What is the true nature of vacuum energy in quantum physics?

In summary: Well, but does the electron actually accelerate or...Yes, the electron does accelerate. It has more energy because it has more velocity.
  • #1
eoghan
207
7
Hi! Let's suppose an electron in a mono-dimensional potential well. According to Heisenberg uncertainty principle, if L is the length of the well, then I have a momentum greater than [tex]\frac{h}{L}[/tex], which means that the electron has a velocity (and so a kinetic energy) greater than [tex]\frac{h}{L*m_e}[/tex]. If I "press" the well, L becomes smaller and smaller, so the kinetic energy of the electron becomes greater and greater; according to the conservation of energy, the electron must take this energy somewhere: where does the electron take the energy needed to increase its kinetic energy?
 
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  • #2
eoghan said:
Hi! Let's suppose an electron in a mono-dimensional potential well. According to Heisenberg uncertainty principle, if L is the length of the well, then I have a momentum greater than [tex]\frac{h}{L}[/tex], which means that the electron has a velocity (and so a kinetic energy) greater than [tex]\frac{h}{L*m_e}[/tex]. If I "press" the well, L becomes smaller and smaller, so the kinetic energy of the electron becomes greater and greater; according to the conservation of energy, the electron must take this energy somewhere: where does the electron take the energy needed to increase its kinetic energy?

You "press" so you yourself provide the energy. If you do it sufficiently slowly, the ratio energy/frequency remains constant (an adiabatic invariant).

Bob_for_short.
 
  • #3
Bob_for_short said:
You "press" so you yourself provide the energy. If you do it sufficiently slowly, the ratio energy/frequency remains constant (an adiabatic invariant).

But the energy used to press the wall is used to press the wall... I mean, the energy is used to make the atoms of the wall nearer, increasing their potential energy. So the energy I use to press the wall it's transformed in potential electrostatic energy and doesn't affect the electron
 
  • #4
eoghan said:
But the energy used to press the wall is used to press the wall... I mean, the energy is used to make the atoms of the wall nearer, increasing their potential energy. So the energy I use to press the wall it's transformed in potential electrostatic energy and doesn't affect the electron

No, if the walls are neutral, then there is no interaction potential between them. They serve just to reflect the electron so they are under pressure of the electron wave.
 
  • #5
Sorry.. I don't uderstand:confused:... what do you mean by "to be under pressure of electron wave"?
 
  • #6
For simplicity imagine a classical particle reflecting from the left and right walls. It makes pressure on walls and likewise.
 
  • #7
Ah, ok... do you mean something like a radiation pressure?
 
  • #8
eoghan said:
Ah, ok... do you mean something like a radiation pressure?

Yes, the radiation pressure in a limited system (with reflecting walls) is of the same nature.
 
  • #9
eoghan said:
Hi! Let's suppose an electron in a mono-dimensional potential well. According to Heisenberg uncertainty principle, if L is the length of the well, then I have a momentum greater than [tex]\frac{h}{L}[/tex], which means that the electron has a velocity (and so a kinetic energy) greater than [tex]\frac{h}{L*m_e}[/tex]. If I "press" the well, L becomes smaller and smaller, so the kinetic energy of the electron becomes greater and greater; according to the conservation of energy, the electron must take this energy somewhere: where does the electron take the energy needed to increase its kinetic energy?

That's the so-called Zero-point energy. You can get it for "free". see this page: http://www.scientificamerican.com/article.cfm?id=follow-up-what-is-the-zer

What is the 'zero-point energy' (or 'vacuum energy') in quantum physics? Is it really possible that we could harness this energy?
 
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  • #10
eoghan said:
Hi! Let's suppose an electron in a mono-dimensional potential well. According to Heisenberg uncertainty principle, if L is the length of the well, then I have a momentum greater than [tex]\frac{h}{L}[/tex], which means that the electron has a velocity (and so a kinetic energy) greater than [tex]\frac{h}{L*m_e}[/tex]. If I "press" the well, L becomes smaller and smaller, so the kinetic energy of the electron becomes greater and greater; according to the conservation of energy, the electron must take this energy somewhere: where does the electron take the energy needed to increase its kinetic energy?


No HUP is about the statistical outcome of measurments, not quantum equation of motion. The quantum equation of motion is governed by the Schrödinger Equation.
 
  • #11
feynmann said:
Zero-point energy is "free". see this page: http://www.scientificamerican.com/article.cfm?id=follow-up-what-is-the-zer

What is the 'zero-point energy' (or 'vacuum energy') in quantum physics? Is it really possible that we could harness this energy?

