A history of Greek mathematics Vol.II from Aristarchus to Diophantus by Heath, Thomas Little, Sir, 1921
MACEDONIA is GREECE and will always be GREECE- (if they are desperate to steal a name, Monkeydonkeys suits them just fine) ΚΑΤΩ Η ΣΥΓΚΥΒΕΡΝΗΣΗ ΤΩΝ ΠΡΟΔΟΤΩΝ!!! ΦΕΚ,ΚΚΕ,ΚΝΕ,ΚΟΜΜΟΥΝΙΣΜΟΣ,ΣΥΡΙΖΑ,ΠΑΣΟΚ,ΝΕΑ ΔΗΜΟΚΡΑΤΙΑ,ΕΓΚΛΗΜΑΤΑ,ΔΑΠ-ΝΔΦΚ, MACEDONIA,ΣΥΜΜΟΡΙΤΟΠΟΛΕΜΟΣ,ΠΡΟΣΦΟΡΕΣ,ΥΠΟΥΡΓΕΙΟ,ΕΝΟΠΛΕΣ ΔΥΝΑΜΕΙΣ,ΣΤΡΑΤΟΣ, ΑΕΡΟΠΟΡΙΑ,ΑΣΤΥΝΟΜΙΑ,ΔΗΜΑΡΧΕΙΟ,ΝΟΜΑΡΧΙΑ,ΠΑΝΕΠΙΣΤΗΜΙΟ,ΛΟΓΟΤΕΧΝΙΑ,ΔΗΜΟΣ,LIFO,ΛΑΡΙΣΑ, ΠΕΡΙΦΕΡΕΙΑ,ΕΚΚΛΗΣΙΑ,ΟΝΝΕΔ,ΜΟΝΗ,ΠΑΤΡΙΑΡΧΕΙΟ,ΜΕΣΗ ΕΚΠΑΙΔΕΥΣΗ,ΙΑΤΡΙΚΗ,ΟΛΜΕ,ΑΕΚ,ΠΑΟΚ,ΦΙΛΟΛΟΓΙΚΑ,ΝΟΜΟΘΕΣΙΑ,ΔΙΚΗΓΟΡΙΚΟΣ,ΕΠΙΠΛΟ, ΣΥΜΒΟΛΑΙΟΓΡΑΦΙΚΟΣ,ΕΛΛΗΝΙΚΑ,ΜΑΘΗΜΑΤΙΚΑ,ΝΕΟΛΑΙΑ,ΟΙΚΟΝΟΜΙΚΑ,ΙΣΤΟΡΙΑ,ΙΣΤΟΡΙΚΑ,ΑΥΓΗ,ΤΑ ΝΕΑ,ΕΘΝΟΣ,ΣΟΣΙΑΛΙΣΜΟΣ,LEFT,ΕΦΗΜΕΡΙΔΑ,ΚΟΚΚΙΝΟ,ATHENS VOICE,ΧΡΗΜΑ,ΟΙΚΟΝΟΜΙΑ,ΕΝΕΡΓΕΙΑ, ΡΑΤΣΙΣΜΟΣ,ΠΡΟΣΦΥΓΕΣ,GREECE,ΚΟΣΜΟΣ,ΜΑΓΕΙΡΙΚΗ,ΣΥΝΤΑΓΕΣ,ΕΛΛΗΝΙΣΜΟΣ,ΕΛΛΑΔΑ, ΕΜΦΥΛΙΟΣ,ΤΗΛΕΟΡΑΣΗ,ΕΓΚΥΚΛΙΟΣ,ΡΑΔΙΟΦΩΝΟ,ΓΥΜΝΑΣΤΙΚΗ,ΑΓΡΟΤΙΚΗ,ΟΛΥΜΠΙΑΚΟΣ, ΜΥΤΙΛΗΝΗ,ΧΙΟΣ,ΣΑΜΟΣ,ΠΑΤΡΙΔΑ,ΒΙΒΛΙΟ,ΕΡΕΥΝΑ,ΠΟΛΙΤΙΚΗ,ΚΥΝΗΓΕΤΙΚΑ,ΚΥΝΗΓΙ,ΘΡΙΛΕΡ, ΠΕΡΙΟΔΙΚΟ,ΤΕΥΧΟΣ,ΜΥΘΙΣΤΟΡΗΜΑ,ΑΔΩΝΙΣ ΓΕΩΡΓΙΑΔΗΣ,GEORGIADIS,ΦΑΝΤΑΣΤΙΚΕΣ ΙΣΤΟΡΙΕΣ, ΑΣΤΥΝΟΜΙΚΑ,ΦΙΛΟΣΟΦΙΚΗ,ΦΙΛΟΣΟΦΙΚΑ,ΙΚΕΑ,ΜΑΚΕΔΟΝΙΑ,ΑΤΤΙΚΗ,ΘΡΑΚΗ,ΘΕΣΣΑΛΟΝΙΚΗ,ΠΑΤΡΑ, ΙΟΝΙΟ,ΚΕΡΚΥΡΑ,ΚΩΣ,ΡΟΔΟΣ,ΚΑΒΑΛΑ,ΜΟΔΑ,ΔΡΑΜΑ,ΣΕΡΡΕΣ,ΕΥΡΥΤΑΝΙΑ,ΠΑΡΓΑ,ΚΕΦΑΛΟΝΙΑ, ΙΩΑΝΝΙΝΑ,ΛΕΥΚΑΔΑ,ΣΠΑΡΤΗ,ΠΑΞΟΙ
MACEDONIA is GREECE and will always be GREECE- (if they are desperate to steal a name, Monkeydonkeys suits them just fine)
ΚΑΤΩ Η ΣΥΓΚΥΒΕΡΝΗΣΗ ΤΩΝ ΠΡΟΔΟΤΩΝ!!!
ΦΕΚ,ΚΚΕ,ΚΝΕ,ΚΟΜΜΟΥΝΙΣΜΟΣ,ΣΥΡΙΖΑ,ΠΑΣΟΚ,ΝΕΑ ΔΗΜΟΚΡΑΤΙΑ,ΕΓΚΛΗΜΑΤΑ,ΔΑΠ-ΝΔΦΚ, MACEDONIA,ΣΥΜΜΟΡΙΤΟΠΟΛΕΜΟΣ,ΠΡΟΣΦΟΡΕΣ,ΥΠΟΥΡΓΕΙΟ,ΕΝΟΠΛΕΣ ΔΥΝΑΜΕΙΣ,ΣΤΡΑΤΟΣ, ΑΕΡΟΠΟΡΙΑ,ΑΣΤΥΝΟΜΙΑ,ΔΗΜΑΡΧΕΙΟ,ΝΟΜΑΡΧΙΑ,ΠΑΝΕΠΙΣΤΗΜΙΟ,ΛΟΓΟΤΕΧΝΙΑ,ΔΗΜΟΣ,LIFO,ΛΑΡΙΣΑ, ΠΕΡΙΦΕΡΕΙΑ,ΕΚΚΛΗΣΙΑ,ΟΝΝΕΔ,ΜΟΝΗ,ΠΑΤΡΙΑΡΧΕΙΟ,ΜΕΣΗ ΕΚΠΑΙΔΕΥΣΗ,ΙΑΤΡΙΚΗ,ΟΛΜΕ,ΑΕΚ,ΠΑΟΚ,ΦΙΛΟΛΟΓΙΚΑ,ΝΟΜΟΘΕΣΙΑ,ΔΙΚΗΓΟΡΙΚΟΣ,ΕΠΙΠΛΟ, ΣΥΜΒΟΛΑΙΟΓΡΑΦΙΚΟΣ,ΕΛΛΗΝΙΚΑ,ΜΑΘΗΜΑΤΙΚΑ,ΝΕΟΛΑΙΑ,ΟΙΚΟΝΟΜΙΚΑ,ΙΣΤΟΡΙΑ,ΙΣΤΟΡΙΚΑ,ΑΥΓΗ,ΤΑ ΝΕΑ,ΕΘΝΟΣ,ΣΟΣΙΑΛΙΣΜΟΣ,LEFT,ΕΦΗΜΕΡΙΔΑ,ΚΟΚΚΙΝΟ,ATHENS