Problem 18
Question
Tritium (\(^{3}_{1}\)H) is an unstable isotope of hydrogen; its mass, including one electron, is 3.016049 u. (a) Show that tritium must be unstable with respect to beta decay because the decay products ( \(^{3}_{2}\)He plus an emitted electron ) have less total mass than the tritium. \right. (b) Determine the total kinetic energy (in MeV) of the decay products, taking care to account for the electron masses correctly.
Step-by-Step Solution
Verified Answer
(A) Tritium is unstable due to lower mass in decay products. (B) Total kinetic energy is 0.491 MeV.
1Step 1: Compare Masses of Reactants and Products
Tritium (
^{3}_{1} ext{H}
) has a mass of 3.016049 u. The decay product,
^{3}_{2} ext{He}
, has an atomic mass of 3.016029 u. The mass of an electron is 0.000548 u. Adding the mass of an electron to
^{3}_{2} ext{He}
gives 3.016029 u + 0.000548 u = 3.016577 u. Since
^{3}_{2} ext{He}
plus an electron is lighter than tritium, the decay is energetically favorable.
2Step 2: Calculate Mass Defect
The mass defect is the difference in mass between the reactants and products. Calculate it as follows: 3.016049 u (tritium mass) - 3.016577 u (
^{3}_{2} ext{He} + electron mass) = -0.000528 u. This indicates a mass loss which is converted into energy in the form of kinetic energy.
3Step 3: Convert Mass Defect to Energy
Use Einstein's relation E=mc² to convert the mass defect to energy. First, convert mass defect from atomic mass units to MeV:
-0.000528 ext{ u} imes 931.5 ext{ MeV/u} = -0.491 ext{ MeV}
. This is the energy released as kinetic energy of the decay products.
Key Concepts
Beta DecayMass DefectKinetic EnergyAtomic Mass Unit
Beta Decay
In nuclear physics, beta decay is a process where an unstable atomic nucleus transforms into a different nucleus. This happens through the emission of beta particles, which are either electrons or positrons.
Beta decay helps to stabilize the nucleus by changing a neutron into a proton (beta-minus decay) or a proton into a neutron (beta-plus decay).
For tritium, which is an unstable hydrogen isotope, beta minus decay occurs.
This forms a fundamental understanding of why beta decay occurs and how it results in more stable, lower mass products.
Beta decay helps to stabilize the nucleus by changing a neutron into a proton (beta-minus decay) or a proton into a neutron (beta-plus decay).
For tritium, which is an unstable hydrogen isotope, beta minus decay occurs.
- This results in the transformation of tritium ( ^{3}_{1} H) into helium-3 ( ^{3}_{2}He) along with the emission of an electron.
- The process is driven by the quest for a more stable energy configuration, as seen in the differing masses.
This forms a fundamental understanding of why beta decay occurs and how it results in more stable, lower mass products.
Mass Defect
Mass defect is a fascinating concept in nuclear physics that explains how the mass of a nucleus differs from the sum of the individual masses of its protons and neutrons.
In the context of tritium decay, the mass defect is the difference between the mass of tritium and the total mass of its decay products, which include helium-3 and an electron.
This energy safety measure accounts for the kinetic energy observed in the decay products.
In the context of tritium decay, the mass defect is the difference between the mass of tritium and the total mass of its decay products, which include helium-3 and an electron.
- The calculation in the exercise shows that the tritium mass, at 3.016049 u, is greater than the combined mass of helium-3 and the electron, at 3.016577 u.
- This discrepancy is termed the "mass defect," and it is equal to -0.000528 u in this case.
This energy safety measure accounts for the kinetic energy observed in the decay products.
Kinetic Energy
Kinetic energy emerges as a significant part of understanding nuclear decay processes like that of tritium.
When tritium undergoes beta decay, the resulting mass defect is converted into kinetic energy.
This transformation follows Einstein's relation \( E=mc^2 \), where the mass defect is turned into energy.
Understanding kinetic energy in nuclear decay helps explain the behavior of particles and how they achieve a state of stability post-decay.
When tritium undergoes beta decay, the resulting mass defect is converted into kinetic energy.
This transformation follows Einstein's relation \( E=mc^2 \), where the mass defect is turned into energy.
- The exercise converts the mass defect from atomic mass units to energy measured in MeV, the standard energy unit in particle physics.
- Specifically, the mass defect of -0.000528 u translates to -0.491 MeV after considering the conversion factor \( 931.5 \text{ MeV/u} \).
Understanding kinetic energy in nuclear decay helps explain the behavior of particles and how they achieve a state of stability post-decay.
Atomic Mass Unit
The atomic mass unit (amu) is a standard unit used to express atomic and molecular masses.
It serves as a convenient way to measure tiny amounts of mass, especially useful when dealing with particles at the atomic scale.
The amu is defined as one-twelfth the mass of a carbon-12 atom, effectively serving as a "mass baseline" for atoms and molecules.
It's a small but powerful unit that makes significant contributions to the study of atomic physics.
It serves as a convenient way to measure tiny amounts of mass, especially useful when dealing with particles at the atomic scale.
The amu is defined as one-twelfth the mass of a carbon-12 atom, effectively serving as a "mass baseline" for atoms and molecules.
- In the context of the exercise, tritium's mass is measured in atomic mass units, showing how manageable these units are for nuclear calculations.
- Converting between amu and energy reveals the profound connections between mass and energy, guided by Einstein's principle of relativity (\( E=mc^2 \)).
It's a small but powerful unit that makes significant contributions to the study of atomic physics.
Other exercises in this chapter
Problem 13
What nuclide is produced in the following radioactive decays? (a) \(\alpha\) decay of \(^{239} \mathrm{Pu} ;\) (b) \(\beta^{-}\) decay of \(_{11}^{24} \mathrm{N
View solution Problem 16
What particle \((\alpha\) particle, electron, or positron) is emitted in the following radioactive decays? (a) \(_{14}^{27} \mathrm{Si} \rightarrow_{13}^{27} \m
View solution Problem 20
BIO Radioactive isotopes used in cancer therapy have a "shelf-life," like pharmaceuticals used in chemotherapy. Just after it has been manufactured in a nuclear
View solution Problem 21
The common isotope of uranium, \(^{238} \mathrm{U},\) has a half-life of \(4.47 \times 10^{9}\) years, decaying to \(^{234} \mathrm{Th}\) by alpha emission. (a)
View solution