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[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF)

INTERNATIONAL JOURNAL OF ENGINEERING SCIENCES

& MANAGEMENT

ON THE TERNARY QUADRATIC DIOPHANTINE EQUATION

2 2

2

4

2

)

3(x

y

xy

z

M.A.Gopalan1

*

, S.Vidhyalakshmi2, A.Kavitha3, D.Mary Madona4

2 , 1

Professor, Department of Mathematics, SIGC, Trichy-620002, Tamil Nadu, 3

Lecturer, Department of Mathematics, SIGC, Trichy-620002, Tamil Nadu 4

M.Phil. Scholar, Department of Mathematics, SIGC, Trichy-620002, Tamil Nadu mayilgopalan@gmail.com

ABSTRACT:

The ternary homogeneous quadratic equation given by

3(x

2

y

2

)

2

xy

4

z

2representing a cone is analyzed for its non-zero distinct integer solutions. A few interesting relations between the solutions and special polygonal and pyramidal numbers are presented. Also, given a solution, formula for generating a sequence of solutions based on the given solution is presented.

KEYWORDS: Ternary quadratic , integer solutions, figurate numbers, homogeneous quadratic, polygonal number, pyramidal number.

2010 Mathematics subject classification: 11D09.

NOTATIONS USED:

1. Polygonal number of rank ‘n’ with sides m

2

)

2

m

)(

1

n

(

1

n

t

m,n

2. Stella octangular number of rank ‘n’

)

1

n

2

(

n

SO

n

2

3. Pronic number of rank ‘n’

)

1

(

Pr

n

n

n

4. Octahedral number of rank ‘n’

)]

1

2

(

[

3

1

2

n

n

OH

n

I.

INTRODUCTION

The Diophantine equations offer an unlimited field for research due to their variety[1-3].In particular, one may refer [4-24] for quadratic equations with three unknowns. This communication concerns with yet another interesting

equation

3(x

2

y

2

)

2

xy

4

z

2representing homogeneous quadratic equation with three unknowns for determining its infinitely many non-zero integral points. Also, a few interesting relations among the solution is presented.

II.

METHOD OF ANALYSIS

Consider the equation

2 2

2

4

2

)

3(x

y

xy

z

(1)

The substitution of the linear transformations

x=u+v ; y=u-v (2)

in (1) gives

u

2

2

v

2

z

2 (3)

(2)

[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF)

METHOD:1

Write (3) in the form of ratio as

=

,

0

v

u

-z

2v

u

z

(4)

This is equivalent to the following two equation,

0

2

v

z

u

0

v

z

u

(5)

Applying the method of cross multiplication ,the above system of equations (5) is satisfied by

u

2

2

2

,

v

2

2

(6)

Substituting the values of u and v in (2),we get

x

x

(

,

)

2

2

2

2



y

y

(

,

)

2

2

2

2



(7)

Thus (6) and (7) represent non-zero distinct integral solutions of (1) in two parameters.

Properties:

A few interesting properties obtained as follows:

x(1,

a)

-

y(1,

a)

-

4t

4,a

-4Pr

a

-

4t

4,a

0

x(a,

2a)

-

y(a,

2a)

-

4

t

6,n

0

(mod

4)

x(a,

2a

-

1)

-

y(a,

2a

-

1)

4

so

a

0(mod

4)

2

2

x(a,1)

-

y(a,1)

-

z(a,1)

pr

a

-

2(mod

5)

x(a,

2a)

y(a,

2a)

-

4

t

10,n

-

t

6,n

0

(mod

11)

Remark:

In addition to (4), (3) may also be expressed in the form of ratios in three different ways that are presented below:

Way 1:

=

2v

u

z

u

z

v

Way 2:

=

v

u

-z

2

u

z

v

Way 3:

=

2v

v

-z

u

z

v

Solving each of the above system of equations by following the procedure presented in Method 1, the corresponding integer solutions to (1) are found to be as given below:

Solution for way 1:

x (

,

) =

2

2

2

2



y (

,

) =

2

2

2

2



z (

,

) =

2

2

2

2 2 2

2

)

,

(

z

(3)

[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF) Solution for way 2:

x (

,

) =

2

2

2

2



y (

,

) =

2

2

2

2



z (

,

) =

2

2

2 Solution for way 3:

x (

,

) =

2

2

2

2



y (

,

) =

2

2

2

2



z (

,

) =

2

2-

2

METHOD 2:

