::::which states only that a system's mass will change by a small amount when it releases or absorbs energy. It's still E=mc<sup>2</sup>; the difference is the definition of m and E. For example, it describes the rather difficult-to-ignore fact that a <sup>4</sup>He nucleus weighs less than the two deuterons from which it was formed. This concept is easier to prove than the more general statement of mass-energy equivalence. [[User:Spielman|Spielman]] 13:06, 11 February 2013 (EST) | ::::which states only that a system's mass will change by a small amount when it releases or absorbs energy. It's still E=mc<sup>2</sup>; the difference is the definition of m and E. For example, it describes the rather difficult-to-ignore fact that a <sup>4</sup>He nucleus weighs less than the two deuterons from which it was formed. This concept is easier to prove than the more general statement of mass-energy equivalence. [[User:Spielman|Spielman]] 13:06, 11 February 2013 (EST) |