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सिद्धान्तशिरोमणि: गणिताध्याय (भास्कराचार्य - ग्रहगणित, मध्यमाधिकार व स्पष्टाधिकार सटीक)

Siddhanta Shiromani Ganitadhyaya of Bhaskaracharya with Commentary

भास्कराचार्य द्वितीय द्वारा

DevanagariHindipublished573 पृष्ठ

291 Comm. Under verse 58, we had to form Hvers h; a doubt might arise as to what this Hvers h would be if h > 90. Hence Bhāskara defines it and the definition is clear from fig. 57. The Unmandala S'anku has the formula R sin δ sin φ so that either when δ is negative or when φ is negative, it will be negative which means it will be in the opposite direction ie. vertically downwards. Since negative latitudes are not considered by the Hindu astronomers, the other case alone is considered. Even from a figure it is evident that when the Sun is in the south of the Equator, the Unmandala S'anku is vertically downwards. In proportions like I given under verse 62, we can use the magnitude of this Unmandala S'anku also and it does not vitiate the results, when we take its numerical value. Verse 65. The Sun crosses the prime-vertical when his northern declination falls short of the latitude. Then alone there is sense in giving the magnitude of his shadow at that moment. When the Sun does not cross the prime- vertical at all, the Sama S'anku which could be computed out of its formulation, though it does not exist, under the Sun, yet, it could be used in proportions (like I under verse 62) and no blunder is committed. Comm. This is a beautiful example cited by Bhāskara where he intuitively uses the so-called principle of geometrical continuity. We have formulated Sama S'anku as (R sin δ) / (sin φ) ie. H cos z = (R sin δ) / (sin φ) . We have a real value of z when δ > φ, for, then only H cos z < R. When φ > δ, then H cos z > R which is impossible, for, no Hindu sine or Hindu cosine could be greater than R just as no modern sine or cosine could be greater than unity.

292 TERMINOLOGY N.B.—In as much this Tripraśnādhyāya has a good number of technical terms whose understanding is necessary to understand the Hindu methods of solving diurnal problems, we shall collect here all such technical terms under this heading for guidance.

Technical termMeaning in modern termsSymbol if anyFormula numberOccurs under verseHindu formulaModern formula
Dṛk-jyāHindu sine of the Zenith-distanceH sin z98H sin zR = 3438<br>R sin z
DṛgamsacāpaZenith-distanceZ
Digjyā*Hindu azimuth measured from the East pointH sin aH sin aR sin a
KrāntijyāH sine of declinationH sin δH sin δR sin δ
AkshajyāH sine of latitudeH

293

Technical termMeaning in modern termsSymbol if anyFormula numberOccurs under verseHindu formulaModern formula
ChāyābhujaPerpendicular from the extremity of the shadow on the East-west line.b38(K H sin z × H sin a) / R²K sin z sin a
Chāyākoṭi√(s² — b²)7"(K H sin z × H cos a) / R²K sin z cos a
ViṣhuvatchāyaGnomonic shadow cast at mid-day on the equi-noctial day at any places"(12 H sin φ) / (H cos φ)12 tan φ
ViṣhuvatkarṇaHypot. of the △, one side being sk"√(s² + 12²)12 sec φ
AgrajyāHindu sine of rising azi-muthA5"(R H sin δ) / (H cos φ)(R sin δ) / Cos φ
KarṇāgraAgrajyā reduced from a circle of radius R to one with radius Ka6"(K H sin δ) / (H cos φ)(K sin δ) / Cos φ
Iṣṭa ŚaṅkuThe Hindu cosine of ZI. S.8"H cos zR cos z
Iṣṭa HṛtiThe hypot. of the △, one side being H cos zI. H.1113–17(R H cos z) / (H cos φ)(R cos z) / Cos φ

294

ŚankutalaThe thrid side of the Δ, aboveS. T.1213-17(H cos z H sin δ) / (H cos φ)R cos z tan φ
KujyāThe ⊥ᵃʳ distance bet. The lines drawn parallel to the east-west line through the rising point and the point of intersection of the diurnal circle and the great circle PEω13/(H sin δ H sin φ) / (H cos φ)R sin δ tan φ
Vishuvat-mandalaCelestial Equator
Krānti MandalaEcliptic
KshitijaHorizon
UnmandalaGreat circle PEω or Equatorial horizon
Yāmyottara-mandalaMeridian
SamamandalaPrime-vertical
Dṛk MandalaVertical
Dhṛva Prota VṛttaDeclination circle

