Wandtemperatur","index":1,"n_rows":9,"n_cols":1,"rows_kept":9,"cut":false,"hidden":false,"merged":[]}
["Wandstärke x [m]"]
["Schrittanzahl n (max=95)"]
["Wärmeleitfähigkeit L [W/m grd]"]
["Spez. Wärmekapazität c [kJ/kg grd]"]
["Dichte d [kg/m³]"]
["Wärmeübergangszahl-Innen  a1 [W/m² K]"]
["Wärmeübergangszahl-Aussen a2 [W/m² K]"]
["Innentemperatur Ti [grd]"]
["Außentemperatur Ta [grd]"]

{"sheet":"Kreisprozesse","index":2,"n_rows":11,"n_cols":12,"rows_kept":11,"cut":false,"hidden":false,"merged":[]}
["Masse m [kg]",null,null,null,null,null,"->","v [m³/kg]","p [Pa]","W [J]","Wt [J]","Q [J]"]
["Gaskonstante R [J/kg K]"]
["Adiabatenexponent x"]
[]
[]
[]
["Zustand Nr."]
["Zustandsänderung"]
["p [Pa]"]
["v [m³/kg]"]
["T [grd K]"]