The fissionability parameter is defined as the atomic number squared divided by the mass number for any given nucleus $\left(Z^{2} / A\right) .$ It can be shown that when this parameter is less than 44 , a nucleus will be stable against small deformation; essentially, the nucleus will be stable against spontaneous fission. Calculate the value of this parameter for (a) ${ }^{235} \mathrm{U},(\mathrm{b})^{238} \mathrm{U},(\mathrm{c})^{239} \mathrm{Pu}$, (d) ${ }^{240} \mathrm{Pu},(\mathrm{e})^{246} \mathrm{Cf}$, and (f) ${ }^{254} \mathrm{Cf}$.