295

Technical termMeaning in modern termsSymbol if anyFormula numberOccurs under verseHindu formulaModern formula
Kadamba Prota VṛttaCircle of celestial latitude
KrāntiHindu declination ie: arc of the declination circle intercepted bet. Ecliptic and Equator
Spaṣṭa KrāntiDeclination
Dhṛvaka or DhṛvaCelestial long measured from the Hindu zero point
Sāyana DhṛvaCelestial longitude
VikṣepaPolar latitude or the arc of the declination circle intercepted bet. the Ecliptic and the celestial body
Sphuṭa VikṣepaCelestial latitude
Vishuvāṁsa CāpaRight ascension
NameDescriptionTextCh.VerseFormula (with H)Formula
AntyāThe length of the ⊥ ar drawn from Q the culminating point of the celestial Equator on the line drawn parallel to the East-west line through the foot of the declination circle of the rising celestial body1413-17R + (R H sin φ H sin δ) / (H cos φ H cos δ)R (1 + tan δ tan φ)
Sama-ŚaṅkuH cos z when the body is on the prime-verticalS. S.1720(R H sin δ) / (H sin φ)R sin δ / sin φ
TaddhṛtiPerpendicular distance between the lines drawn parallel to the East-west line through the rising point and the point where the diurnal circle cuts the prime-vertical18(R² H sin φ) / (H cos δ H sin φ)(R sin δ) / (Cos φ sin δ)
PūrvāparāEast-west line
Udayāsta SūtraLine joining the rising and setting points
Unmaṇḍala ŚaṅkuH cos z when the body is on the Equatorial HorizonU. S.1925(H sin δ H sin φ) / RR sin δ sin φ
Dinārdha ŚaṅkuH cos z at the culminating pointD. S.2131-32H cos (φ ~+ δ)R cos (φ ~+ δ)
296

297

Technical termMeaning in modern termsSymbol if anyFormula numberOccurs under verseHindu formulaModern formula
YaṣṭiThe length of the $\perp^{ar}$ dropped from the culminating point on a plane parallel to the Horizon and passing thro/ the point of intersection of the diurnal circle and Equatorial horizonY2133$\dfrac{H cos \varphi H cos \delta}{R}$$R cos \varphi cos \delta$
HṛtiThe line in the diurnal circle corresponding to Antiyā in the plane of the celestial Equator or the length of the $\perp^{ar}$ from the culminating point on Udayāstasūtra223$H cos \delta + \dfrac{H sin \delta H sin \varphi}{H cos \varphi}$$R(cos \delta + sin \varphi tan \varphi)$
SūtraOM (O = centre of the sphere, M = foot of $\perp^{ar}$ on OQ from the foot of declination circle2653–54$H cos h$$R cos h$
KālaCorresponding line in diurnal circle27$\dfrac{H cos h H cos \delta}{R}$$R cos h cos \delta$
IṣṭāntyaLine corresponding to Iṣṭahṛti, on the Equatorial plane28$\dfrac{R^2 H cos z}{H cos \varphi H cos \delta}$$\dfrac{R cos z}{Cos \varphi cos \delta}$

298 | Cara Cāpa | Arc of the celestial Equator bet. the East point and foot of the declination circle | | | | | Carajyā | H sine of the above or the corresponding line of Kujya in the plane of the celestial Equator | 13 | 13-17 | (R · H sin φ · H sin δ) / (H cos φ · H cos δ) | R tan φ tan δ | | Natakāla | Hour angle h | | | | | | Unnata | Time elapsed after rise | | | | | | Śara | Corresponding line of phala in the Equatorial plane | 29 | 58 | H vers (h) | R (1 — cos h) | | Phala | ⊥ᵃʳ from the culminating point on a line through the celestial body parallel to Udayāstastūtra | 30 | | (H vers h · H cos δ) / R | R cos δ (1 — cos h) | | Ūrdhwa | Orthogonal projection of phala on the plane of the meridian | 31 | 59 | (H vers h · H cos φ · H cos δ) / R² | R cos φ cos δ (1-cosh) |

