Energy & Particles
What Is The Lawson Criteria, Or How to Make Fusion Power Viable
Mark Hoffman
First Posted: Mar 23, 2013 07:25 PM EDT
There is a magic but very simple formula that defines the criteria required to achieve energy producing fusion power. It was first formulated by a young engineer working on nuclear fusion, who in 1955 decided to work out exactly how enormous the task of achieving fusion is. Although his colleagues were optimistic about their prospects, he wanted to prove it to himself. His name was John Lawson, and his findings – that the conditions for fusion power relied on three vital quantities – became the landmark Lawson Criteria.
The genesis of Lawson’s Criteria is simple enough – he calculated the requirements for more energy to be created than is put in, and came up with a dependence on three quantities: temperature (T), density (n) and confinement time (τ). With only small evolution thanks to some subtle changes of definition, this is basically the same figure of merit used by today’s fusion scientists – the triple product, nτT.
Nonetheless the fusion collisions – between the nuclei - have to be at high speed. This allows the nuclei to overcome their electrostatic repulsion, and get close enough for the strong force – that governs fusion – to take over and stick the particles together. The speed of a gas or plasma particle is equivalent to its temperature: the second of Lawson’s criteria. Again there is a limit – if the two particles are moving really fast then the time they are in close enough proximity for fusion to occur decreases. The bremsstrahlung also increases at higher temperatures, due to faster moving electrons. The Goldilocks temperature turns out to be in the vicinity of 100 – 200 million degrees, a seemingly huge task in the fifties that has become a standard condition today.
With the first two criteria satisfied fusion reactions can occur, but to get a substantial amount of power generated you need time to allow the reactions to happen – on this basis Lawson’s third criteria comes into play, the energy confinement time. This is the time that energy remains in the plasma before escaping, and it is here that the most remarkable gains have been made during the course of fusion research. From only microseconds in Lawson’s time, the confinement time has improved by a factor of a million to reach about one second in JET and is planned to hit around 5 seconds in ITER.
It is a neat quirk of physics that conditions for achieving ignition in a tokamak depend linearly on these three quantities – just multiply them together to get an indication of your tokamak’s performance. The magic figure for ignition is a triple product of greater than 5 x 1021 m-3s keV . In its high power experiments of 1997 JET achieved around one fifth of that value.
Thanks to the years of study of fusion, our knowledge of how to achieve these criteria is very detailed. An appropriate value for density is easily achieved and tokamak heating systems have successfully created the necessary temperatures with radio-frequency heating and neutral beam injection. The remaining piece of the puzzle is the confinement time. Great improvements have been made in the plasma profiles and magnetic control that influence the confinement, but the largest improvement can be made simply by building a bigger tokamak, thereby increasing the plasma volume relative to its surface area.
John Lawson died in 2008, and so did not live to see ITER turn on. However, with its ten-fold increase over JET’s volume, the huge fusion experiment will put the last piece into place and see Lawson’s criteria finally satisfied.
See Now:
NASA's Juno Spacecraft's Rendezvous With Jupiter's Mammoth Cyclone
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First Posted: Mar 23, 2013 07:25 PM EDT
There is a magic but very simple formula that defines the criteria required to achieve energy producing fusion power. It was first formulated by a young engineer working on nuclear fusion, who in 1955 decided to work out exactly how enormous the task of achieving fusion is. Although his colleagues were optimistic about their prospects, he wanted to prove it to himself. His name was John Lawson, and his findings – that the conditions for fusion power relied on three vital quantities – became the landmark Lawson Criteria.
The genesis of Lawson’s Criteria is simple enough – he calculated the requirements for more energy to be created than is put in, and came up with a dependence on three quantities: temperature (T), density (n) and confinement time (τ). With only small evolution thanks to some subtle changes of definition, this is basically the same figure of merit used by today’s fusion scientists – the triple product, nτT.
Nonetheless the fusion collisions – between the nuclei - have to be at high speed. This allows the nuclei to overcome their electrostatic repulsion, and get close enough for the strong force – that governs fusion – to take over and stick the particles together. The speed of a gas or plasma particle is equivalent to its temperature: the second of Lawson’s criteria. Again there is a limit – if the two particles are moving really fast then the time they are in close enough proximity for fusion to occur decreases. The bremsstrahlung also increases at higher temperatures, due to faster moving electrons. The Goldilocks temperature turns out to be in the vicinity of 100 – 200 million degrees, a seemingly huge task in the fifties that has become a standard condition today.
With the first two criteria satisfied fusion reactions can occur, but to get a substantial amount of power generated you need time to allow the reactions to happen – on this basis Lawson’s third criteria comes into play, the energy confinement time. This is the time that energy remains in the plasma before escaping, and it is here that the most remarkable gains have been made during the course of fusion research. From only microseconds in Lawson’s time, the confinement time has improved by a factor of a million to reach about one second in JET and is planned to hit around 5 seconds in ITER.
It is a neat quirk of physics that conditions for achieving ignition in a tokamak depend linearly on these three quantities – just multiply them together to get an indication of your tokamak’s performance. The magic figure for ignition is a triple product of greater than 5 x 1021 m-3s keV . In its high power experiments of 1997 JET achieved around one fifth of that value.
Thanks to the years of study of fusion, our knowledge of how to achieve these criteria is very detailed. An appropriate value for density is easily achieved and tokamak heating systems have successfully created the necessary temperatures with radio-frequency heating and neutral beam injection. The remaining piece of the puzzle is the confinement time. Great improvements have been made in the plasma profiles and magnetic control that influence the confinement, but the largest improvement can be made simply by building a bigger tokamak, thereby increasing the plasma volume relative to its surface area.
John Lawson died in 2008, and so did not live to see ITER turn on. However, with its ten-fold increase over JET’s volume, the huge fusion experiment will put the last piece into place and see Lawson’s criteria finally satisfied.
See Now: NASA's Juno Spacecraft's Rendezvous With Jupiter's Mammoth Cyclone