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Page 921: Practice Problems
Parent nucleus: $_{88}^{226}$ Ra that undergoes alpha decay. When a nucleus undergoes alpha decay, it gives off an $alpha$ particle or $_{2}^{4} He$, it also loses 2 protons and 2 neutrons in the process. Due to this, its atomic number (Z) decreases by 2 and mass number (A) by 4.
Since our parent nucleus has atomic number (Z$_{parent}$) = 88, and mass number (A$_{parent}$) = 226, due to alpha decay, its daughter nucleus will have an atomic number (Z$_{daughter}$) = 86, and mass number (A$_{daughter}$) = 222.
Thus the daughter nucleus is: $boxed{_{86}^{222} Rn}$
In $^{226}_{88}$Ra, $Z=88$ and $N = 226 – 88 = 138$.
When $^{226}_{88}$Ra undergoes alpha decay it looses 2 protons and 2 neutrons. So the atomic number and neutron number of daughter nucleus are $Z = 88-2 = 86$ and $N = 138 – 2 = 136$ respectively. It is the nucleus of radon (Rn).
The mass number is $A = Z + N = 86 + 136 = 222$.
So the daughter nucleus is $^{222}_{86}$Rn.
$^{226}_{88}$Ra $rightarrow$ $^{222}_{86}$Rn $+$ $^4_2$He $+$ energy.
Alpha decay of $_{86}^{226}$ Ra that releases 4.871 MeV
a) Since the nucleus of the element undergoes alpha decay, then it loses 2 protons and 2 neutrons, thus $boxed{text{decreasing its mass}}$. The energy released from this decay came from the change in mass of the nucleus.
b) The change in mass can be computed using the formula:
$$
begin{align*}
E &= (text{change in mass})E_u \
text{change in mass} &= dfrac{E}{E_u} \
&= dfrac{4.871 text{MeV}}{931.5 text{MeV}} \
&= boxed{0.00523 u}
end{align*}
$$
b) $0.00523$ u
(b) $1 :u = 931.5:MeV$
So the change in mass is given by
$4.871:cancel{MeV} times dfrac{1:u}{931.5:cancel{MeV}} = dfrac{4.871}{931.5} :u = 0.00523:u$
$Z rightarrow Z-2$
$A rightarrow A-4$
For $^{242}_{96}$Cm, $Z=96$ and $A = 242$.
When $^{242}_{96}$Cm undergoes alpha decay, the atomic number of the daughter nucleus is $Z = 96 – 2 = 94$. It is plutonium (Pu) element. The mass number of Pu is $A = 242 – 4 = 238$.
So the daughter nucleus is $^{238}_{96}$Pu.
$^{242}_{96}$Cm $rightarrow$ $^{238}_{94}$Pu $+$ $^4_2$He $+$ energy