299 Yet (R sin δ) / (sin φ) will have a value greater than R ie. even though the Sama-S'anku is never born so to say, it has a magnitude. ‘तत्कथमिदं वन्ध्यासुतवत्’ Bhāskara exclaims with respect to the magnitudes of Sama-S'anku and Taddhṛti as well, both of which are not there, yet, both of which have magnitudes greater than R. So he says “those magnitudes of the Sama-S'anku and Taddhṛti are like the sons of a barren lady”. Then he says ‘तदपि प्रदर्श्यते’ ie. ‘We shall show how they arise.’ Here he uses his intuition of the principle of geo- metrical continuity. Even when the diurnal circle does not cut the prime-vertical, their planes intersect, out- side the sphere and the perpendicular dropped from the point of intersection on the plane of the horizon is the Sama S'anku which has a magnitude greater than R. Similarly the Taddhṛti could be seen what it is now. These magnitudes can enter into a proportion like the I in verse 22, and do help us to get the other real magnitudes like the Unmandala S'anku etc. Verses 66, 67 and first half of 68. To obtain the time from the shadow. Iṣṭāntyakā = (U.K. × Carajyā) / I.K. = (D.K. × Antyā) / I.K. = (k × R²) / (R cos δ × I.K.) ; Rvers⁻¹ (Antyā − I. A.) = h Dinārdha − h = Unnatakāla where K = Karṇa, k = Vishuvat Karṇa, I.A. = Iṣṭāntya. Comm. We had under verse 62. Iṣṭa-Karṇa × Iṣṭa-Hṛti = D. K. × Hṛti = S. K. × Taddhṛti = U. K. × Kujyā multiplying throughout by R / (R cos δ)

300 Iṣṭa-Karṇa × I. A. = D. K. × Antyā = U. K. × Carajyā so that I.A. = (D.K. × Antyā) / I.K. – (U.K. × Carajyā) / I.K. I But U.K. = 12 R / U.S. (verse 40) ∴ U.K. × Carajyā = (12R × Carajyā) / U.S. = (12R × Kujyā × R) / (U.S. × H cos δ) since Carajyā = (Kujyā × R) / (H cos δ) But Kujyā and U.S. are the Karṇa and Koṭi of the seventh latitudinal triangle so that Kujyā / U.S. = k / 12 Comparing with the first fundamental latitudinal triangle. ∴ U.K. × Carajyā = (12R² × k) / (H cos δ 12) = kR² / (H cos δ) Hence substituting in I I.A. = (U.K. × Carajyā) / I.K. = kR² / (H cos δ × I.K.) Thus we have proved the first part of the statement. Having obtained I.A., from fig. 52 we have Antyā – I.A. =(FQ–AN)=CQ. The Utkrama Cāpa of CQ = NQ = h and Dinārdha – h = Unnatakāla. Let us see what this procedure means in practice. Since on any day at any place, φ and the declination of the Sun are known we can compute all the magnitudes given in the verse or more easily H cos δ so that from the formula Iṣṭāntyā = 12R² / (H cos δ × I.K.) where K = √(S² + 12), the shadow being observed Iṣṭāntya could be computed in no time. Also the Antyā of the day R+(H tan φ tan δ) can be computed so that the segment CQ can be got. The inverse Hversine of this is h. The arc CQ above was symbolized as Sara.

301 Bhāskara’s proof of I.A. = kR² / (H cos δ × I.K.) proceeds from first principles as follows :—(i) If by k we have 12 as the Koṭi what have we for R? The result is H cos z, Mahāśaṅku. ∴ Mahā Śaṅku = 12 R / I.K. From Mahā Śaṅku we pass on to Iṣṭa Hṛti with which it forms a latitudinal triangle. If by the gnomon of 12 units we have k the Viṣuvat Karṇa, what have we by Mahā Śaṅku? The result is (12 R / I.K.) × (k / 12) = kR / I.K. Again from the Iṣṭa-Hṛti we pass on to I.A. by multiplying by R / (H cos δ) so that I.A. = kR² / (H cos δ × I.K.) as given. Second half of verse 68. The inverse Hversine if a quantity x greater than R, is 5400 + H sin ⁻¹ (θ) when x - R = θ. Comm. Since Hvers (90 + θ) = R + H sin θ = x (say) 90 + θ = Hvers ⁻¹ (R + H sin θ) = But 90° are equal to 5400 asus and θ = H sin ⁻¹ (H sin θ) = H sin ⁻¹ (x - R) = त्रिज्याधिकभागस्यक्रमचापम् ∴ 5400 + त्रिज्याधिकभागक्रमचापम् = Utkrama Cāpa of a त्रिज्यादिक quantity. Verse 69. Alternate method of obtaining the time that has elapsed after Sunrise noting the shadow S. Subtract Charajyā from or add it to Iṣṭāntyā according as δ is north or south. Obtain inverse H sine of the remainder and add the Caracāpa to this inverse H sine. Then we have the unnatakāla by converting the result into time.

