R1i^dZddlZddlZddlmZddlZddlZejdk(Z ejZ GddejZd dZ dZ Gd d e Zy) z)Helpers for making Skyfield tests stable.N)earthlibic eZdZdZedZy)datetimeNc"tjSN)r _fake_nowX/home/cursorai/projects/iching/venv/lib/python3.12/site-packages/skyfield/tests/fixes.pynowz datetime.nows!!!r )__name__ __module__ __qualname__r staticmethodr r r r rr sI""r rc tdtj|tjj ddtj _fdtjj_ t_ tt_y)Npandas.F)verbosecSrr )selffake_nows r zsetup..shr ) __import__dtrskyfieldiokitLoaderapiloadtimelib Timescale_utcnowr)utcrs @r setupr$s^x{{C H --c5-AHLL)>H&!HBKr ctjjdtj_t j jtjj_ tt _y)Nr) rrrrrrrutcnowr r!r"_real_datetime_classr r r teardownr(sB --c2HLL)+););H&&BKr c"eZdZdZdZdZdZy)low_precision_ERAa9Compute the Earth rotation angle with only a single float for UT1. Skyfield now uses two floats ``t.whole`` and ``t.ut1_fraction`` to represent the UT1 Julian date, supplying an additional 16 digits of precision. For the Earth rotation angle, which moves very quickly per unit time compared to most other astronomical quantities, this knocks Skyfield out of agreement with other libraries like NOVAS and SOFA that round UT1 to a single float. Various tests use this context manager to make Skyfield match the lower-precision output. cXtj|_|jt_yr)rearth_rotation_anglesavedera)rs r __enter__zlow_precision_ERA.__enter__/s22 (,%r c.|jt_yr)r-rr,)rargss r __exit__zlow_precision_ERA.__exit__2s(, %r c.||z}|j|Sr)r-)rwholefractionrounded_single_floats r r.zlow_precision_ERA.era4s$x/zz.//r N)r rr__doc__r/r2r.r r r r*r*#s 130r r*))i r8)r7rrsysrr skyfield.apiskyfield.timelibmaxsize IS_32_BITr'r$r(objectr*r r r r@sU/  [[J & {{"r{{" ' 00r