What is the percentage of useful energy that we get from antimatter ?

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    Antimatter Energy
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Discussion Overview

The discussion revolves around the theoretical aspects of energy production from antimatter annihilation, specifically focusing on what constitutes "useful energy" in this context. Participants explore the types of energy released during annihilation, including photons, neutrinos, and pions, and consider their implications for practical applications such as nuclear reactors and explosions.

Discussion Character

  • Theoretical exploration
  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that a significant portion of energy from antimatter annihilation is in the form of neutrinos, which they argue cannot be considered useful energy.
  • Others propose that the annihilation primarily produces photon pairs, specifically mentioning electron-positron annihilation resulting in 511 keV photons.
  • There is a claim that hadron annihilations produce more pions than photons, with charged pion decays leading to neutrinos, suggesting that neutrinos account for a considerable fraction of the total energy.
  • Some participants question the validity of estimating that at least 50% of the energy goes to the explosion, seeking clarification on the origin of this figure.
  • Concerns are raised about the harmful radiation produced by antimatter annihilation, particularly regarding gamma rays and their implications for shielding requirements.
  • Participants discuss the kinetic energy of pions and whether it should be considered lost energy, with some suggesting that charged pions interact with matter and can transfer kinetic energy, while others note that uncharged pions may not interact before decaying.
  • There is a discussion about the fate of kinetic energy if pions decay before losing it, with some asserting that decay products retain this energy.

Areas of Agreement / Disagreement

Participants express differing views on the nature and quantity of useful energy derived from antimatter annihilation, with no consensus reached on the percentage of energy that can be classified as useful. The discussion remains unresolved regarding the implications of neutrinos and pions in this context.

Contextual Notes

Participants acknowledge the theoretical nature of the discussion, emphasizing the lack of practical experimentation with antimatter and the complexities involved in measuring and defining useful energy in annihilation processes.

Hurricane93
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This is a theoretical question since we haven't made enough antimatter to try it in reality of course. But I am asking about the physics part in this.

Also, by "useful energy" I mean the energy we are able to use either as a heating source for something like a nuclear reactor, or as energy for an explosion like nuclear explosions.

If I am not mistaken, a large part of the energy we get from the annihilation is in the form of neutrinos, which we for some reason can't consider them useful energy. So now, if we subtract the energy of the neutrinos, it is safe to consider the rest as useful energy as I explained ?

Please try to be as simple as possible because I don't speak English very well.
 
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I'm not sure what you are asking here. Currently, there is NO method of getting ANY "useful energy" from matter-anti-matter interaction.
 
Hurricane93 said:
This is a theoretical question since we haven't made enough antimatter to try it in reality of course. But I am asking about the physics part in this.

Also, by "useful energy" I mean the energy we are able to use either as a heating source for something like a nuclear reactor, or as energy for an explosion like nuclear explosions.

If I am not mistaken, a large part of the energy we get from the annihilation is in the form of neutrinos, which we for some reason can't consider them useful energy. So now, if we subtract the energy of the neutrinos, it is safe to consider the rest as useful energy as I explained ?

Please try to be as simple as possible because I don't speak English very well.

I believe you are mistaken about the output of annihilation. It consists of photon pairs. For example, electron-positron ends up as two 511 kev photons.
 
@mathman: Hadron annihilations produce more pions than photons, and charged pion decays lead to neutrinos.

snorkack and I discussed that in this thread. We could not find a number, but neutrinos will get a significant fraction of the total energy.
 
mfb said:
@mathman: Hadron annihilations produce more pions than photons, and charged pion decays lead to neutrinos.

snorkack and I discussed that in this thread. We could not find a number, but neutrinos will get a significant fraction of the total energy.

So as the link you provided states, is it safe to consider at minimum that 50% of the energy goes to the explosion ?
Also, does matter and antimatter annihilation produce harmful radiation ?
If a large amount of gamma rays is released, then we should consider this bomb a source of radiation, shouldn't we ?
 
Hurricane93 said:
So as the link you provided states, is it safe to consider at minimum that 50% of the energy goes to the explosion ?
I don't see where that number comes from.
Also, does matter and antimatter annihilation produce harmful radiation ?
Sure.
If a large amount of gamma rays is released, then we should consider this bomb a source of radiation, shouldn't we ?
Sure.
 
mfb said:
I don't see where that number comes from.

Check the 3rd post in the link you provided, please.

One last thing. It is known that gamma radiation require less shielding than neutron radiation, so in case of a "hypothetical" Antimatter reactor, would that mean that it would need less massive shielding to reduce the radiation to non-harmful levels ?
 
By the way , energy doesn't go into explosion like people go into a house , the explosion or the artistic effects of it like mushroom cloud , a blast wave and a lot of heat are just different side effects of the primary nuclear reaction going on at the heart of the bomb or whatever , a lot of heat is produced which rapidly expands creating a shock wave , all kinds of radiation is produced.

you could use antimatter for energy production , there is only a slight problem , we don't have any and as it turns out , atleast with our current understanding and methods it takes a lot of energy to make it so in the end of the day you wasted energy and got back the same or even less + you have to contain it somewhere as normally it would try to annihilate with matter.
 
Hurricane93 said:
Check the 3rd post in the link you provided, please.
Ah. Hmm, sounds reasonable. This applies to bombs only, as it is not reasonable to keep all muons within some container.