The zerop point energy is per definition the lowest energy a system can have, thus we can not "use" it, e.g. we can not de-excite the hydrogen atom further down than it's ground state.
 
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  • #12
malawi_glenn said:
No HUP is about the statistical outcome of measurments, not quantum equation of motion. The quantum equation of motion is governed by the Schrödinger Equation.

Well, but does the electron actually accelerate or doesn't?
 
  • #13
eoghan said:
Well, but does the electron actually accelerate or doesn't?

Electron (or any other particle) in the ground state is a standing wave of the lowest harmonic. It should exist. If there is no wave, there is no electron and there is no wave equation for it.

You can think without contradiction that the electron do not accelerate in the ground or in any excited state. It "accelerates" and radiates while transitions from one state to another.

Bob.
 
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  • #14
eoghan said:
Well, but does the electron actually accelerate or doesn't?

define acceleration in quantum mechanics...
 
  • #15
According to HUP, things just don't like to be confined and become more and more agitated when attempts are made to confine them in ever smaller containers of any type.

One way to think about this: According to E = hf , energy increases as frequency does which means wavelength decreases; as a container is made smaller the wavelength of the contained particle is forcefully decreased...hence it's energy is forced to increase...it becomes more and more agitated

I'm unsure if vacuum energy is a source; I have always wondered if we really don't understand it whatsoever and the discovery of massive amounts of dark energy has just made me more suspicious...anyway, the work done to increase the pressure by making the container smaller seems more appealing...
 
  • #16
Naty1 said:
According to HUP, things just don't like to be confined and become more and more agitated when attempts are made to confine them in ever smaller containers of any type.

HUP is about the statistical outcome of measurements, not energy levels...
 
  • #17
malawi_glenn said:
HUP is about the statistical outcome of measurements, not energy levels...

More importantly, it relates the statistical standard deviation in the measurements, not the magnitude of the mean of the measurements.
 
  • #18
Born2bwire said:
More importantly, it relates the statistical standard deviation in the measurements, not the magnitude of the mean of the measurements.

That is correct
 
  • #19
feynmann said:
What is the 'zero-point energy' (or 'vacuum energy') in quantum physics? Is it really possible that we could harness this energy?

The Casimir effect (kind of Van der Waals force) is too weak to be harnessed, in my opinion.

I would like to give my own view on the "zero-point" or "vacuum" energy. Normally they say that the vacuum field fluctuations exist in the vacuum. In my opinion it is not exact since, for example, the quantized electromagnetic field is in permanent "interaction" with electrons (or charges). So it is more naturally to consider them as "fluctuations" in a compound system charge+EMF. Such a model of charge-field coupling (an electronium) has been advanced in "Reformulation instead of Renormalizations" and in "Atom as a "dressed" nucleus" by Vladimir Kalitvianski available in arXiv. The vacuum field wave functions are similar to the ground state atomic wave functions which also describe a compound system (an atom). Each charge has its own quantum EMF oscillators just like each nucleus in atoms has its own electrons around. This physical model seems unusual first but quite natural after analysing the atom description reported in Atom as a "dressed" nucleus". These "atomic" results are correct but are still rather unknown.

Bob_for_short.
 

1. What is an electron in a potential well?

An electron in a potential well refers to the behavior of an electron when it is confined within a region of space where it experiences a potential energy barrier. This can occur in various physical systems, such as atoms, molecules, and solid-state materials.

2. What causes an electron to be trapped in a potential well?

An electron can be trapped in a potential well due to the presence of attractive forces that create a potential energy barrier. This barrier prevents the electron from escaping and keeps it confined within the well.

3. How does the depth of a potential well affect the electron's behavior?

The depth of a potential well determines the amount of energy required for the electron to escape. A deeper potential well requires more energy for the electron to escape, while a shallower potential well allows the electron to escape more easily.

4. How does the shape of a potential well affect the electron's behavior?

The shape of a potential well determines the distribution of electron energy levels within the well. A narrower potential well results in a smaller range of energy levels for the electron, while a wider potential well allows for a larger range of energy levels.

5. What are some practical applications of studying electrons in potential wells?

Studying electrons in potential wells is important in understanding the behavior of electrons in various physical systems. This knowledge is essential in fields such as quantum mechanics, solid-state physics, and electronics. Some practical applications include the development of electronic devices and materials with specific electronic properties.

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