This page further illustrates the use of the Three Phase ISM tool. It assumes you have considerable familiarity with the tool. If you do not, you should first try out the beginner and the 129I/127I tutorials.
The particular problem addressed in this tutorial is that of the concentration of 238U and 232Th in the interstellar medium and its three phases. These two isotopes are of interest because they are both long-lived, so they help us infer the duration of Galactic nucleosynthesis. Furthermore, they are both actinides; thus, they are only produced by the r-process of nucleosynthesis.
Solar Abundance Ratio
The solar abundances today of 238U and 232Th are 0.00893 and 0.0335, respectively, on the scale Si=106. This gives an abundance ratio of 0.00893/0.0335=0.267. We may now determine the abundance ratio at the time of the Sun's birth 4.567x109 years ago. 232Th has a half life of 1.405x1010 years. The age of the Solar System is thus 0.3246 232Th half lives, and the abundance of 232Th 4.56x109 years ago was 0.0335x20.3251=0.0420. Similarly, the 238U half life is 4.468x109 years, and we may calculate that the 238U abundance was 0.0181 at the time of the Sun's birth. This means the 238U/232Th abundance ratio at the beginning of the Solar System was 0.0181/0.0420=0.431. We may use the Three Phase ISM tool to try to best fit that number.
Galactic Disk Age
Open the Three Phase ISM Tool and enter the species information for 232Th and 238U (the half lives are in the preceding paragraph). We now seek the age of the Galactic disk. Since the Universe is now known to be 13.7 x 109 years old, and because we seek the abundance ratio at the time of the Sun's birth 4.567x109 years ago, choose a Galactic disk age of 13.7x109 minus 4.567x109 = 9.1x109 years. Galaxies may not have begun to form until 109 years after the Big Bang, so the better Galactic disk age may be 8.1x109 years. Enter that number. For Delta and k, enter the default values 2x108 years and 3, respectively.
Production Ratio
We now seek a production ratio. The actual production ratio must be obtained from a detailed calculation of r-process nucleosynthesis. Such calculations tend to give results ranging from 0.4 to 0.7. We choose here to follow the simple route of assuming equal abundances of short-lived progenitors of the two isotopes and adding the abundance they contribute to 232Th and 238U.
We begin with 232Th. The following isotopes alpha decay into 232Th in a time short compared to the 232Th half life: 236U (100%), 240Pu (100%), 244Pu (99.88%), 248Cm (91.61%), and 252Cf (96.91%). Mass numbers greater than A=252 all spontaneously fission and do not contribute to 232Th. The numbers in parenthesis give the percentage of the progenitor that actually alpha decays--the remainder is lost to fission. These numbers are obtained from the Nuclear Wallet Cards database. Adding these up, including 232Th itself, and accounting for loss due to fission, we find 1 + 1 + 1 + 0.9988 x ( 1 + 0.9161 x ( 1 + 0.9691 ) ) = 5.8 progenitors. Note that we account for the fact that 91.61% of 248Cm decays into 244Pu and then 99.88% of this new 244Pu alpha decays.
For 238U, the progenitors are itself (100%), 242Pu (100%), 246Cm (99.97%) and 250Cm (18%). Adding these up we find 1 + 1 + 0.9997 x (1 + 0.18) = 3.2 progenitors. The resulting 238U/232Th production ratio is then 3.2/5.8 = 0.55. Enter this number in the Production Ratio panel form.
Results
For the remainder of the input, the masses in the three phases and the mixing times between the phases, enter the default values Mass_1=0.3, Mass_2=0.3, Mass_3=0.4 and Time_1=Time_2=1.0e7. Here are the results of the calculation. The average ISM abundance ratio is 0.47. This is also true for all three phases since the mixing time is so short compared to the lifetimes of the two species. Interestingly, this number exceeds 0.431, the value we inferred from meteoritic data for the initial solar system ratio. A lower production ratio will solve this discrepancy, which may thus be telling us about the r-process, but perhaps there other solutions. Try the tool to find out.