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0468 Report of a Mission to Yarkund in 1873 : vol.1
Report of a Mission to Yarkund in 1873 : vol.1 / Page 468 (Grayscale High Resolution Image)

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[Figure] l SPECIMEN COPY OF COMPUTATION OF ONE DAY'S OBSERVATIONS FOR LONGITUDE AT KASHGHAR. Computation of Longitude from Lunar Zenith Distances. At Kashghar ( Yangi-Shahr) Station, on 28th December 1873 ( Civil Date, P.M.)

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doi: 10.20676/00000196
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SPECIMEN COPY OF COMPUTATION OF ONE DAY'S
Computation of Longitude fr
At Kashghar (Yangi-Shahr) Station, on

Moon { West of Meridian.
Lower Limb observed. Lat. N. = φ = 39 24 32 Assumed

Ref.
No. No. of observation (Mean of F. L. and F. R.) 1 2 3

(1) Chronometer Time of observation ... 10 47 55·2 10 52 31·3 10 57 26·2
(2) Correction ... – 22 20·4 22 20·4 22 20·4
(3) Local Mean Time (Ast. D.) = 28 days ... + 10 25 34·8 10 30 10·9 10 35 5·8
(4) Approx. Gr. Mean Time = (3) + L₁ = 28 days + 5 20 34·8 5 20 10·9 5 30 5·8
(5) ☽'s observed Zenith Distance ... = ζ₁ 46 56 38 47 43 14 48 33 30
(6) Refraction (for B and T) = r ... – 57 59 1 0
(7) ☽'s Semi-diameter at (4) from N. A. = S ... – 16 2 16 2 16 2
(8) From Table I Δ S ... – 11 11 11
(9) (5) + (6) + (7) + (8) = ζ₂ 46 41 22 47 28 0 48 18 17
(10) ☽'s Horizontal Parallax at (4) from N. A. = π' + 58 45 58 44 58 44
(11) From Table II Δ π' + 5 5 5
(12) Log. π₁' = log. (π + Δ π)' ... { 3·54777 3·54765 3·54765
(13) Log. ζ₂ ... { 1·86192 1·86740 1·87314
(14) (12) + (13) = log. (π₁ sin ζ₂)' ... { 3·40969 3·41505 3·42079
(15) π₁ sin ζ₂ ... 42 49 43 20 43 55
(16) (9) − (15) = ζ₂ − π₁ sin ζ₂ = ... ζ₁ 45 58 33 46 44 40 47 34 22
(17) ☽'s Declination at (4) from N.A. = δ 11 57 8 11 58 15 11 59 27
(18) Δδ from Table III ... + 15 15 15
(19) (17) + (18) = δ + Δ δ = δ₁ ... + 11 57 23 11 58 30 11 59 42
(20) φ − (19) = (φ − δ₁) ... 27 27 9 27 26 2 27 24 50
(21) (16) + (20) = ζ₁ + (φ − δ₁) = 2 σ₁ ... 73 25 42 74 10 42 74 59 12
(22) (16) − (20) = ζ₁ − (φ − δ₁) = 2 σ₂ ... 18 31 24 19 18 38 20 9 32
(23) σ₁ ... 36 42 51 37 5 21 37 29 36
(24) σ₂ ... 9 15 42 9 39 19 10 4 46
(25) Log. sin σ₁ ... 1·7765729 1·7803585 1·7843813
(26) Log. sin σ₂ ... 1·2066735 1·2245847 1·2430716
(27) Log. sec φ ... 0·1120256 0·1120256 0·1120256
(28) Log. sec δ₁ ... 0·0095255 0·0095554 0·0095876
(29) (25) + (26) + (27) + (28) = log. sin 2½ t' 1·1047975 1·1265242 1·1490661
(30) Log. sin ½ t ... 1·5523988 1·5632621 1·5745331
(31) t (in arc) ... + 41 48 18 42 54 56 44 6 8
(32) S. T. Gr. Mean Noon on 28 days (see (4)) ... 18 28 5·8 18 28 5·8 18 28 5·8
(33) Local Mean Time (same as (3)) ... 10 25 34·8 10 30 10·9 10 35 5·8
(34) Acceleration for (4) ... 52·7 53·4 54·2
(35) (32) + (33) + (34) = local S. T. of observation = θ 4 54 33·3 4 59 10·1 5 4 5·8
(36) t (in time) deduced from (31) ... + 2 47 13·2 2 51 39·7 2 56 24·5
(37) ☽'s Right Ascension or AR = θ − t ... 2 7 20·1 2 7 30·4 2 7 41·3
(38) Greenwich Mean Time for (37) from N. A. ... 5 21 1·1 5 25 47·8 5 30 51·2
(39) (38) − (33) = Approx. Long. = L₂ ... – 5 4 33·7 5 4 23·1 5 4 14·6
(40) (39) − L₁ = L₂ = L₁ ... = β' + 26·3 36·9 45·4
(41) At (38) change in ☽A R for increment of 1ᵐ = λ' + 2·155 2·155 2·156
(42) Do. Do. Deen. Do. = β' + 14·621 14·615 14·609
(43) Log. cos φ (see (27)) ... 1·8880 1·8880 1·8880
(44) Log. sin t (see (31)) ... 1·8239 1·8331 1·8426
(45) Log. cosec ζ₁ (see (16)) ... 0·1432 0·1377 0·1319