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This is what the intro student (indeed myself) comes to special relativity with. The magnetic field example (again I must say that I've calculated and set the fields for
bending high speed protons using 'relativistic mass' and been quite successful in getting the beam to the target) presents us with a measured velocity but a momentum that has increased non-linearly with that velocity.
Of course. That's what momentum does. And I'll bet that I can set the fields pretty accurately too using the simple fact that the required field is directly proportional to the momentum.