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Seid.lm@, 1988). The TT is d.fined in FlatioD witb the "lnt matioDl A<strong>lo</strong>nic Tine"<br />

T"I=TAI+]2F.IE4<br />

c.l.t)<br />

Btce TAI it dgul.t€d &cording ro atomic rimc, In TAI $c b6ic uoir of rime is thc SI<br />

sond {defined by Bueu Inremarional des Poids.l M.su6, BIPM, in t96?, a<br />

dudlion of9,192,611,770 periods of rodiarions cooesponding ro lh. tmsition b€rween<br />

uo htFrfinc levcls ofd.gbund slat oflneCesinm lll abm G.t tenerat.,2OOt)).<br />

A day on rhk scale is 86400 SI seonds <strong>lo</strong>ng {Astonomicat Atndrc, 200?). On rbe<br />

other hand rhe clet dm." is thc Univ.Ml Tin€ (Ul denned wirb rcf.r.nc€ ro nem<br />

sun and Nocialed vi1h thc Crccnwicn Md Sid@t Tim. (GMST). UT is detircd as<br />

$e hour angle ofrhe Med Sun ar cEenwicb ptus 12i6. Due ro rhe in€euta ries in the<br />

rctations of th€ Eanh ihcr N di$repancies b.reen the lwo rimes. rhe TT and rhc UT.<br />

This dillcrcrce is ruferred ro as $c delht (At):<br />

AI=TT-UT<br />

(2.t.2)<br />

Th.rcaore wh.nevcr w wanl b dd@irc th€ position of $. SM and lhe M@.<br />

lbr a panicular lime on ou! c<strong>lo</strong>cks w€ have to fomutate rhe rine argudenr using rhese<br />

cons'dcEiions othcnvi* fie c<strong>lo</strong>ck dn. of the phcnomena shaU nor be appropriat€.<br />

Finally. rhc lime arSunenl in drc rhcorics requi,es lhe delemimtioh otrh€ Jutim Dare of<br />

the UT in question. TIE Julim Dale is th. sys!€h ofconrinuols limc sle lhar begins o.<br />

Noon or crcen*i.h Jduary t, y6 -4?t2 (cdlcd lhc cpoch oftne..r!lian dde,) ln rhis<br />

r,m€ scare tlre moment described by a date (CEeorie or Julie) ond rine (UT) is<br />

considercd as rhe "nmb.r of dayJ,, d.nor.

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