Originally posted by lethe
not really sure what this has to do with string theory of LQG. perhaps this would look better in the general physics forum?
here is my answer:
any physical system can accelerate when a force is exerted on it. the mass is a measure of the inertia of the system, which tells you how strongly it resists acceleration under a given force.
there is a nice alternative definition for elementary particles: mass is a casimir invariant of the Poincaré group, so it is a quantum number that labels which irrep of the Poincaré group the particle lives in.
of course, the two definitions coincide for particles at rest.
this really would look better, as Lethe says, in the general physics forum
Lethe suggests mass is "a measure of inertia" the ratio of the force applied to the acceleration produced.
This is well-defined (independent of the direction of the force) only in case the object to which force is applied is at rest. If an object is moving, then the acceleration produced by a force will depend slightly on the direction in which the force is applied and so the ratio of the two is not well-defined. IIRC Einstein pointed this out in 1905---it may have been he who introduced the terms "transverse inertia" and "longitudinal inertia" for inertia crossways to the object's motion and in line with the motion.
Anyway the simple concept of inertia is only defined for objects at rest. So a photon of light, for example, cannot have inertia because there is no frame in which it is at rest.
I agree with Lethe's choice of a definition of mass as inertia. In my experience it is the most prevalent meaning for the unmodified term "mass". Other concepts need some adjective in front of the word to indicate that a specialized meaning is intended.
the reason I especially like this definition is that it is primitive. It gives an operational non-abstract meaning to the concept, so it can be used as a foundation for building up other ideas, like energy and momentum. It only works for objects at rest, but it is real simple. Force is measurable by the watt balance by electrical means without the use of a standard mass. (one reason metrology is an interesting field these days) (Foundations of physics is also interesting---how basic concepts are defined.)
IIRC Einstein's 1905 paper that introduced E = mc
2 was entitled "Does the INERTIA of an object depend on its energy-content?" Evidently for him at that point mass meant inertia and that's good enough for me. It's traditional.
What Lethe says about a particle's (rest) mass also being a parameter of the group representation is cool.
I put "rest" in parens because in modern physics usage it is redundant: not needed in the above sentence. A particle's mass is understood by working physicists to mean its inertia in the rest frame.