VOICE,ΧΡΗΜΑ,ΟΙΚΟΝΟΜΙΑ,ΕΝΕΡΓΕΙΑ, ΡΑΤΣΙΣΜΟΣ,ΠΡΟΣΦΥΓΕΣ,GREECE,ΚΟΣΜΟΣ,ΜΑΓΕΙΡΙΚΗ,ΣΥΝΤΑΓΕΣ,ΕΛΛΗΝΙΣΜΟΣ,ΕΛΛΑΔΑ, ΕΜΦΥΛΙΟΣ,ΤΗΛΕΟΡΑΣΗ,ΕΓΚΥΚΛΙΟΣ,ΡΑΔΙΟΦΩΝΟ,ΓΥΜΝΑΣΤΙΚΗ,ΑΓΡΟΤΙΚΗ,ΟΛΥΜΠΙΑΚΟΣ, ΜΥΤΙΛΗΝΗ,ΧΙΟΣ,ΣΑΜΟΣ,ΠΑΤΡΙΔΑ,ΒΙΒΛΙΟ,ΕΡΕΥΝΑ,ΠΟΛΙΤΙΚΗ,ΚΥΝΗΓΕΤΙΚΑ,ΚΥΝΗΓΙ,ΘΡΙΛΕΡ, ΠΕΡΙΟΔΙΚΟ,ΤΕΥΧΟΣ,ΜΥΘΙΣΤΟΡΗΜΑ,ΑΔΩΝΙΣ ΓΕΩΡΓΙΑΔΗΣ,GEORGIADIS,ΦΑΝΤΑΣΤΙΚΕΣ ΙΣΤΟΡΙΕΣ, ΑΣΤΥΝΟΜΙΚΑ,ΦΙΛΟΣΟΦΙΚΗ,ΦΙΛΟΣΟΦΙΚΑ,ΙΚΕΑ,ΜΑΚΕΔΟΝΙΑ,ΑΤΤΙΚΗ,ΘΡΑΚΗ,ΘΕΣΣΑΛΟΝΙΚΗ,ΠΑΤΡΑ, ΙΟΝΙΟ,ΚΕΡΚΥΡΑ,ΚΩΣ,ΡΟΔΟΣ,ΚΑΒΑΛΑ,ΜΟΔΑ,ΔΡΑΜΑ,ΣΕΡΡΕΣ,ΕΥΡΥΤΑΝΙΑ,ΠΑΡΓΑ,ΚΕΦΑΛΟΝΙΑ, ΙΩΑΝΝΙΝΑ,ΛΕΥΚΑΔΑ,ΣΠΑΡΤΗ,ΠΑΞΟΙ
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j<br />
EUTOCIUS. ANTHEMIUS 541<br />
missing solution, promised <strong>by</strong> Archimedes in On the Sphere<br />
and Cylinder, <strong>II</strong>. 4, <strong>of</strong> the auxiliary problem amounting<br />
<strong>to</strong> the solution <strong>by</strong> means <strong>of</strong> conies <strong>of</strong> the cubic equation<br />
(a — x)x 2 = be 2 , (3) the solutions (a) <strong>by</strong> Diocles <strong>of</strong> the original<br />
problem <strong>of</strong> <strong>II</strong>. 4 without bringing in the cubic, (b) <strong>by</strong> Dionysodorus<br />
<strong>of</strong> the auxiliary cubic equation.<br />
Anthemius <strong>of</strong> Tralles, the architect, mentioned above, was<br />
himself an able mathematician, as is<br />
a work <strong>of</strong> his, On Burning-mirrors.<br />
seen <strong>from</strong> a fragment <strong>of</strong><br />
This is a document <strong>of</strong><br />
considerable importance for the <strong>his<strong>to</strong>ry</strong> <strong>of</strong> conic sections.<br />
Originally edited <strong>by</strong> L. Dupuy in 1777, it was reprinted in<br />
Westermann's <strong>II</strong>apaSo£oy pd(f>oi (Scrip<strong>to</strong>res rerum mirabiliwm<br />
Graeci), 1839, pp. 14 9-58. The first and third portions <strong>of</strong><br />
the fragment are those which interest us. 1 The first gives<br />
