Chapter 15: Problem 19
To illustrate the principle, let's say we start with a nucleus whose mass is \(200.000\) a.m.u. and inject \(1,600 \mathrm{MeV}\) of energy to completely dismantle the nucleus into its constituent parts. How much mass would the final collection of parts have? a) the exact same: \(200.000\) a.m.u. b) less than \(200.000\) a.m.u. c) more than \(200.000\) a.m.u.