General Magnetic Dipole Moment For an Electron in an Atom

In summary: Magnetic moment is physically not the same as angular momentum but the quantities are related by$$\hat{\vec{\mu}}=\mu_{\text{B}}(g_L \hat{\vec{L}} + g_s \hat{\vec{s}}).$$Since we deal with electrons you have ##g_L \simeq -1## and ##g_s \simeq -2##.
  • #1
rtareen
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TL;DR Summary
The book (Young and Freedman Univeristy Physics E14) uses the same symbol ##\mu_z## for the magnetic dipole moment associated with orbital angular momentum and the moment associated with spin. Are these the same?
On the first attached page ##\mu_z## is associated with orbital angular momentum (Eq. 41.34). On the following pages (Eq. 41.38) it is associated with spin angular momentum? Are these both part of the same thing? I tried to read further but the book does not address this. In example 41.6 it implies that both contribute to the total as the orbital angular momentum is zero. What is the equation for the total magnetic moment?
 

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  • #2
This smells like a chemistry book (despite it being a physics book)... They should really define a new quantity and not reuse the same symbol. In general, there are two contributions to the energy, one for intrinsic angular momentum and one for orbital angular momentum.
 
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  • #3
Haborix said:
This smells like a chemistry book (despite it being a physics book)... They should really define a new quantity and not reuse the same symbol. In general, there are two contributions to the energy, one for intrinsic angular momentum and one for orbital angular momentum.

Thank you, but do these two momentums combine into one single, total, angular momentum? (I'm two semesters removed from mechanics so I forgot).
 
  • #4
Also, do they both contribute to a single magnetic moment, or are these exclusive quantities?
 
  • #5
rtareen said:
do these two momentums combine into one single, total, angular momentum?

All of these things are operators. There are three "angular momentum" operators; the usual nomenclature and symbols are ##L## for orbital angular momentum, ##S## for spin angular momentum, and ##J## for total angular momentum. Usually textbooks will tell you that ##J = L + S##; but it should be noted that it is not always possible to split ##J## up into ##L## and ##S## in any invariant way, so in some cases ##J## is the only really meaningful operator.

rtareen said:
do they both contribute to a single magnetic moment, or are these exclusive quantities?

"Magnetic moment" is really just another word for "angular momentum" (or strictly speaking, "angular momentum of something that has magnetic properties"), usually with different units to further confuse people. Or one can think of "magnetic moment" as the result of measuring angular momentum about some axis.
 
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  • #6
PeterDonis said:
All of these things are operators. There are three "angular momentum" operators; the usual nomenclature and symbols are ##L## for orbital angular momentum, ##S## for spin angular momentum, and ##J## for total angular momentum. Usually textbooks will tell you that ##J = L + S##; but it should be noted that it is not always possible to split ##J## up into ##L## and ##S## in any invariant way, so in some cases ##J## is the only really meaningful operator.
"Magnetic moment" is really just another word for "angular momentum" (or strictly speaking, "angular momentum of something that has magnetic properties"), usually with different units to further confuse people. Or one can think of "magnetic moment" as the result of measuring angular momentum about some axis.

So if ##\vec{J} = \vec{L} + \vec{S}## then is it as simple as ##\mu_{zj} = \mu_{zl} + \mu_{zs} = -e/2m( L_z+2.002S_z)##? I just added both the moments together. Would this be the total moment in the z-direction?
 
  • #7
rtareen said:
So if ##\vec{J} = \vec{L} + \vec{S}## then is it as simple as ##\mu_{zj} = \mu_{zl} + \mu_{zs} = -e/2m( L_z+2.002S_z)##?

No, because your first equation is a vector equation and your second is not. In the simple case where we are measuring all operators about the same axis, in this case ##z##, yes, you can just add the moments since they are measurement results and the measurement results will add in that way. But if you are not measuring all the operators about the same axis, that simple relationship will no longer hold.
 
  • #8
Thank you
PeterDonis said:
No, because your first equation is a vector equation and your second is not. In the simple case where we are measuring all operators about the same axis, in this case ##z##, yes, you can just add the moments since they are measurement results and the measurement results will add in that way. But if you are not measuring all the operators about the same axis, that simple relationship will no longer hold.

Thank you PeterDonis! You are always great help. Please never leave PhysicsForums!
 
  • #9
rtareen said:
Thank you PeterDonis! You are always great help. Please never leave PhysicsForums!

You're welcome! Thanks for the kudos.
 
  • #10
PeterDonis said:
"Magnetic moment" is really just another word for "angular momentum" (or strictly speaking, "angular momentum of something that has magnetic properties"), usually with different units to further confuse people. Or one can think of "magnetic moment" as the result of measuring angular momentum about some axis.
Magnetic moment is physically not the same as angular momentum but the quantities are related by
$$\hat{\vec{\mu}}=\mu_{\text{B}}(g_L \hat{\vec{L}} + g_s \hat{\vec{s}}).$$
Since we deal with electrons you have ##g_L \simeq -1## and ##g_s \simeq -2##. For details, you may start at

https://en.wikipedia.org/wiki/Landé_g-factor
 
  • #11
vanhees71 said:
Magnetic moment is physically not the same as angular momentum

Ah, yes, that's right, the gyromagnetic ratio is different for orbital and spin angular momentum.
 
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1. What is the general magnetic dipole moment for an electron in an atom?

The general magnetic dipole moment for an electron in an atom is a measure of the strength and direction of the electron's magnetic field. It is a fundamental property of an electron and is a result of its spin and orbital motion.

2. How is the general magnetic dipole moment for an electron in an atom calculated?

The general magnetic dipole moment for an electron in an atom can be calculated using the formula μ = -g * (e/2m) * S, where μ is the magnetic moment, g is the electron's g-factor, e is the electron's charge, m is its mass, and S is its spin angular momentum.

3. What is the significance of the general magnetic dipole moment for an electron in an atom?

The general magnetic dipole moment for an electron in an atom plays a crucial role in understanding the behavior of atoms and molecules in magnetic fields. It also helps in explaining the magnetic properties of materials and is essential in various fields such as quantum mechanics, solid-state physics, and chemistry.

4. How does the general magnetic dipole moment for an electron in an atom vary in different elements?

The general magnetic dipole moment for an electron in an atom varies depending on the element and its electronic configuration. It is generally higher for atoms with unpaired electrons and lower for atoms with paired electrons. The strength of the magnetic dipole moment also increases with an increase in the atomic number of an element.

5. Can the general magnetic dipole moment for an electron in an atom be measured experimentally?

Yes, the general magnetic dipole moment for an electron in an atom can be measured experimentally using techniques such as electron spin resonance, nuclear magnetic resonance, and Mössbauer spectroscopy. These methods allow scientists to accurately determine the strength and direction of an electron's magnetic moment in an atom.

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