a solution <strong>of</strong> the problem, To contrive that a ray <strong>of</strong> the sun<br />
(admitted through a small hole or window) shall fall in a<br />
given spot, without moving away at any hour and season.<br />
This is contrived <strong>by</strong> constructing an elliptical mirror one focus<br />
<strong>of</strong> which is at the point where the ray <strong>of</strong> the sun is<br />
admitted<br />
while the other is at the point <strong>to</strong> which the ray is required<br />
<strong>to</strong> be reflected at all times. Let B be the hole, A the point<br />
<strong>to</strong> which reflection must always take place, BA being in the<br />
meridian and parallel <strong>to</strong> the horizon. Let BO be at right<br />
angles <strong>to</strong> BA, so that OB is an equinoctial ray ; and let BD be<br />
the ray at the summer solstice, BE a winter ray.<br />
Take F at a convenient distance on BE and measure FQ<br />
equal <strong>to</strong> FA. Draw HFG through F bisecting the angle<br />
AFQ, and let BG be the straight line bisecting the angle EBO<br />
between the winter and the equinoctial rays. Then clearly<br />
since FG bisects the angle QFA, if we have a plane mirror in<br />
the position HFG, the ray BFE entering at B will be reflected<br />
<strong>to</strong> J..<br />
To get the equinoctial ray similarly reflected <strong>to</strong> A, join GA,<br />
and with G as centre and GA as radius draw a circle meeting<br />
BO in K. Bisect the angle KGA <strong>by</strong> the straight line GLM<br />
meeting BK in L and terminated at 31, a point on the bisec<strong>to</strong>r<br />
<strong>of</strong> the angle CBD. Then LM bisects the angle KLA also, and<br />
KL = LA, and KM = MA.<br />
the ray BL will be reflected <strong>to</strong> A.<br />
1<br />
If then GLM is a plane mirror,<br />
See Bibliotheca mathematica, vii 3 , 1907, pp. 225-33.<br />
542 COMMENTATORS AND BYZANTINES<br />
