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The differential form of the Momentum Principle is the equation Ftot where in general = ymů In non-relativistic physics, and assuming constant mass, this principle takes on the familiar form involving acceleration, Ētot=må. For a relativistic particle, what would be the corresponding equation containing acceleration? To keep things simple, assume the particle is traveling in one dimension. Write your answer symbolically using the variables m, a, v, c and/or gamma. (And use the word "gamma" in your response rather than the Greek symbol.) F=