Bussards description of WB-6 Startup, explained.
Posted: Fri May 04, 2012 3:26 am
Bussards’ IAF paper provides us some idea of how to startup WB-6. The machine was placed in a vacuum chamber. The chamber was pumped down to <1E-7 torr. The rings are now in a vacuum environment. First deuterium is puffed into the chamber. There has been talk about using ion guns to inject deuterium. However in WB-6 this injection was “gas puffed” into the chamber. Puffing gas into the vacuum raises the vacuum pressure. It is not clear if it raises the pressure to 3E-4 torr, but this startup calculation is done for that pressure. This may be some kind of error. If an expert would like to weigh into clear up this confusion we would appreciate it. This description is lifted from reference [8] on bottom of page 11. The startup calculation is done for a pressure of 3E-4 torr. However, Bussard states and shows that the WB-6 experiment started at 1E-7 torr.
Now high energy electrons are injected. They are injected using an electron gun. This “gun” makes a voltage drop from the electron source to some other point in the chamber. The electrons see the voltage, experience a Lorenz force and fall down the voltage. They pass through the gas cloud in the center. Bussard now describes a mechanism to ionize the cloud. The fast moving electrons ionize the gas inside WB-6. The fast moving electrons strip off electrons from the deuterium. This increases the number of free electrons and free ions flying around. It separates material inside the machine. Ideally, both clouds of electrons and ions have too much energy to recombine. It would not take much energy to strip off these electrons. The ionization energy for deuterium is 14.9 eV. Bussard stated in his Google presentation that the drive voltage for WB-6 was 12,500 volts. Hence, a high energy electron might come into the cloud with 12,500 eV of energy. With so much energy if it hits a deuterium atom, it will heat it up. If the deuterium is now “hotter” than 14.9 eV, the electron flies off. The gas is ionized. Now you can see one reason why the Navy wants to get several 10,000 volt electron guns for their reactor [10]. These drive beams seemed to all be within this range. Bussard stated in his Google presentation that the e-beam voltage for the PZL-1 machine (built in 2003) was 15,000 volts [19].
The number of electrons is growing inside the machine. As the electron cloud grows the cloud of ionized deuterium grows. Bussard estimated that this process happens on the order of several microseconds. He estimated that all the electrons were stripped off the deuterium in about this amount of time. At this point the beta ratio is 0.01. The beta ratio is the ratio of the plasma pressure to the magnetic field pressure. It sets the limits to this process. When the beta ratio is 1 the plasma pressure has equaled the magnetic field pressure outside. The device is full. The cloud in the center cannot handle any more electrons and ions. Past this amount and the cloud becomes unstable. This instability comes from magnetohydrodynamics. As I understand it, there is a beta ratio for the electrons and the ions. When the electron beta ratio is 0.01, Bussard estimated that the electrons are at 100 eV [8].
Now Bussard proposes that there is electron heating. Let us assume that the hot beam of electrons is still being injected. This is possible because the center is not filled up yet. In fact the magnets are not turned on. Bussard turns the magnetics on. More specifically, he starts pumping roughly 4,000 amps of current through the rings. This generates six fields. These six fields are all pointed into the center. If they were bar magnetics it would be like 6 north poles pointed into the middle. In the center there is a zone of no magnetic field, a pocket. It is a star structure with 14 points; one point pointing to each corner and each side. It may be possible that the magnetic fields reconnect. This is a totally open question. Someone needs to examine if plasma fields, under such pressures and energies would even be in the right operating conditions for reconnection. Reconnection is when magnetic fields in the presence of plasma recombine. It is a strange concept for many to understand. We are taught that magnetic field lines can never cross or reconnect. Someone please look at this: would we even expect this to happen? If it did happen, what would this mean for containment?
The electrons are coming in at 12,500 eV, and the average electron is still 100 eV and the magnetic fields are switched on. Now Bussard argues that electron heating occurs. The argument is the hot electrons hit the cold electrons in the center and impart energy. This continues until the average electron energy is 2,500 eV. Bussard calculates that the time scale for heating as 1 microsecond. Within a few microseconds, the gas is entirely ionized and in about 20 microseconds the machine is full of electrons at an average temperature of 2,500 eV. For the WB-6 test this was about a fourth the temperature of the ions. Rider would disagree here. He predicts that the ions cannot have more than 5% variation in temperature [17]. Also, the ion and electron energies supposedly equilibrate. The rate of transfer of energy essentially depends on the ratio of the number of electrons moving more slowly than the ions [18]. This is shown below.
Electron-ion Heating Rate ~ Electrons with lower energy than ion mean/ Electrons with higher energy than ion mean
Hence, Rider argues, the cloud must be at roughly one temperature.