302 Comm. Ref. fig. 52. I.A. = AN. I.A. - Carajyā = B.N. Hvers⁻¹ (BN) = arc EN. Arc EN + Caracāpa = EN + EM = MN. This converted into time is evidently the Unnatakāla because the arc MN of the equator is the arc intercepted between the feet of the declination circles at rising and at the time concerned M being the foot of the rising declination circle and N the foot of that at the time in question. The convention of signs is clear. Verse 70 and first half of 71. To obtain the Sun's longitude from the shadow S. The gnomonic shadow at noon, being multiplied by R and divided by K, the inverse H sine of the result gives the meridian zenith-distance. This being decreased or increased by the latitude gives the Sun's declination according as the extremity of the shadow is north or south. From the declination, we have the Sun's longitude by the formula H sin δ = (H sin λ H sin ω) / R . Comm. We have from the triangle formed by the gnomon and the shadow S, S / K = sin z or SR / K = H sin z ∴ H sin⁻¹ (SR / K) = z. Since we are directed to take the mid-day shadow, we have the meridian zenith-distance and from the formula z + δ = φ we have δ. If the extremity of the shadow be north, the Sun is south of the zenith, and then φ ~ z = δ. The word वियुक्ताः is used to signify difference which is positive. If z > φ then the declination is south and vice-versa. If the extremity of the shadow is on the south, the Sun is on the north of the zenith. in which case φ + z = δ. Second half of verse 71. To obtain φ from δ.

308 If the zenith-distance and the declination are of the same direction, their difference, otherwise their sum will be the latitude. [Fig. 58] Comm. Suppose the zenith- distance is north and decli- nation also north, then clearly from fig. 58, in this position S₁ of the Sun QS₁ — ZS₁ = ϕ = δ — Z (1) Again in the position S₃ of the Sun, zenith-distance is south and declination is also south ; so, here also difference gives ϕ ie. ZS₃ — QS₃ = Z — δ = ϕ. (3) In the position S₂, how- ever, Z is south and δ is north, so that their sum is equal to ϕ. It will be noted that the Hindu convention of signs does not contemplate negative declination and also it uses the word 'difference' to signify the positive difference, as for example, in the first two cases δ ~ Z is taken as ϕ. The modern formula Z + δ = ϕ applies universally with the convention that δ is +ve if north, ϕ is +ve if south. Verses 72, 73. To obtain the Bhuja from the shadow. Karṇa Vrittāgrā = (A × K) / R where A = Agrā and K the Chāyākarṇa. This Karnāgrā is to be taken as belonging to the opposite hemisphere to the Sun. Calling this Karnāgra as a and the equinoctial shadow as s, a ⨦ s according as δ is south or north gives the Chāyābhuja b. Thus a ⨦ s = b. If the extremity of the shadow be on the north and δ be north, then b + a = s ; if δ be south b ~ a = s. If b be north, b ~ s = A, otherwise ie. if south b + s = a. (R × a) / K = Agrā and (Agrā × Koṭi of latitudinal triangle) / (Karṇa of the latitudinal triangle) = H sin δ.

304 Comm. These verses are very important and the contents have been already elucidated under verses 13–17. We shall elucidate the convention of signs in more detail both from the modern point as well as from the Hindu traditional point. First we shall discuss the modern. We have the formula A = S + B where A = Agrā, S = Sankutala and B, Sanku-bhuja. Let us confine ourselves to north latitudes alone, for, south latitudes did not concern the Hindu astronomers. Then treating north declination as positive and also north Hindu azimuth as positive the above formula holds universally. (Ref. fig. 59) Let the figure represent the meridian plane. Let S₁, S₂, S₃ be the projections of the Sun's positions in their diurnal circles on to the meridian plane. Let A, B. be the Fig, 59

