Nuclear binding energy and mass difference

In summary, the textbook on nuclear physics discusses the concept of atomic weight and mass number and how they relate to the mass difference, denoted by Δ. The Δ value is the difference between the atomic weight and the mass number, expressed in MeV. The more stable a nucleus is, the greater amount of energy is required to break it apart, known as its binding energy. The atomic mass unit is defined as 1/12 of the mass of an atom of carbon, and the mass defect of a nucleus can be converted to energy in units of MeV. However, there may be errors in the terminology used, as the book states that Δ = M - A, but the units do not match up.
  • #1
Hercuflea
596
49

Homework Statement


The textbook on nuclear physics I am going through says:

"The atomic weight M of a nuclide of mass number A can be found in the mass difference, ##\Delta##, given in column 3. The quantity ##\Delta = M-A## gives the difference between the nuclides atomic weight and its atomic mass number, expressed in MeV."

Homework Equations



##\Delta = M-A##

The Attempt at a Solution


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My question is if the mass difference is defined to be the mass of a particle minus the sum of the masses of the particle's parts, why does a free neutron have a mass difference of ##\Delta = 8.0714 MeV## instead of ##\Delta = 0 MeV##?

Also, if the atomic weight of Carbon, (from the periodic table) is 12.011 amu and it's atomic mass A=12, then why is ##\Delta =M - A = 0## for Carbon?
 
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  • #2
The nucleons in a stable nucleus are held tightly together.

Therefore, energy is required to separate a stable nucleus into its constituent protons and neutrons.

The more stable the nucleus is, the greater is the amount of energy needed to break it apart. The required energy is called the binding energy of the nucleus.
Hercuflea said:
Also, if the atomic weight of Carbon, (from the periodic table) is 12.011 amu and it's atomic mass A=12, then why is Δ=M−A=0Δ=M−A=0\Delta =M - A = 0 for Carbon?

The atomic mass unit is defined as 1/12 of the mass of an atom of carbon. In terms of this unit, the mass of a carbon atom is exactly 12 u.
If one adds up the nucleon's masses in atomic mass unit (u) one will get a mass defect and its equivalent energy is binding energy of carbon.
 
  • #3
drvrm said:
The atomic mass unit is defined as 1/12 of the mass of an atom of carbon. In terms of this unit, the mass of a carbon atom is exactly 12 u.
If one adds up the nucleon's masses in atomic mass unit (u) one will get a mass defect and its equivalent energy is binding energy of carbon.
Why does the book say the mass difference is atomic weight minus atomic mass? Wouldn't that be 12.011 - 12 = 0.011 amu?
 
  • #4
Hercuflea said:
Why does the book say the mass difference is atomic weight minus atomic mass? Wouldn't that be 12.011 - 12 = 0.011 amu?

I think there is error in terminology being used- In popular nuclear physics atomic weights are being used(it may include the mass of electrons)
Carbon -12 is a nuclide (a group of protons and neutrons) these protons/neutrons are not having mass as equal to one atomic mass unit
A proton has mass = 1,0073 u ,similarly a neutron has mass= 1.0087 u so adding up together these twelve nucleons will have larger mass and the
mass defect converted to energy units will give its binding energy say about 7.5 MeV per nucleon as 1 u= 931.5 MeV
in the above about .008 u is average difference per nucleon so converted to energy it will approx. to about 7.5 MeV

one can see detail calculations in <http://staff.orecity.k12.or.us/les.sitton/Nuclear/313.htm> for model calculations on say He nucleus etc.
 
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  • #5
I still don't really understand why the mass defect of a single neutron should be 8.0714 MeV?
 
  • #6
In other words, my question is basically about what the textbook means when it says
$$ \Delta = M - A$$

It seems to be subtracting a unitless number A from a number M with units of either ##\frac{MeV}{c^2}## or ##u##? The table in the back provides ##\Delta## values in ##MeV##, not ##\frac{MeV}{c^2}##. How is he getting units of ##MeV## by subtracting ##\frac{MeV}{c^2} - (unitless~integer)##?
 

What is nuclear binding energy?

Nuclear binding energy is the amount of energy required to hold the nucleus of an atom together. It is also known as the potential energy of the strong nuclear force that binds protons and neutrons together in the nucleus.

How is nuclear binding energy calculated?

Nuclear binding energy is calculated by taking the difference between the mass of an atom and the sum of the masses of its individual protons and neutrons. This difference is known as the mass defect, and it represents the amount of mass that is converted into energy during the formation of the nucleus.

What is the relationship between nuclear binding energy and nuclear stability?

The higher the nuclear binding energy, the more stable the nucleus is. This is because a higher binding energy means that more energy is required to break apart the nucleus, making it less likely to undergo nuclear reactions or decay.

How does nuclear binding energy affect nuclear reactions?

In nuclear reactions, the difference in nuclear binding energy between the reactants and products determines the amount of energy released or absorbed. If the binding energy of the products is higher than that of the reactants, energy will be released, and vice versa.

What is the role of nuclear binding energy in nuclear power plants?

Nuclear power plants utilize nuclear binding energy by splitting the nuclei of atoms (nuclear fission) to produce heat, which is then converted into electricity. The energy released during this process is a result of the mass defect and the conversion of mass into energy, as described by Einstein's famous equation E=mc².

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