IRJET- A Study on the Homogeneous Cone x2 + 7y2 = 23z2

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International Research Journal of Engineering and Technology (IRJET)

e-ISSN: 2395-0056

Volume: 06 Issue: 03 | Mar 2019

p-ISSN: 2395-0072

www.irjet.net

A Study on the Homogeneous Cone x 2  7 y 2  23 z 2 S. Vidhyalakshmi1, T. Mahalakshmi2 1Professor,

Department of Mathematics, Shrimati Indira Gandhi College, Trichy-620002, TamilNadu, India Professor, Department of Mathematics, Shrimati Indira Gandhi College, Trichy-620002, TamilNadu, India ---------------------------------------------------------------------***---------------------------------------------------------------------2Assistant

Abstract - The cone represented by the ternary quadratic Diophantine equation x 2  7 y 2  23z 2 is analyzed for its patterns of non-zero distinct integral solutions. A few interesting properties between the solutions and special polygonal numbers are exhibited.

Key Words: Ternary quadratic, cone, integral solutions. 2010 Mathematics Subject Classification: 11D09 1. INTRODUCTION

The Diophantine equation offers an unlimited field for research due to their variety [1-3]. In particular, one may refer [4-14] for quadratic equations with three unknowns. This communication concerns with yet another interesting equation x 2  7 y 2  23 z 2 representing non-homogeneous quadratic with three unknowns for determining its infinitely many non-zero integral points. Also, a few interesting relations among the solutions are presented. 2. METHOD OF ANALYSIS

The Ternary Quadratic Diophantine equation representing homogeneous cone under consideration is

x 2  7 y 2  23 z 2

(1)

We present below different methods of solving (1). Method I: Equation (1) is written in the form of ratio as x  4 z 7( z  y )    z y x  4z 

,  0

(2)

which is equivalent to the system of double equations

 x   y  (4   ) z  0   x  7 y  (7  4 ) z  0 Applying the method of cross multiplication, the corresponding values of x, y, z satisfying (1) are given by

x( ,  )  4 2  28 2  14 y( ,  )   2  7 2  8 z( ,  )   2  7 2 © 2019, IRJET

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