{"text_format":"1","workbook":"xlsx","n_sheets":1,"sheets":["Sheet1"],"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":"Sheet1","index":0,"n_rows":11,"n_cols":3,"rows_kept":11,"cut":false,"hidden":false,"merged":[]}
[]
[]
[null,"温度T [℃]=",0]
[null,"モル数n [mol]=",1]
[null,"体積V [L]＝",22.4]
[null,"van der Waals定数a [Pa･m6/mol2]=",0.36599999999999999]
[null,"van der Waals定数b [m3/mol]=",4.2799999999999997E-5]
[]
[]
[null,"理想気体法則による圧力P１ [atm]=",1.0008149147033691]
[null,"van der Waalsの式による圧力P2 [atm]=",0.99553012847900391]