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IOSR Journal of Applied Physics (IOSR-JAP)
e-ISSN: 2278-4861.Volume 4, Issue 2 (Jul. - Aug. 2013), PP 31-32
www.iosrjournals.org
www.iosrjournals.org 31 | Page
Proposal of New Operator in Four-Dimensional Wave Equation
Umasankar Dolai
Assistant Teacher, Dwarigeria Pry. School, Garhbeta south C.L.R.C., Satbankura-721253
Dist.-Paschim Medinipur, West Bengal, India
Abstract: Four-dimensional equation of a progressive wave is proposed to express wave-criterion in four-
dimensional world. Moreover in this equation a new mechanical operator is obtained.
Keywords- Three and Four-Dimensional Wave Criteria, Relativistic Mechanics, Progressive Gravitational
Wave.
I. Introduction
It is already known that three-dimensional equation of a progressive wave is d2
ψ/dx2
+ d2
ψ/dy2
+
d2
ψ/dz2
=1/u2
.d2
ψ/dt2
; where ψ is wave amplitude and u is the velocity of wave. But when a progressive wave
moves in four-dimensional nature, then it can obviously obey four-dimensional wave equation. Here four-
dimensional formulation of a progressive wave can be drawn to deduce the reality of this wave in four-
dimensional world.
II. Formation of Operator-Relation
In four-dimensional generalization, it is written that x1=x, x2=y, x3=z and x4=ict. In terms of
differentials, dx1=dx, dx2=dy, dx3=dz and dx4=icdt. From operator representation, d/dx1=d/dx, d/dx2=d/dy,
d/dx3=d/dz and d/dx4=1/ic.d/dt.Now taking square in both sides, d2
/dx1
2
=d2
/dx2
, d2
/dx2
2
=d2
/dy2
, d2
/dx3
2
=d2
/dz2
and d2
/dx4
2
=1/i2
c2
.d2
/dt2
. By addition, d2
/dx1
2
+ d2
/dx2
2
+ d2
/dx3
2
+ d2
/dx4
2
=d2
/dx2
+ d2
/dy2
+ d2
/dz2
-1/c2
.d2
/dt2
. This
is the desired operator-relation.
III. Foundation of Wave Equation
If the amplitude of a progressive wave is ψ; then multiplying in both sides of above operator-relation
by ψ, it is obtained that d2
ψ/dx1
2
+ d2
ψ/dx2
2
+ d2
ψ/dx3
2
+ d2
ψ/dx4
2
=d2
ψ/dx2
+ d2
ψ/dy2
+ d2
ψ/dz2
-1/c2
.d2
ψ/dt2
. This is
the required wave-relation.
From three-dimensional wave equation, it is written that d2
ψ/dx2
+ d2
ψ/dy2
+ d2
ψ/dz2
=1/u2
.d2
/dt2
or
d2
ψ/dx2
+ d2
ψ/dy2
+ d2
ψ/dz2
-1/u2
.d2
/dt2
=0. In case of light wave, the relation is d2
ψ/dx2
+ d2
ψ/dy2
+ d2
ψ/dz2
-
1/c2
.d2
/dt2
=0; where c is the velocity of light. Thus by putting the above value, the four-dimensional wave
equation is d2
ψ/dx1
2
+ d2
ψ/dx2
2
+ d2
ψ/dx3
2
+ d2
ψ/dx4
2
=0.
IV. Suggestion for New Operator
The above wave equation be considered as the following form: [d2
/dx1
2
+ d2
/dx2
2
+ d2
/dx3
2
+ d2
/dx4
2
]ψ=0.
Let it be assumed that d2
/dx1
2
+ d2
/dx2
2
+ d2
/dx3
2
+ d2
/dx4
2
=◊2
=a new mechanical operator in relativistic
mechanics. So ◊2
ψ=0. This is the modified form of four-dimensional wave equation of a progressive wave.
V. Conclusion
In course of discussion, it is discussed that the progressive wave which moves with a velocity equals to
the velocity of light can obey the above wave equation. In this respect, gravitational wave is mentioned here.
According to general relativity, gravitational energy is carried by gravitational waves. These waves move with
the velocity of light. Thus the wave equation of a progressive gravitational wave is ◊2
ψ=0. This relation can
express the reality of progressive gravitational waves.
Acknowledgements
I wish to thank Prof. Sriranjan Banerji and Prof. Asit Banerjee, Department of Physics, Jadavpur
University for their book ‘The Special Theory of Relativity’. I indebt to thank Shree Gouri Sankar Dolai, student
of Higher Secondary School for his help to type this paper. I also like to thank Mr. Koushik Dhara, Teacher of
Computer Science for his inspiration to write this type of article by me.
Submitted Date 19 June 2013 Accepted Date: 24 June 2013
Proposal of New Operator in Four-Dimensional Wave Equation
www.iosrjournals.org 32 | Page
REFERENCES
[1] R. Resnick, Introduction to special Relativity (Wiley Eastern, New Delhi, 1989).
[2] H. Goldstein, Classical Mechanics (Narosa, New Delhi, 1998).
[3] C. Moller, The Theory of Relativity (Oxford University Press, 1972).
[4] P. G. Bergmann, Introduction to the Theory of Relativity (Prentice-Hall, New Delhi, 1969).
[5] S. N. Ghoshal, Introductory Quantum Mechanics (Calcutta Book House, Reprint-2011).