(3) is written as

1

*

2

2 2 2

2

z

z

v

u

(8)

Assume

z

z

(

a

,

b

)

a

2

2

b

2 (9) where a, b are non –zero integers, write 1 as

1 =

9

)

2

2

i

-)(1

2

i2

(1

(10)

Substituting (9) and(10) in (8) , it is written in the factorizable form as

(

(

2

)

2

(

2

)

2

3

)

2

2

1

(

3

)

2

2

1

(

)

2

)(

2

v

u

i

v

i

i

a

i

b

a

i

b

i

u

Equating the positive & negative factors,we get

(

(

2

)

2

3

)

2

2

1

(

)

2

v

i

a

i

b

i

u

(11)

(

(

2

)

2

3

)

2

2

1

(

)

2

v

i

a

i

b

i

u

(12)

On equating real and imaginary parts in either(11) or (12), we get

3

)

8

2

(

a

2

b

2

ab

u

3

)

2

4

2

(

a

2

b

2

ab

v

Substituting the values u and v in(2),we have

)

2

2

(

)

,

(

2 2

ab

b

a

b

a

x

x

(13)

3

)

10

2

(

)

,

(

2 2

ab

b

a

b

a

y

y

(14)

As our interest centers on finding integers solutions, it is seen that x and y are integers for suitable choices of a and b .Replacing a by 3a and by 3b, the corresponding non zero distinct integer solutions to (1) are given by

ab

b

a

b

a

x

x

(

,

)

9

2

18

2

18

ab

b

a

y

y

(

,

)

3

2

6

2

30

2 2

18

9

)

,

(

a

b

a

b

z

z

Properties:

A few interesting properties obtained as follows:

(4)

[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF)

2x(1,

a)

-

2z(1,

a)

-

12

t

8,n

24(mod36)

2y(a

1,

a

1)

-

z(a

1,

a

1)

56

t

8,n

-

216(mod

81)

y(1,

a)

-

z(1,

a)

3t

10,n

-

12(mod

39)

2y(1,

a)

2z(1,

a)

-

12t

10,n

-12

(mod

24)

METHOD:3

In addition to (9), write 1 as

1 =

121

)

2

i6

-)(7

2

6

i

(7

(15)

Substituting (9) and(15) in (8) , it is written in the factorizable form as

2 2

)

2

(

)

2

(

121

)

2

6

7

)(

2

6

7

(

)

2

)(

2

(

u

i

v

u

i

v

i

i

a

i

b

a

i

b

Equating the positive & negative factors ,we get

2

)

2

(

11

)

2

6

7

(

)

2

(

u

i

v

i

a

i

b

(16)

2

)

2

(

11

)

2

6

7

(

)

2

(

u

i

v

i

a

i

b

(17)

On equating real and imaginary parts in either(15) or (16) , we get

11

)

24

14

7

(

a

2

b

2

ab

u

11

14

12

6

a

2

b

2

ab

v

Substituting the values u and v in(2),we have

11

)

10

26

13

(

)

,

(

2 2

ab

b

a

b

a

x

x

(18)

11

)

38

2

(

)

,

(

2 2

ab

b

a

b

a

y

y

(19)

As our interest centers on finding integers solutions, it is seen that x and y are integers for suitable choices of a and b .Replacing a by 11a and by 11b, the corresponding non zero distinct integer solution to (1) are given by

ab

b

a

b

a

x

x

(

,

)

143

2

286

2

110

ab

b

a

y

y

(

,

)

11

2

22

2

418

2 2

242

121

)

,

(

a

b

a

b

z

z

Properties:

A few interesting properties obtained as follows:

x(a,1)

-

z(a,1)

-

11t

6,n

-

528(mod

99)

x(2a,

a)

z(2a,

a)

-

1056t

4,n

-

22t

6,n

-

55

t

10,n

0(mod187)

x(a,1)

-

y(a,1)

33

t

10,n

-

264(mod

407)

x(2a,

a)

y(2a,

a)

-

308t

6,n

1364t

4,n

0(mod

308)

(5)

[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF) METHOD:4

Write (3) as

1

*

2

2 2 2

2

u

u

v

z

(20)

Write 1 as

1=

(

3

2

2

)(

3

2

2

)

(21)

