Final unification with three gravitational constants associated with nuclear, electromagnetic and gravitational interactions


  • Satya Seshavatharam UV I-SERVE, Hyderabad, AP, India.Sr. Engineer, QA-DIP, Lanco Industries Ltd, Tirupati, AP, India.
  • Lakshminarayana S Andhra university, India





Final Unification, Gravitational Constants Associated with Strong and Electromagnetic Interactions.


By introducing two large pseudo gravitational constants assumed to be associated with strong and electromagnetic interactions, we make an attempt to combine the old Abdus Salam’s ‘strong gravity’ concept with ‘Newtonian gravity’ and try to understand the constructional features of nuclei, atoms and neutron stars in a unified approach. From the known elementary atomic and nuclear physical constants, estimated magnitude of the Newtonian gravitational constant is (6.66 to 6.70) x10-11 m3/kg/sec2. Finally, by eliminating the proposed two pseudo gravitational constants, we inter-related the Newtonian gravitational constant, Fermi’s weak coupling constant and Strong coupling constant, in a generalized approach.


[1] Ashoke Sen. Developments in Superstring theory. CERN Document server, hep-ph/9810356 (2009) 29.

[2] Edward Witten. What Every Physicist Should Know About String Theory. GR Centennial Celebration, Strings 2015, Bangalore, India. (2105). /2015/26-06-2015-Edward-Witten.pdf.

[3] Salam A, Sivaram C. Strong Gravity Approach to QCD and Confinement. Mod. Phys. Lett., A8 (4), 321-326. (1993)

[4] U. V. S. Seshavatharam and S. Lakshminarayana.Towards a workable model of final unification. International Journal of Mathematics and Physics 7, No1, 117-130 (2016).

[5] U. V. S. Seshavatharam and S. Lakshminarayana. Understanding the basics of final unification with three gravitational constants associated with nuclear, electromagnetic and gravitational interactions. 61st DAE-BRNS Symposium on Nuclear Physics. F40

[6] U. V. S. Seshavatharam and S. Lakshminarayana Understanding nuclear stability and binding energy with nuclear and electromagnetic gravitational constants. 61st DAE-BRNS Symposium on Nuclear Physics. A136.

[7] K.A. Olive et al. (Particle Data Group), Chin. Phys. C, 38, 090001 (2014).

[8] Chowdhury, P.R. et al. Modified Bethe-Weizsacker mass formula with isotonic shift and new driplines. Mod. Phys. Lett. A20 p.1605-1618. (2005).

[9] W. D. Myers et al. Table of Nuclear Masses according to the 1994 Thomas-Fermi Model. (From

[10] Srinivasan, G. The Maximum Mass of Neutron Stars. Bulletin of Astronomic Society of India, 30, 523-547. (2002).

[11] Sebastien Guillot et al. Measurement of the Radius of Neutron Stars with High S/N Quiescent Low-mass X-ray Binaries in Globular Clusters. Astrophys.J. 772 (2013).

[12] E. Rutherford, the Scattering of α and β rays by Matter and the Structure of the Atom, Philos. Mag., vol 6, ppioi.21, (1911).

[13] Robert Hofstadter, Rudolf Mössbauer. The electron-scattering method and its application to the structure of nuclei and nucleons. Nobel Lecture, (December 11, 1961).

[14] The Periodic Table of the Elements (including Atomic Radius).

[15] S. Bethke, G. Dissertori, and G.P. Salam. Quantum chromodynamics: Olive et al. (PDG), Chin. Phys. C38, 090001 (2014).

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