One last thing. It is known that gamma radiation require less shielding than neutron radiation, so in case of a "hypothetical" Antimatter reactor, would that mean that it would need less massive shielding to reduce the radiation to non-harmful levels ?
That depends on the energy. If the neutron energy is not too high (below 1 GeV), they are easier to shield. To contain the gamma rays, something like 1-3m of iron is a good start.
 
  • #10
mfb said:
Ah. Hmm, sounds reasonable. This applies to bombs only, as it is not reasonable to keep all muons within some container.

What about the kinetic energy of the pions ?
should we consider them as lost energy too ?
 
  • #11
Hurricane93 said:
What about the kinetic energy of the pions ?
should we consider them as lost energy too ?

If electrically charged, then they probably interact readily with normal matter like any charged particle and can transfer their kinetic energy. But if they aren't charged, then it's likely they don't interact before they decay, as their lifetimes are so short and without electric charge they would pass through matter in a similar manner to neutrons.
 
  • #12
Drakkith said:
If electrically charged, then they probably interact readily with normal matter like any charged particle and can transfer their kinetic energy. But if they aren't charged, then it's likely they don't interact before they decay, as their lifetimes are so short and without electric charge they would pass through matter in a similar manner to neutrons.

Charged pions have a mean lifetime in the range of a nanosecond, so does this mean they will transfer their kinetic energy during this relatively short lifetime ?
 
  • #13
The interactions between charged pions and electrons are similar to those between muons and electrons - they lose some energy, but not enough to get stopped within the bomb.
Nuclear interactions are different.
 
  • #14
mfb said:
The interactions between charged pions and electrons are similar to those between muons and electrons - they lose some energy, but not enough to get stopped within the bomb.
Nuclear interactions are different.

Could you please explain a little bit more ?
Like just before decaying, would the charged pion have lost all of its kinetic energy ?
 
  • #15
Hurricane93 said:
Charged pions have a mean lifetime in the range of a nanosecond, so does this mean they will transfer their kinetic energy during this relatively short lifetime ?

If they hit something, then yes, they will transfer at least part of their kinetic energy.
Of course, I'm assuming that if a pion hits a proton with enough force then there are other interactions possible other than a simple transfer of kinetic energy. I don't know how much energy the pions from an antimatter reaction have.
 
  • #16
Drakkith said:
If they hit something, then yes, they will transfer at least part of their kinetic energy.
Of course, I'm assuming that if a pion hits a proton with enough force then there are other interactions possible other than a simple transfer of kinetic energy. I don't know how much energy the pions from an antimatter reaction have.

Should we consider the air as "something" ?
Also, what will happen if it decays before it loses its kinetic energy ? where will this energy go ?
 
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  • #17
Hurricane93 said:
Should we consider the air as "something" ?

I would.

Also, what will happen if it decays before it loses its kinetic energy ? where will this energy go ?

The decay products retain this energy.
 
  • #18
Drakkith said:
The decay products retain this energy.

I don't really know how fast charged pion move, but assuming it moves at the speed of light, with its 70 nanosecond mean lifetime, it will travel 21 meters in its lifetime. So it will surely go through the casing of the bomb for example. So if this material is say 5 cm thick of iron or lead, would this material get a significant part of the kinetic energy of the pion ?

Sorry if I have been asking too many question, but I think this is the last one. Thanks in advance.
 
  • #19
Hurricane93 said:
I don't really know how fast charged pion move, but assuming it moves at the speed of light,

A pion is a particle that has mass. As such it will never go the speed of light. Such a thing is impossible.
 
  • #20
Hurricane93 said:
Like just before decaying, would the charged pion have lost all of its kinetic energy ?
That is very unlikely.

So if this material is say 5 cm thick of iron or lead, would this material get a significant part of the kinetic energy of the pion ?
At least not via the electromagnetic interaction. Some pions will do inelastic collisions with nuclei, in that case they can deposit most of their energy within 5cm of iron or lead.
Drakkith said:
A pion is a particle that has mass. As such it will never go the speed of light. Such a thing is impossible.
That is true, but most pions from baryon annihilations are high-energetic (average gamma factor of 2-3 if I remember correctly), for their mean flight distance the speed of light is a reasonable approximation.

@Hurricane93: Don't forget time dilatation.
 
  • #21
mfb said:
That is very unlikely.

At least not via the electromagnetic interaction. Some pions will do inelastic collisions with nuclei, in that case they can deposit most of their energy within 5cm of iron or lead.

What about the gamma ray energy lose ?
Is the attenuation or radiation length relevant here ?
 
  • #22
The radiation length will be important for the absorption of gamma rays, right.
 
  • #23
I found something that I thing is interesting and might help here. Check this : http://www.wolframalpha.com/input/?...+200+MeV+gamma+radiation+halved+in+intensity?
For Lead and 200 MeV incident gamma rays, you only need ~6mm to absorb half the energy of the gamma rays.

So, after that, can we assume that if we could absorb 50% of the gamma rays energy, then that will contribute to the useful energy from antimatter or an explosion for example ?
 
  • #24
Hurricane93 said:
So, after that, can we assume that if we could absorb 50% of the gamma rays energy, then that will contribute to the useful energy from antimatter or an explosion for example ?
Sure.
 

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