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Energy of Gamma Photon Emitted in Alpha Decay of Radium

Consider a 88226Ra^{226}_{88}\text{Ra} nucleus initially at rest in its ground state that undergoes α\alpha-decay to form an excited 86222Rn^{222}_{86}\text{Rn} nucleus. The emitted α\alpha particle has a kinetic energy of 4.44 MeV4.44\text{ MeV}. The 86222Rn^{222}_{86}\text{Rn} nucleus subsequently transitions to its ground state via γ\gamma-decay. Find the energy of the emitted γ\gamma photon in keV\text{keV}. [Given: atomic mass of 88226Ra=226.005 u^{226}_{88}\text{Ra} = 226.005\text{ u}, atomic mass of 86222Rn=222.000 u^{222}_{86}\text{Rn} = 222.000\text{ u}, atomic mass of α particle=4.000 u\alpha\text{ particle} = 4.000\text{ u}, 1 u=931 MeV/c21\text{ u} = 931\text{ MeV/c}^2, and cc is the speed of light]

Official Numerical Answer135

Step-by-Step Solution

The total energy released (QtotalQ_{\text{total}}) in the decay of a 88226Ra^{226}_{88}\text{Ra} nucleus from its ground state to the ground state of 86222Rn^{222}_{86}\text{Rn} is given by the mass defect:

Δm=M(Ra)−M(Rn)−M(α)\Delta m = M(\text{Ra}) - M(\text{Rn}) - M(\alpha)

Given values: M(Ra)=226.005 uM(\text{Ra}) = 226.005\text{ u} M(Rn)=222.000 uM(\text{Rn}) = 222.000\text{ u} M(α)=4.000 uM(\alpha) = 4.000\text{ u}

Δm=226.005−222.000−4.000=0.005 u\Delta m = 226.005 - 222.000 - 4.000 = 0.005\text{ u}

Using 1 u=931 MeV/c21\text{ u} = 931\text{ MeV}/c^2, the total QQ-value is: Qtotal=0.005×931 MeV=4.655 MeVQ_{\text{total}} = 0.005 \times 931\text{ MeV} = 4.655\text{ MeV}

Now, consider the α\alpha-decay of 88226Ra^{226}_{88}\text{Ra} at rest to an excited state of 86222Rn^{222}_{86}\text{Rn}. Let QαQ_{\alpha} be the energy released in this step. By conservation of linear momentum, the momenta of the excited 86222Rn^{222}_{86}\text{Rn} nucleus and the α\alpha-particle are equal in magnitude:

pRn=pαp_{\text{Rn}} = p_{\alpha}

The kinetic energy of the recoil 86222Rn^{222}_{86}\text{Rn} nucleus is: KRn=pRn22MRn=MαMRnKαK_{\text{Rn}} = \frac{p_{\text{Rn}}^2}{2 M_{\text{Rn}}} = \frac{M_{\alpha}}{M_{\text{Rn}}} K_{\alpha}

Thus, the energy QαQ_{\alpha} shared between the kinetic energies of the α\alpha-particle and the recoil nucleus is: Qα=Kα+KRn=Kα(1+MαMRn)Q_{\alpha} = K_{\alpha} + K_{\text{Rn}} = K_{\alpha} \left(1 + \frac{M_{\alpha}}{M_{\text{Rn}}}\right)

Given Kα=4.44 MeVK_{\alpha} = 4.44\text{ MeV}, Mα=4.000 uM_{\alpha} = 4.000\text{ u}, and MRn=222.000 uM_{\text{Rn}} = 222.000\text{ u}: Qα=4.44×(1+4222)=4.44×(1+2111)=4.44×113111=4.52 MeVQ_{\alpha} = 4.44 \times \left(1 + \frac{4}{222}\right) = 4.44 \times \left(1 + \frac{2}{111}\right) = 4.44 \times \frac{113}{111} = 4.52\text{ MeV}

The excitation energy E∗E^* of the 86222Rn^{222}_{86}\text{Rn} nucleus is the difference between the total energy available and the energy released in the α\alpha-decay:

E∗=Qtotal−Qα=4.655 MeV−4.520 MeV=0.135 MeVE^* = Q_{\text{total}} - Q_{\alpha} = 4.655\text{ MeV} - 4.520\text{ MeV} = 0.135\text{ MeV}

When the excited 86222Rn^{222}_{86}\text{Rn} nucleus transitions to its ground state, it emits a γ\gamma-photon of energy equal to this excitation energy (since the nuclear recoil during photon emission is negligible):

Eγ=E∗=0.135 MeV=135 keVE_{\gamma} = E^* = 0.135\text{ MeV} = 135\text{ keV}

Answer: 135