• anonymous
Review: Limits In the theory of relativity, the mass of a particle with velocity v is $$\sf m = \large \frac{m_0}{\sqrt{1 − v^2/c^2}}$$ where $$\sf m_0$$ is the mass of the particle at rest and c is the speed of light. What happens as $$\sf v → c^−$$?
Mathematics

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