This exploration delves into the nuanced relationship between relativistic mass (m′) and energy in the context of special relativity, treating m′ as an equivalent of an effective mass (mᵉᶠᶠ). The discussion unfolds by highlighting the distinctions between relativistic mass and rest mass (m₀), emphasizing that m′ is not treated as an invariant mass. The pivotal equation m′ = m₀/√1 - (v²/c²) - m₀ is examined, revealing that m′ manifests in an energetic form due to its reliance on the Lorentz factor. The unit of m′, identified as Joules (J), underscores its nature as an energetic quantity. A practical example involving an "effective mass" of 0. 001 kg (mᵉᶠᶠ = 0. 001 kg) elucidates the application of E = m′c², yielding an actual energy of 9 × 10¹³ J. This abstract encapsulates the essence of the discourse, unravelling the energetic implications of relativistic mass as an equivalent to effective mass within the framework of special relativity.
Soumendra Nath Thakur (2024) studied this question.
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