Assume u = u (a, b)=

a

2

2

b

2 (22) where a ,b are non –zero integers, Using (20) and (21) in (22) ,it is written in the factorizable form as

2 2

)

2

(

)

2

)(

2

2

3

)(

2

2

3

(

)

2

)(

2

(

z

v

z

v

a

b

a

b

Equating the positive & negative factors ,we get

2

)

2

)(

2

2

3

(

)

2

(

z

v

a

b

(23)

2

)

2

)(

2

2

3

(

)

2

(

z

v

a

b

(24) On equating rational and irrational parts in either(23) or (24), we get

ab

b

a

z

3

2

6

2

8

ab

b

a

v

2

2

4

2

6

(25) Substituting the values u and v in (2),we have

ab

b

a

b

a

x

x

(

,

)

3

2

2

2

6

ab

b

a

b

a

y

y

(

,

)

2

6

2

6

(26)

Note that (25) and (26) represent the non –zero distinct interger solutions to (1)

Properties:

A few interesting properties obtained as follows:

x(a,

a)

y(a,

a)

-

t

6,n

t

10,n

0(mod

2)

x(2a,

a)

y(2a,

a)

-

4t

10,n

-

4t

6,n

-

24

t

4,n

0(mod16)

x(a,

a

1)

-

z(a,

a

1)

2

t

8,n

-

4(mod

14)

x(a

1,

a)

y(a

1,

a)

t

6,n

-

2(mod

3)

z

(

2

a

,

a

)

y(2a,

a)

x(2a,

a)

-

5t

4,n

4

t

6,n

-

4t

10,n

0

(mod

16)

III.

Remarkable observations

If the non zero integer triple (

x

0,

y

0,

z

0

)

is any solution of(1) ,then a general formula for generating a sequence

of solutions based on the given solution is illustrated below :

Let (

x

0,

y

0,

z

0

)

be any given solution of (1) and let the second solution of (1) be,

1

x

=

x

0+

h

1

y

=

y

0

h

0

(27)

1

z

=

h

-

z

0

Substituting (27S) in (1) & performing a few calculations, we have

h

=

6

x

0

8

z

0and then

1

x

=

7

x

0

8

z

0

1

(6)

[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF)

This is written in the form of matrix as









0 0

1 1

y

x

y

x

M

(28)

where





7

6

8

7

M

From the second solution, we get the corresponding third solution (

x

2,

y

2,

z

2

)

as given below.

2

x

=

97

x

0

112

z

0

2

y

=

y

0

0 0

2

90

104

z

x

z

Repeating the above process, the general solution

x

n

,

y

n

to (1) is given by









0 0

n n

y

x

y

x

n

M

(29)

To find

M

n, the Eigen values of M are

7

4

3

,

7

4

3

. It is well-known that

)

-(

-)

-(

-

M

I

M

I

M

n n

n

Using the above formula, we have

n n

n n

n

A

B

B

A

M

3

4

6

8

3

4

3

8

1

Where

A

n

(

n

n

)

B

n

(

n

n

)

Hence we get the

n

thsolution to be

n 0 0

n

(

4

3

A

x

8

z

2

1

x

B

n

0 n

y

y

n 0 0

n

(

6

B

x

4

3

z

3

8

1

Z

A

n

IV.

Conclusion

In this paper, we have obtained infinitely many non-zero distinct integer solutions to the ternary quadratic Diophantine equation represented by

2 2

2

4

2

)

3(x

y

xy

z

As quadratic equations are rich in variety, one may search for their choices of quadratic equation with variables greater than or equal to 3 and determine their properties through special numbers.

V.

Acknowledgement:

(7)

[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF)

References

[1] Dickson. I.E” History of Theory of Numbers”, Volume 2. Diophantine analysis, New York, Dover, 2005. [2] Model .L.J.,” Diophantine Equations” Academic Press, New York, 1969.

[3] Carmichael.R.D”The Theory of numbers and Diophantine Analysis”, New York, Dover, 1959.

[4] M.A.Gopalan, Geetha D and Lattice points on the Hyberboloid of two sheets

4

5

2

6

6

2 2

2

z

y

x

y

xy

x

, Impact J Sci Tech 2010;4:23-32

[5] M.A.Gopalan and Vidhyalakshmi S, Kavitha A . Integral points on the Homogeneous cone

z

2

2

x

2

7

y

2

,The Diophantus J M ath 2012;1(2):127-136.

