Problem 63
Question
\(^{8} \mathrm{Li}\) is an isotope that has a lifetime of less than one second. Its mass is \(8.022485 \mathrm{u} .\) Calculate its binding energy in \(\mathrm{MeV}\).
Step-by-Step Solution
Verified Answer
Based on the step-by-step solution provided, provide a short answer to the question:
To calculate the binding energy of Lithium-8, first determine the number of protons and neutrons, which are 3 and 5, respectively. Then, find the total mass of protons and neutrons using their respective masses in atomic mass units. Next, calculate the mass defect by subtracting the mass of the Lithium-8 nucleus from the sum of the masses of its individual protons and neutrons. Finally, convert the mass defect to energy using the mass-energy equivalence formula E=mc² and the conversion factor 1u = 931.4941 MeV/c². This will give you the binding energy of Lithium-8 in MeV.
1Step 1: Determine the number of protons and neutrons
As we are given Lithium-8, it has 8 nucleons in total, with 3 protons (since Lithium has an atomic number of 3) and the rest being neutrons. So there are 5 neutrons in the nucleus.
2Step 2: Calculate the mass of individual protons and neutrons
Knowing the atomic mass unit, which is approximately \(1.660539 \times 10^{-27} \mathrm{kg}\) and using the mass of a proton (\(1.007276 \mathrm{u}\)) and the mass of a neutron (\(1.008665 \mathrm{u}\)), we can calculate the mass of 3 protons and 5 neutrons.
Total mass of protons: \(3 \times 1.007276 \mathrm{u}\)
Total mass of neutrons: \(5 \times 1.008665 \mathrm{u}\)
3Step 3: Calculate the mass defect
Now, we will find the mass defect by subtracting the mass of the Lithium-8 nucleus from the sum of the masses of its individual protons and neutrons.
Mass defect = (Total mass of protons + Total mass of neutrons) - Mass of Lithium-8
Mass defect = \((3 \times 1.007276 \mathrm{u} + 5 \times 1.008665 \mathrm{u}) - 8.022485 \mathrm{u}\)
4Step 4: Convert mass defect to energy
Using the mass-energy equivalence formula, E=mc², where 'E' is energy, 'm' is the mass defect, and 'c' is the speed of light (\(2.99792458 \times 10^8 \mathrm{m/s}\)). We will also use the conversion factor \(1 \mathrm{u} = 931.4941 \mathrm{MeV/c^2}\) in our calculation.
Energy = Mass defect × c²
Energy = Mass defect × (\(931.4941 \mathrm{MeV/c^2}\))
5Step 5: Calculate the binding energy
Now, plug in the mass defect from step 3 into the energy equation from step 4 and solve for the binding energy.
Binding energy = (Mass defect) × (931.4941 MeV/c²)
Make sure to include units in the final answer.
Key Concepts
IsotopeMass DefectMass-Energy EquivalenceAtomic Mass Unit
Isotope
An isotope refers to any of the different forms of atoms of the same element. These forms have the same number of protons but different numbers of neutrons.
For instance, take Lithium, which normally has 3 protons, as its atomic number is 3. An isotope like \(^8\text{Li}\) is distinguished by its total of 8 nucleons. When we subtract the number of protons, we find that there are 5 neutrons in \(^8\text{Li}\). Different isotopes of the same element behave differently in nuclear calculations, such as binding energy analysis.
Isotopes are crucial because they allow scientists to study atomic behavior in different nuclear and chemical reactions, highlighting the versatility and depth of chemical elements.
For instance, take Lithium, which normally has 3 protons, as its atomic number is 3. An isotope like \(^8\text{Li}\) is distinguished by its total of 8 nucleons. When we subtract the number of protons, we find that there are 5 neutrons in \(^8\text{Li}\). Different isotopes of the same element behave differently in nuclear calculations, such as binding energy analysis.
Isotopes are crucial because they allow scientists to study atomic behavior in different nuclear and chemical reactions, highlighting the versatility and depth of chemical elements.
Mass Defect
The mass defect is the difference in mass between the measured atomic mass of an isotope and the sum of the individual masses of its constituent protons, neutrons, and electrons. It provides insight into how energy is released during nuclear reactions.
Calculating the mass defect involves summing the masses of protons and neutrons individually and subtracting the actual isotopic mass from this total.
Calculating the mass defect involves summing the masses of protons and neutrons individually and subtracting the actual isotopic mass from this total.
- The mass of 3 protons: \(3 \times 1.007276 \, \text{u}\)
- The mass of 5 neutrons: \(5 \times 1.008665 \, \text{u}\)
Mass-Energy Equivalence
Mass-energy equivalence is a fundamental concept introduced by Albert Einstein, described by the famous equation \(E=mc^2\). This equation tells us that mass can be converted into energy and vice versa.
In the context of binding energy calculations, the mass defect calculated from the isotopes can be used to find the energy released or required to hold that nucleus together.
To convert the mass defect into energy:
In the context of binding energy calculations, the mass defect calculated from the isotopes can be used to find the energy released or required to hold that nucleus together.
To convert the mass defect into energy:
- Multiply the mass defect by the speed of light squared (\(c^2\)).
Atomic Mass Unit
An atomic mass unit (u) is a unit of mass used to measure atomic and molecular weights, approximately equal to \(1.660539 \times 10^{-27} \, \text{kg}\).
It provides a more practical scale for measuring the masses of atoms and subatomic particles.
The atomic mass unit is a standard in physics and chemistry for denoting the mass on an atomic scale. It is essential in calculating the mass defect and subsequently the binding energy.
Key aspects include:
It provides a more practical scale for measuring the masses of atoms and subatomic particles.
The atomic mass unit is a standard in physics and chemistry for denoting the mass on an atomic scale. It is essential in calculating the mass defect and subsequently the binding energy.
Key aspects include:
- 1 u = 1/12 of the mass of a carbon-12 atom
- Conveniently used to express mass on a nuclear scale
Other exercises in this chapter
Problem 59
How close can a \(5.00-\mathrm{MeV}\) alpha particle get to a uranium- 238 nucleus, assuming the only interaction is Coulomb?
View solution Problem 60
Pu decays with a half-life of 24,100 yr via a 5.25 \(\mathrm{MeV}\) alpha particle. If you have a \(1.00 \mathrm{~kg}\) spherical sample of \({ }^{239} \mathrm{
View solution Problem 64
What is the total energy released in the decay \(n \rightarrow p+e^{-}+\bar{\nu}_{e} ?\)
View solution Problem 66
\(10^{30}\) Atoms of a radioactive sample remain after 10 half-lives. How many atoms remain after 20 half-lives?
View solution