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Proposal of New Operator in Four-Dimensional Wave Equation

  • 1. IOSR Journal of Applied Physics (IOSR-JAP) e-ISSN: 2278-4861.Volume 4, Issue 2 (Jul. - Aug. 2013), PP 31-32 www.iosrjournals.org www.iosrjournals.org 31 | Page Proposal of New Operator in Four-Dimensional Wave Equation Umasankar Dolai Assistant Teacher, Dwarigeria Pry. School, Garhbeta south C.L.R.C., Satbankura-721253 Dist.-Paschim Medinipur, West Bengal, India Abstract: Four-dimensional equation of a progressive wave is proposed to express wave-criterion in four- dimensional world. Moreover in this equation a new mechanical operator is obtained. Keywords- Three and Four-Dimensional Wave Criteria, Relativistic Mechanics, Progressive Gravitational Wave. I. Introduction It is already known that three-dimensional equation of a progressive wave is d2 ψ/dx2 + d2 ψ/dy2 + d2 ψ/dz2 =1/u2 .d2 ψ/dt2 ; where ψ is wave amplitude and u is the velocity of wave. But when a progressive wave moves in four-dimensional nature, then it can obviously obey four-dimensional wave equation. Here four- dimensional formulation of a progressive wave can be drawn to deduce the reality of this wave in four- dimensional world. II. Formation of Operator-Relation In four-dimensional generalization, it is written that x1=x, x2=y, x3=z and x4=ict. In terms of differentials, dx1=dx, dx2=dy, dx3=dz and dx4=icdt. From operator representation, d/dx1=d/dx, d/dx2=d/dy, d/dx3=d/dz and d/dx4=1/ic.d/dt.Now taking square in both sides, d2 /dx1 2 =d2 /dx2 , d2 /dx2 2 =d2 /dy2 , d2 /dx3 2 =d2 /dz2 and d2 /dx4 2 =1/i2 c2 .d2 /dt2 . By addition, d2 /dx1 2 + d2 /dx2 2 + d2 /dx3 2 + d2 /dx4 2 =d2 /dx2 + d2 /dy2 + d2 /dz2 -1/c2 .d2 /dt2 . This is the desired operator-relation. III. Foundation of Wave Equation If the amplitude of a progressive wave is ψ; then multiplying in both sides of above operator-relation by ψ, it is obtained that d2 ψ/dx1 2 + d2 ψ/dx2 2 + d2 ψ/dx3 2 + d2 ψ/dx4 2 =d2 ψ/dx2 + d2 ψ/dy2 + d2 ψ/dz2 -1/c2 .d2 ψ/dt2 . This is the required wave-relation. From three-dimensional wave equation, it is written that d2 ψ/dx2 + d2 ψ/dy2 + d2 ψ/dz2 =1/u2 .d2 /dt2 or d2 ψ/dx2 + d2 ψ/dy2 + d2 ψ/dz2 -1/u2 .d2 /dt2 =0. In case of light wave, the relation is d2 ψ/dx2 + d2 ψ/dy2 + d2 ψ/dz2 - 1/c2 .d2 /dt2 =0; where c is the velocity of light. Thus by putting the above value, the four-dimensional wave equation is d2 ψ/dx1 2 + d2 ψ/dx2 2 + d2 ψ/dx3 2 + d2 ψ/dx4 2 =0. IV. Suggestion for New Operator The above wave equation be considered as the following form: [d2 /dx1 2 + d2 /dx2 2 + d2 /dx3 2 + d2 /dx4 2 ]ψ=0. Let it be assumed that d2 /dx1 2 + d2 /dx2 2 + d2 /dx3 2 + d2 /dx4 2 =◊2 =a new mechanical operator in relativistic mechanics. So ◊2 ψ=0. This is the modified form of four-dimensional wave equation of a progressive wave. V. Conclusion In course of discussion, it is discussed that the progressive wave which moves with a velocity equals to the velocity of light can obey the above wave equation. In this respect, gravitational wave is mentioned here. According to general relativity, gravitational energy is carried by gravitational waves. These waves move with the velocity of light. Thus the wave equation of a progressive gravitational wave is ◊2 ψ=0. This relation can express the reality of progressive gravitational waves. Acknowledgements I wish to thank Prof. Sriranjan Banerji and Prof. Asit Banerjee, Department of Physics, Jadavpur University for their book ‘The Special Theory of Relativity’. I indebt to thank Shree Gouri Sankar Dolai, student of Higher Secondary School for his help to type this paper. I also like to thank Mr. Koushik Dhara, Teacher of Computer Science for his inspiration to write this type of article by me. Submitted Date 19 June 2013 Accepted Date: 24 June 2013
  • 2. Proposal of New Operator in Four-Dimensional Wave Equation www.iosrjournals.org 32 | Page REFERENCES [1] R. Resnick, Introduction to special Relativity (Wiley Eastern, New Delhi, 1989). [2] H. Goldstein, Classical Mechanics (Narosa, New Delhi, 1998). [3] C. Moller, The Theory of Relativity (Oxford University Press, 1972). [4] P. G. Bergmann, Introduction to the Theory of Relativity (Prentice-Hall, New Delhi, 1969). [5] S. N. Ghoshal, Introductory Quantum Mechanics (Calcutta Book House, Reprint-2011).