Planck (1906a) defined the relativistic
momentum and gave the correct values for the longitudinal and transverse mass by correcting a slight mistake of the expression given by Einstein in 1905. Planck's expressions were in principle equivalent to those used by Lorentz in 1899.
[80] Based on the work of Planck, the concept of
relativistic mass was developed by
Gilbert Newton Lewis and
Richard C. Tolman (1908, 1909) by defining mass as the ratio of momentum to velocity. So the older definition of longitudinal and transverse mass, in which mass was defined as the ratio of force to acceleration, became superfluous. Finally, Tolman (1912) interpreted relativistic mass simply as
the mass of the body.
[81] However, many modern textbooks on relativity do not use the concept of relativistic mass anymore, and
mass in special relativity is considered as an invariant quantity.