Frontier physics
Nuclear fusion
Explore the conditions for thermonuclear fusion: ions in hot plasma must overcome the Coulomb barrier via the Maxwell–Boltzmann tail. Observe the roles of temperature and density and check the trend .
Equipment
- Virtual plasma chamber with thermally moving ions
- Maxwell–Boltzmann distribution plot with Coulomb-barrier region
- Sliders for relative temperature and density
Procedure
Observe ion collisions
In figure 1 "Ions in hot plasma", watch the ions move and collide; most encounters are stopped by Coulomb repulsion. Read the current temperature and density in the readout. Only ions in the high-energy tail of the distribution (aided by quantum tunnelling) can fuse.
Raise the temperature
Drag "Relative temperature" up and watch the Maxwell–Boltzmann curve in figure 2 widen, its high-energy tail thickening: . The count of ions fast enough to cross the barrier grows steeply even for a modest temperature rise — which is why stars and fusion reactors need K.
Vary density and compare
With T high, raise "Relative density": more ions means more encounters per second — the reaction rate scales as . Compare two settings (high T, low n) and (moderate T, high n): both may yield similar event counts, hinting at the Lawson criterion that a burning plasma must exceed.