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Title: Revisiting Ramakrishnan's approach to relatively. [Velocity addition theorem uniqueness]

Abstract

The conditions under which the velocity addition theorem (VAT) is formulated by Ramakrishnan gave rise to doubts about the uniqueness of the theorem. These conditions are rediscussed with reference to their algebraic and experimental implications. 9 references.

Authors:
;
Publication Date:
Research Org.:
Indian Inst. of Tech., Madras
OSTI Identifier:
6088628
Resource Type:
Journal Article
Journal Name:
J. Math. Anal. Appl.; (United States)
Additional Journal Information:
Journal Volume: 67:2
Country of Publication:
United States
Language:
English
Subject:
71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; RELATIVITY THEORY; VELOCITY; ALGEBRA; FIELD THEORIES; GENERAL RELATIVITY THEORY; MATHEMATICS; 657003* - Theoretical & Mathematical Physics- Relativity & Gravitation

Citation Formats

Nandi, K.K., and Shankara, T.S. Revisiting Ramakrishnan's approach to relatively. [Velocity addition theorem uniqueness]. United States: N. p., 1979. Web. doi:10.1016/0022-247X(79)90032-5.
Nandi, K.K., & Shankara, T.S. Revisiting Ramakrishnan's approach to relatively. [Velocity addition theorem uniqueness]. United States. doi:10.1016/0022-247X(79)90032-5.
Nandi, K.K., and Shankara, T.S. Thu . "Revisiting Ramakrishnan's approach to relatively. [Velocity addition theorem uniqueness]". United States. doi:10.1016/0022-247X(79)90032-5.
@article{osti_6088628,
title = {Revisiting Ramakrishnan's approach to relatively. [Velocity addition theorem uniqueness]},
author = {Nandi, K.K. and Shankara, T.S.},
abstractNote = {The conditions under which the velocity addition theorem (VAT) is formulated by Ramakrishnan gave rise to doubts about the uniqueness of the theorem. These conditions are rediscussed with reference to their algebraic and experimental implications. 9 references.},
doi = {10.1016/0022-247X(79)90032-5},
journal = {J. Math. Anal. Appl.; (United States)},
number = ,
volume = 67:2,
place = {United States},
year = {1979},
month = {2}
}