By taking the point<br />
AT on BD such that MN = MA, and<br />
bisecting the angle NMA <strong>by</strong> the straight line MOP meeting<br />
BD in 0, we find that, if MOP is a plane mirror, the ray BO<br />
is reflected <strong>to</strong> A.<br />
Similarly, <strong>by</strong> continually bisecting angles and making more<br />
mirrors, we can get any number <strong>of</strong> other points <strong>of</strong> impact. Making<br />
the mirrors so short as <strong>to</strong> form a continuous curve, we get<br />
the curve containing all points such that the sum <strong>of</strong> the distances<br />
<strong>of</strong> each <strong>of</strong> them <strong>from</strong> A and B is constant and equal <strong>to</strong> BQ, BK,<br />
or BN. '<br />
If then ', says Anthemius, ' we stretch a string passed<br />
round the points A, B, and through the first point taken on the<br />
rays which are <strong>to</strong> be reflected, the said curve will be described,<br />
which is part <strong>of</strong> the so-called " ellipse ", with reference <strong>to</strong><br />
which (i.e. <strong>by</strong> the revolution <strong>of</strong> which round BA) the surface<br />
<strong>of</strong> impact <strong>of</strong> the saichmirror has <strong>to</strong> be constructed*'<br />
We have here apparently the first mention <strong>of</strong> the construction<br />
<strong>of</strong> an ellipse<br />
<strong>by</strong> means <strong>of</strong> a string stretched tight round<br />
the foci. Anthemius's construction depends upon two propositions<br />
proved <strong>by</strong> Apollonius (1) that the sum <strong>of</strong> the focal<br />
distances <strong>of</strong> any point on the ellipse is constant, (2) that the<br />
focal distances <strong>of</strong> any point make equal angles with the<br />
tangent at that point, and also (3) upon a proposition not<br />
found in Apollonius, namely that the straight line joining