So I have given it. What of the electron energy budget? How many 80MeV electrons do you need to create for each fusion to take place?Joseph Chikva wrote:Certainly I want more qualified criticism.
Cyclic Fusion Reactor. Colliding Beams.
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I am ready to discuss 33MeV electrons for the following example:chrismb wrote:So I have given it. What of the electron energy budget? How many 80MeV electrons do you need to create for each fusion to take place?Joseph Chikva wrote:Certainly I want more qualified criticism.
Deuterium+Tritium Reaction
• Deuterium – 300 keV
• Tritium – 200 keV
• Center-of-mass collision energy – 20.2 keV
• Reaction cross section – 0.4 barn
• Ions’ relative velocity – 1.8*10^6 m/s
• Electron – 33 MeV
• Relativistic factor of electrons – 65.6
For the frame of reference connected with Deuterium beam this corresponds to electron’s relativistic factor equal to 66.7 and for Tritium – 66.3)
For condition that ions in their frame of reference should be in negative potential well we need the less electron number dencity:
-for Deuterium - 1/4449
-for Tritium - 1/4395
Deuterium nuclei has velocity =0.018c and Tritium =0.012c and electron 0.9999....c
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And for effective pinch the required current of electron beam should be more than only ~1/52.6 of current of Tritium beam and ~1/80 of Deuterium.chrismb wrote:The question is the energy budget - how many electrons do you need to generate for each fusion reaction?
And from these reasonings we can accept the ratio between electron and Tritium and Deuterium currents equal to 1/50 and 1/75 correspondently.
The raw estimation of required energy that should to be put into the beams specified on a single fusion event (initial energy consumption of a single fusion event)
In case if only 80% of nuclei will react initially we should spend per one fusion event:
(300keV+1/75*33MeV+200keV+1/50*33MeV)/0.8=2MeV
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No, sorry, it was comprehending your meaning, so I deleted the message after I comprehended it and decided I needed to re-phrase it, but you seem to be on line permanently and answered immediately before I deleted. I was expecting A ratio; electrons per fusion.
What is the argument you put forward for this ratio? What is the loss rate at the end of the device? Remember, 'current' and 'total population' are different for charges at different velocities.
What is the argument you put forward for this ratio? What is the loss rate at the end of the device? Remember, 'current' and 'total population' are different for charges at different velocities.
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Argument is simple: mentioned above number densities correspond to mentioned electron currents which should then be summarized.chrismb wrote:What is the argument you put forward for this ratio? What is the loss rate at the end of the device? Remember, 'current' and 'total population' are different for charges at different velocities.
Energy losses via braking radiation and also we should compensate the alignment of ions velocities. And in the same electric field Deuterium nuclei have higher rate of acceleration.
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For example we can build reactor into each impulse of which we will put the following energy:
• 3MJ for deuterium
• 2MJ for tritium
• 11MJ for electrons
And repeatability 10Hz
This is rather costly. Energy storage capacitors are very expensive. For example General Atomic produces high quality capacitors for these application and 2MJ costs about 20-25 millions USD.
• 3MJ for deuterium
• 2MJ for tritium
• 11MJ for electrons
And repeatability 10Hz
This is rather costly. Energy storage capacitors are very expensive. For example General Atomic produces high quality capacitors for these application and 2MJ costs about 20-25 millions USD.
But Argument doesn't provide all details!Joseph Chikva wrote:Argument is simple: mentioned above number densities correspond to mentioned electron currents which should then be summarized.
Energy losses via braking radiation and also we should compensate the alignment of ions velocities. And in the same electric field Deuterium nuclei have higher rate of acceleration.
You would need to know the residence time of an electron in your device to relate current with density. Very fast streams will give lower density for a given current. Slower streams have higher density for given current. How fast - and for how long (i.e. energy confinement time of electrons?).
What does analysis say for electron energy confinement time versus power output?
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Electron and ions or in other words non-neutral plasma have the same confinement time. And besides that they are in potential well of each other they also confined by external fields of betatron type device.chrismb wrote:But Argument doesn't provide all details!Joseph Chikva wrote:Argument is simple: mentioned above number densities correspond to mentioned electron currents which should then be summarized.
Energy losses via braking radiation and also we should compensate the alignment of ions velocities. And in the same electric field Deuterium nuclei have higher rate of acceleration.
You would need to know the residence time of an electron in your device to relate current with density. Very fast streams will give lower density for a given current. Slower streams have higher density for given current. How fast - and for how long (i.e. energy confinement time of electrons?).
What does analysis say for electron energy confinement time versus power output?
Or you are asking the feasible confinement time?
Betatron by its method of creating of circular electric field very similar to TOKAMAK as on both devices plasma torus and circulated beam considered as secondary winding of transformer.
We will have lower circulated current and much lower temperature. In TOKAMAKs confinement time has seconds order.
And we need about tens milliseconds as projected repeatability of device is 10Hz.
Dubious claim, especially when electric potential wells are involved. Can you back it up?Joseph Chikva wrote:Electron and ions or in other words non-neutral plasma have the same confinement time.
Electric potential and cyclotron radius (related to mass/charge ratio) both have an impact on particle confinement time.
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In case when electric potential wells are not involved confinement time equal to zero.hanelyp wrote:Dubious claim, especially when electric potential wells are involved. Can you back it up?Joseph Chikva wrote:Electron and ions or in other words non-neutral plasma have the same confinement time.
Electric potential of what?hanelyp wrote:Electric potential and cyclotron radius (related to mass/charge ratio) both have an impact on particle confinement time.
If impact
Cyclotron radius how? What do you think increasing radius we increase or decrease confinement time?

Feasible confinement time depends on development of instabilities. And not on nothing else. As the offered system cinematically (single particle’s behavior) is absolutely stable.
Strictly speaking the instabilities task can not be solved analytically. But on base of common experience and taking into account that the offered confinement concept is very similar to TOKAMAK and also the temperature in device is much lower than in TOKAMAK, we can wait that the feasible confinement time will not be less than in at least in TOKAMAKs (seconds order) and we need only milliseconds.
High relativistic factor of electrons should also add the stability as it has been proved by G.I.Budker.
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I just calculated energy consumption for the following parameters:
• Deuterium - 450keV
• Tritium - 300keV
• Electron - 40.6MeV
And energy consumption specified per a single fusion event is about 1.8MeV
Taking into account that collision energy in center-of-mass frame for this case is 30keV (30keV vs. 20.2keV) and so ratio between fusion and scattering sections is more attractive, we should also wait less further energy losses that for previous case estimated as 0.7MeV per each event.
• Deuterium - 450keV
• Tritium - 300keV
• Electron - 40.6MeV
And energy consumption specified per a single fusion event is about 1.8MeV
Taking into account that collision energy in center-of-mass frame for this case is 30keV (30keV vs. 20.2keV) and so ratio between fusion and scattering sections is more attractive, we should also wait less further energy losses that for previous case estimated as 0.7MeV per each event.