In: Physics
a.) A neutron can cause 235U to fission, producing two daughter nuclei (tin and molybdenum) and three more neutrons. These three neutrons can then, in turn, cause three more 235U nuclei to split. One typical reaction is summarized as follows:
n + 235U ® 131Sn + 102Mo + 3 1n
Find the energy released in this process (in MeV), given that M(235U)=235.0439 u; M(131Sn)=130.9169 u; M(102Mo)=101.9103 u.
b.)Lise Meitner’s work in 1938 predicted that the fission of 235U would produce 200 MeV of energy per fission event. How did she do? Find a %-error.
c.)131Sn is radioactive, and typical undergoes three successive b– decays. What is the final product?
d.)How many nuclei are in 1 kg of 235U? This is, incidentally, how many fission events occur if 1 kg of 235U were to fission.
e.)In each “generation” of a chain reaction of 235U, the number of events is three times the number in the previous generation. Hence events go as 1® 3® 9® 27® 81® 243 etc. If n tells you which generation, find the limit of the ratio of (events in nth generation)/(total # of events) as n ® large. (You don’t need to use calculus, just use your calculator and notice the pattern. The series starts 1, 3/4, 9/13, etc.)
f.)Given these results, estimate the number n of chain reaction “generations” that would occur if 1 kg of 235U were to fission.
g.)If each “generation” lasts on the order of 10–7 seconds, estimate the time for the entire fission chain reaction to occur.
a) Energy released E = (M(235U) - M(131Sn) - M(102Mo) - 2 x M(n))
=>E = (235.0439 - 130.9169 - 101.9103 - 2 x 1.008664) 931.5 MeV = 185.72 MeV
b) %age error = (Exact value - approximate value) x 100 / Exact value = (185.72 - 200) x 100 / 185.72 = 7.69 %
The information about the accurate mass of U, Sn and Mo lead to the error in the estimation of released energy.
c) 131Sn - -> 131Sb - -> 131Te - -> 131I
Hence the final product will be 131I.
d) One nuclei of 235U weighs 235.0439 u = 235.0439 x 1.66 x 10-27 kg =
Number of nuclei in 1 kg = 1 / (235.0439 x 1.66 x 10-27 ) = 2.56 x 1024 nuclei.