pmb_phy
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Note that if you take the scalar product of observer and 4-momentum and divide by c2 youi have a scalar product (tensor of rank zero = invariant) which equals the inertial mass measured by the observer.robphy said:"relativistic mass" (being an observer-dependent/coordinate-dependent quantity) is not an invariant property of the particle alone. Instead, it is a property of the "pair consisting of the particle and an observer". Both need to be specified. If you keep the qualification of "a particle and an observer", then the property is actually an invariant [since it's a scalar formed from two distinct tangent vectors (that of the particle and that of the observer) and the metric].
I'd like to add a few things of my own here. First off - If someone here asks a question then we may not know who the person asking the question is. We can take a guess at their knowledge of SR by the question asked as is the case here. So it is appropriate to respond to the question as posted if we don't know the person asking and they're expertise in SR. Second off there are two ways to correctly respond to the question as asked: (1) Ask what they mean by "mass" of (2) tell them that if they mean "proper mass" then the answer is a photon has no mass. If they mean "inertial mass" (aka relativistic mass) then the answer is yes, photons do have mass. People learning SR should know this difference since in reading some very famous physics literarture (E.g. Feynman Lectures, etc) then they should know what the author means when he uses the term "mass". It can be gathered by the usage of the word in most cases. In the third case - There is a ton of SR literature out there for the beginner who needs to know the difference. And when they ask "Why?" then we also need to know how to respond. E.g. in particle physics, when it comes to proper mass then it is the subject being studied and it is a pain in the butt to keep using "proper mass" when that is all they use to study intrinsic properties. For the fourth reason ... whew! I'm too tired to go on.
http://www.geocities.com/physics_world/mass_paper.pdf
Problem is that its too complicated for the beginner and of no interested to those on the con-relativistic side. Only those with a truly open mind will get something out of it.
Pete
Actually, he was one of the folks I had in mind who could check this. (Is he still at Boston U.?) From what I can tell, he's a nice guy with lots of interesting insights. Too bad I only get a brief chance to chat with him at busy conferences... and at these opportunities I don't get a chance to ask my real questions.