Take the total differential of the logarithm of the relativistic energy, with the speed of light fixed:
Using the chain rule,
Every term is a dimensionless fractional change. The differential relation is exact; applying it to finite small changes is a first-order Taylor expansion.
Equal energies mean in the linear approximation. Evaluate the coefficients at particle , where , and use . The fractional rest mass change is
Consequently
As a check beyond the requested first-order approximation, exact equality of relativistic energy gives , consistent with the sign and approximate size of the difference.

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