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Under certain rare circumstances, a nucleus can decay by emitting a particle more massive than an alpha particle. Consider the decays Ra223Pb209+C12andRa223Ra219+He4

Calculate the Qvalue for the (a) first and (b) second decay and determine that both are energetically possible. (c) The Coulomb barrier height for alpha-particle emission is 30.0 MeV. What is the barrier height for14Cemission ? (Be careful about the nuclear radii.) The needed atomic masses are

Ra223223.01850uC1414.00324uRa20920.98107uC44.00260uRa219219.00948u

Short Answer

Expert verified
  1. The Q-value for the first decay is 31.8 MeV.
  2. The Q-value for the second decay is 5.98 MeV .
  3. The barrier height for C14emission is 86 MeV.

Step by step solution

01

Given data

The atomic masses of the nuclides are given.

The Coulomb barrier height for alpha-particle emission,U2=30MeV

02

Understanding the concept of decay  

Massive nuclides tend to undergo alpha decay releasing disintegration energy. The disintegration energy, also known as the Q-value, is the energy that is absorbed or released when a nuclear reaction takes place. The nuclear radii for both the system of decay are approximately in the same energy system, thus the potential barrier is only dependent on the product of charges.

Formulae:

The disintegration energy of a nuclear reaction,

Q=mparentnucleus-mdaughternucleic2(1)

The potential energy of a system of two charged nuclei, U=kq1q2r...2

03

a) Calculation of the disintegration energy for the first decay

The disintegration energy or the Q-valuefor radium-223 鈥渄ecaying鈥 into lead-209 and carbon-12is given using the atomic masses and equation (1) as follows:

Q=m223Ra-m209Pb-m12Cc2=223.01850u-208.98107u-14.00324u931.5MeV/u=31.8MeV

Hence, the disintegration energy is 31.8MeV.

04

b) Calculation of the disintegration energy for the second decay

The disintegration energy or the Q-valuefor radium-223 鈥渄ecaying鈥 into radium-219 and helium-4is given using the atomic masses and equation (1) as follows:

Q=m223Ra-m219Rn-m4Hec2=223.01850u-219.00948u-4.00260u931.5MeV/u=5.98MeV

Hence, the disintegration energy is 5.98 MeV.

05

c) Calculation for the barrier height for the carbon emission

From equation (2), we can get that the potential energy or the potential barrier height is proportional toUq1q2r

Now, for the same universe that is the decay is from the same radium-223 nucleus, thus the nuclear radii of the system having the decay are approximately same.

Thus, using the above relation, the potential barrier height for the carbon-14 emission is given as follows:

U1qPbqCqRnqHeU2=82e6e86e2e30MeV=86MeV

Hence, the value of the barrier height is 86 MeV.

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The radionuclide C11decays according to

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role="math" localid="1661759171201" Q=(mC-mB-2me)c2

WheremCandmBare the atomic masses ofC11andB11, respectively, andmeis the mass of a positron. (b) Given the mass valuesmC=11.011434u,mB=11.009305uandme=0.0005486u, calculate Qand compare it with the maximum energy of the emitted positron given above. (Hint:LetmC andmBbe the nuclear masses and then add in enough electrons to use the atomic masses.)

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