However, if you continue with Bussards description the electron cloud is at 2,500 eV and it has created a 10,000 voltage drop in the center of the device. Using Gausses law you can estimate that the cloud in WB-6 had about 5.5E11 net electrons inside WB-6. The ions are flying in at 10,000 eV and fusing. We know that if they hit with that much energy they are in the right ballpark for fusion. NIF and ITER both are trying to get their average cloud temperatures to around 10,000 to 20,000 eV. It may be that Rider and Bussard are both correct. The average temperature of the ions could be 2,500 eV, the same at the electrons, except that the ions have a bell curve of energies. If part of that bell curve of ion energy contains ions at 10,000 eV, then fusion seems likely for a small amount of material.
Now high energy electrons are injected. They are injected using an electron gun. This “gun” makes a voltage drop from the electron source to some other point in the chamber. The electrons see the voltage, experience a Lorenz force and fall down the voltage. They pass through the gas cloud in the center. Bussard now describes a mechanism to ionize the cloud. The fast moving electrons ionize the gas inside WB-6. The fast moving electrons strip off electrons from the deuterium. This increases the number of free electrons and free ions flying around. It separates material inside the machine. Ideally, both clouds of electrons and ions have too much energy to recombine. It would not take much energy to strip off these electrons. The ionization energy for deuterium is 14.9 eV. Bussard stated in his Google presentation that the drive voltage for WB-6 was 12,500 volts. Hence, a high energy electron might come into the cloud with 12,500 eV of energy. With so much energy if it hits a deuterium atom, it will heat it up. If the deuterium is now “hotter” than 14.9 eV, the electron flies off. The gas is ionized. Now you can see one reason why the Navy wants to get several 10,000 volt electron guns for their reactor [10]. These drive beams seemed to all be within this range. Bussard stated in his Google presentation that the e-beam voltage for the PZL-1 machine (built in 2003) was 15,000 volts [19].
The number of electrons is growing inside the machine. As the electron cloud grows the cloud of ionized deuterium grows. Bussard estimated that this process happens on the order of several microseconds. He estimated that all the electrons were stripped off the deuterium in about this amount of time. At this point the beta ratio is 0.01. The beta ratio is the ratio of the plasma pressure to the magnetic field pressure. It sets the limits to this process. When the beta ratio is 1 the plasma pressure has equaled the magnetic field pressure outside. The device is full. The cloud in the center cannot handle any more electrons and ions. Past this amount and the cloud becomes unstable. This instability comes from magnetohydrodynamics. As I understand it, there is a beta ratio for the electrons and the ions. When the electron beta ratio is 0.01, Bussard estimated that the electrons are at 100 eV [8].
Now Bussard proposes that there is electron heating. Let us assume that the hot beam of electrons is still being injected. This is possible because the center is not filled up yet. In fact the magnets are not turned on. Bussard turns the magnetics on. More specifically, he starts pumping roughly 4,000 amps of current through the rings. This generates six fields. These six fields are all pointed into the center. If they were bar magnetics it would be like 6 north poles pointed into the middle. In the center there is a zone of no magnetic field, a pocket. It is a star structure with 14 points; one point pointing to each corner and each side. It may be possible that the magnetic fields reconnect. This is a totally open question. Someone needs to examine if plasma fields, under such pressures and energies would even be in the right operating conditions for reconnection. Reconnection is when magnetic fields in the presence of plasma recombine. It is a strange concept for many to understand. We are taught that magnetic field lines can never cross or reconnect. Someone please look at this: would we even expect this to happen? If it did happen, what would this mean for containment?
The electrons are coming in at 12,500 eV, and the average electron is still 100 eV and the magnetic fields are switched on. Now Bussard argues that electron heating occurs. The argument is the hot electrons hit the cold electrons in the center and impart energy. This continues until the average electron energy is 2,500 eV. Bussard calculates that the time scale for heating as 1 microsecond. Within a few microseconds, the gas is entirely ionized and in about 20 microseconds the machine is full of electrons at an average temperature of 2,500 eV. For the WB-6 test this was about a fourth the temperature of the ions. Rider would disagree here. He predicts that the ions cannot have more than 5% variation in temperature [17]. Also, the ion and electron energies supposedly equilibrate. The rate of transfer of energy essentially depends on the ratio of the number of electrons moving more slowly than the ions [18]. This is shown below.
Electron-ion Heating Rate ~ Electrons with lower energy than ion mean/ Electrons with higher energy than ion mean
Hence, Rider argues, the cloud must be at roughly one temperature.
However, if you continue with Bussards description the electron cloud is at 2,500 eV and it has created a 10,000 voltage drop in the center of the device. Using Gausses law you can estimate that the cloud in WB-6 had about 5.5E11 net electrons inside WB-6. The ions are flying in at 10,000 eV and fusing. We know that if they hit with that much energy they are in the right ballpark for fusion. NIF and ITER both are trying to get their average cloud temperatures to around 10,000 to 20,000 eV. It may be that Rider and Bussard are both correct. The average temperature of the ions could be 2,500 eV, the same at the electrons, except that the ions have a bell curve of energies. If part of that bell curve of ion energy contains ions at 10,000 eV, then fusion seems likely for a small amount of material.