305 projections of the rising points of the Sun on the same plane. Let perpendiculars be dropped from S₁, S₂, S₃ on the plane of the horizon. Let o be the centre of the sphere. Let ns be the north-south line. In position S₁, S₁C = Śanku-Bhujā, KA = Śankutala, oA = Agrā, so that A = S + B (1) In the position S₂. S₂D = Śanku-Bhuja, LA = Śanku-tala, oA = Agrā, so that B + A = S; but here B is negative, a the azimuth being south so that writ- ing - B for B, - B + A = S ∴ A = S + B again. In position S₃, OB = A, MB = S, OM = B so that A + S = B; but here A is +ve, δ being south and B is negative a being south; hence writing - A and - B for A and B A + S = - B or A = S + B again. This shows that with the convention cited above A = S + B holds good universally. Now let us consider the situation with respect to the Karnāgrā. Each of the three quantities a, b, s have now opposite directions. If δ be north, the Sun will be on the north of Equator, but the extremity of the shadow will now be on the south of the Equinoctial shadow line (E.S.L.) ie. the line which is parallel to the East-west line at a distance of the equinoctial shadow s, and which is tbe locus of the extremity of the shadow on the equinoctial day; thus when the Agrā is considered to be positive being on the north of the East point, the Karnāgrā, though it is on fhe south will have to be considered positive. Similarly when the azimuth of the Sun a is on the north of the prime-vertical and is so considered to be positive, the extremity of the shadow being on the south of the East-west line and has a negative azimuth, the bhuja is still to be considered positive. Again the Śankutala being always south of the Udayāsta Sūtra being considered south and positive, the corresponding quantity into which it gets converted on the horizontal dial namely the equinoctial shadow s will be north of the East-west line and will be considered 39

306 positive. In other words in the equation a = b + s, a is positive when δ is north, b is +ve when the azimuth of the Sun is north of the East point, and s is always positive. Since in north latitudes, Śaṅkutala will be always south of the Udayāstasūtra and considered positive, the E.S.L. will be on the north of the East-west line so that s is considered positive. We should have had to consider s negative in southern latitudes, as per the above convention but as the Hindu astronomers did not have to concern themselves with south latitudes, the question of sign for s did not arise except taking it as always posi- tive. Hence the equation a = b + s will hold universally with the same conventions of sign which we stipulated with respect to the equation A = B + S. The foregoing analysis is on the modern lines. [चित्र: वृत्त के अंतर्गत W-E व्यास, E·S·L समानांतर रेखा, तथा बिन्दु O, C, P, R, M, L, A, N, B, K युक्त ज्यामितीय आरेख] Fig. 60

307 Now let us see how the convention of signs is stipulated in Hindu astronomy with respect to the equation a = b + s. We have said that ‘s’ is always north of the East-west line and considered positive. Regarding ‘a’, it is said by Bhāskara व्यस्तगोला which means that when δ is north and the Sun is said to be in northern hemisphere, a is said to belong to the southern hemisphere. Also when the Sun is on the north of the prime-vertical and Śankubhuja is considered north, the Chāyābhuja being south of the East-west line is considered south. With these conventions of directions (we say of directions, and not signs because the Hindu astronomers do not speak of signs but only of directions) it is stipulated in Hindu astronomy that quantities of like directions are to be added, otherwise their difference is to be taken ‘तुल्यदिशोर्योगः, भिन्नदिशोः अन्तरम्’. This convention stipul- ating addition or difference is technically called ‘संस्कार, Samskāra’. That is why it is said simply “पलच्छायया सौम्यया संस्कृता” ie. ‘Samskāra (on the aforesaid lines) is to be effected between a and s to get bhuja b’. Here it may be reiterated that the word ‘अन्तरम्’ ie. ‘difference’ is used in its restricted sense namely that the positive difference alone is to be taken. Thus the ‘antaram’ of 8 and 5 is 3 as well as that of 5 and 8 is also 3. Then it might be asked how to decide the direction of the bhuja, if we were to take s as equal to a ~ b and not a-b or b-a. The answer is that between a and s whose directions are known as per the aforesaid convention, equating their difference ie. a ~ s to b, we have to take b as having that direction which is indicated by that quantity either a or s which has a larger numerical value. Thus while on modern lines we take a = b + s to hold universally with the convention of signs which we have agreed to on modern lines namely that a is +ve if δ is north and b is positive if the Hindu azimuth is north of the East point and s is always +ve, we take on the Hindu lines a ± s = b with the conventions stipulated with respect