[6] M.A.Gopalan, Vidhyalakshmi S, Sumati G ,Lattice points on the Hyberboloid one sheet

4

3

2

2 2

2

y

x

z

.Diophantus J Math 2012;1(2):109-115

[7] M.A.Gopalan and Vidhyalakshmi S ,lakshmi k. Intergral points on the Hyberboloid of two sheets

21

7

3

y

2

x

2

z

2

Diophantus J Math 2012;1(2):99-107.

[8] Gopalan MA, Vidhyalakshmi S, Mallika S. Observation on Hyperboloid of one sheet

x

2

2

y

2

z

2

2

Bessel J of Math 2012; 2(3):221-226.

[9] Gopalan MA, Vidhyalakshmi S, Usha Rani TR. Mallika S.

6

2

3

2

2

2

0

x

y

z

Integral points on the Homogeneous cone. Impact J Sci Tech 2012;6(1):7-13.

[10]. Gopalan MA, Vidhyalakshmi S, Sumathi G. Lattice points on the Elliptic parabol

9

x

2

4

y

2

z

Advances in Theoretical and Applied Mathematics2012; 7(4):379-385.

[11]. Gopalan MA, Vidhyalakshmi S, Usha Rani TR. Integralpoints on the non-homogeneous cone

0

4

8

4

2

z

2

xy

x

z

. Global Journal ofMathematics and Mathematical Sciences 2012;2(1):61-67.

[12]. Gopalan MA, Vidhyalakshmi S, Lakshmi K. Lattice points on the elliptic paraboloid

16

y

2

9

z

2

4

x

Bessel J of Math 2013; 3(2):137-145.

[13]. Gopalan MA, Vidhyalakshmi S, UmaRani J, Integralpoints on the homogeneous cone

x

2

4

y

2

37

z

2Cayley J of Math, 2013, 2(2):101-107.

[14]. Gopalan MA, Vidhyalakshmi S, Kavitha A.Observations on the Hyperboloid of two Sheets

4

)

(

3

7

x

2

y

2

z

2

z

y

x

. InternationalJournal of Latest Research in Science and technology 2013; 2(2):84-86.

[15]. Gopalan MA, Sivagami B. Integral points on the homogeneous cone

z

2

3

x

2

6

y

2IOSR Journal ofMathematics 2013; 8(4):24-29.

[16]. Gopalan MA, Geetha V. Lattice points on the Homogeneous cone

z

2

2

x

2

8

y

2

6

xy

. Indianjournal of Science 2013; 2:93-96.

[17]. Gopalan MA, Vidhyalakshmi S, Maheswari D. Integral points on the homogeneous

cone

2

x

2

3

y

2

35

z

2Indian Journal of Science 2014; 7:6-10.

[18]. Gopalan. MA, Vidhyalakshmi S, Umarani J. On theTernary Quadratic Diophantine

(8)

[Gopalan, 5(2): April-June, 2015] ISSN: 2277-5528 Impact Factor: 2.745 (SIJF)

[19]. Meena K, Vidhyalakshmi S, Gopalan MA, Priya IK. Integral points on the cone

3

(

x

2

y

2

)

5

xy

47

z

2Bulletin of Mathematics and Statistic Reseach 2014; 2(1):65-70.

[20]. Gopalan MA, Vidhyalakshmi S, Nivetha S. On Ternary Quadratics

equation

4

(

x

2

y

2

)

7

xy

31

z

2 Diophantus J Math 2014; 3(1):1-7.

[21]. Meena K, Vidhtalakshmi S, Gopalan MA, Thangam SA. Integer Solutions on the Homogeneous

cone

4

x

2

3

y

2

28

z

2 Bulletin of Mathematics and statistics Research 2014; 2(1):47-53.

[22]. Shanthi J, Gopalan MA, Vidhyalakshmi. Lattice pointson the Homogeneous cone

2 2

2

56

15

)

(

8

x

y

xy

z

Sch Journal of PhyMath Stat 2014; 1(1):29-32.

[23]. Gopalan MA, Vidhyalakshmi S, Mallika S. On ternary quadratic Diophantine equation

8

(

x

2

y

2

)

15

xy

80

z

2, BOMSR, 2014; 2(4):429-433.

[24] .Gopalan MA, Meena k, Vidhyalakshmi S, Thiruniraiselvi N. On Ternary Quadratics

References

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