308 to directions (not of signs) namely that a is south if δ is north, s is always north and b is to be taken to belong to that direction to which the numerically bigger quantity of a and s belongs in the case of difference. Also it is to be taken to belong to that direction of a and s when both of them have the same direction. With this convention in mind, Bhāskara clarifies the convention by citing examples. (1) S=5, δ is north, Agrā=916'-48'' K=30 so that a = KA / R = (916⅘ × 30) / 3438 = 8 units (south, because it should be taken to be व्यस्तगोला ie. belonging to the direction opposite to that of δ). Question. "What is b and of what direction?" Answer. b = a +~ s = 8 (south) ~ 5 (north). (We are taking the difference because Samskāra is to be construed as addition of quantities having the same direction and difference of quantities of opposite direction ∴ b = 3 and is on the south because the numerically bigger quantity of 8 and 5 belongs to south. Q. 2. δ is north S=5, A=916'-48'' ; K=15, 'what is b and in what direction?' Answer. a = KA / R = 4; b = a +~ s = 4 +~ 5 = 4~5 (here a is south δ being north and s is north so that difference is stipulated as above) = 1 (north because 5 belongs to north. We add here two more examples to illustrate addition by saying that δ is south in the above examples so that a is north in both the examples. Hence in (1) b=8+5=13 (north) and in (2) b=4+5=9 (north). Refering to Fig. 60, we see there three cases depicted namely the extremi-

309 ties of the shadows being A, B and C. In the first case AL = Karnāgra = a (Karnāgra is the distance of the extremity of the shadow from the E.S.L. namely K.L.R. whereas bhuja is the distance of the same from the East- west line namely PMN) AM = bhuja and ML = s so that b=a+s addition being justified since both a and s are of the same direction namely north. In the second case BK = Karnāgra, BN = bhuja and NK = s so that b=s-a, the difference being justified because a is south and s north. Here we have taken the difference as s-a and not a-s because s is numerically greater and being oriented north, the bhuja is north. In the third case, PR=s, CP=b and CR=a so that b=a-s, the difference being justified be- cause s is north and a south. Also we have taken the difference as a-s and not s-a because a is numerically greater and as such lends its direction namely 'south' to the bhuja. Thus in the three examples cited, addition is prescribed between a and s only when the extremity of the shadow is to the north of E.S.L. In the case of A=S+B or B=A-S also, addition is prescribed only when δ is south, which means that the corresponding a ie. AL is north. In fact the prescription of addition or differ- ence accord in the cases of both the equations either A=B+S or a=b+s. Verses 74 and 75. Hereafter questions are being set and answered on diurnal problems. Seeing the shadow of the gnomon, the azimuth and longitude of the Sun or seeing two shadows with their respective directions, whoever knows the equinoctial shadow of the place, I consider him as the Garuda or Eagle who could overcome the false pride of puffed up snakes of astronomers. Given that when K=30 units, the bhuja is 3 units south, and when K=15, the bhuja is 1 unit north, com- pute the latitude, or again given H sin δ = 846 and given K and b of a shadow, compute the equinoctial shadows.

310 Comm. The questions are clear the second verse illustrating the first. Verse 76. Answer of the first question. (b₁ K₂ ⁺~ b₂ K₁) / (K₂ ~ K₁) = s according as the bhujas are of the same or opposite directions. Comm. Suppose b₁ and b₂ are of the same direction so that b₁ = a₁ - s and b₂ = a₂ - s, taking the modern convention of signs. But a₁ = (K₁A) / R and a₂ = (K₂A) / R ∴ b₁ = (K₁A) / R - s and b₂ = (K₂A) / R - s ∴ (b₁ + s) / K₁ = A / R = (b₂ + s) / K₂ ∴ K₂ b₁ - K₁ b₂ = s (K₁ - K₂) ∴ s = (K₂ b₁ - K₂ b₂) / (K₁ - K₂) If, however b₁ and b₂ are of opposite directions ie. of opposite signs, writing - b₂ for b₂, we have s = (K₂ b₁ + K₁ b₂) / (K₁ - K₂) . Here we have chosen to follow the modern convention of signs; otherwise we have to con- sider four alternatives, for, bhujas of the same direction might mean both of the type OC (fig. 60) or both of the type of OB or one of the tyye OB and one of the type of OA or both of the type OA. Verses 77 and 78. Answer to the second question. Let Laghu ≡ L = ((KH sin δ) / R)² ; 12² (L - b²) ≡ Ādya ; Para = 12² b. Let Ādya and Para be divided by L ~ 12² ; call them still Ādya and Para; then √(Para² + A) ± Para = s according as b is north or south.