PHYSICS LAB
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NUCLEAR PHYSICS · INTERACTIVE LAB 72

Nuclear fusion

Explore how temperature, density, confinement and quantum tunnelling influence fusion in an idealised plasma.
Deuterium–tritium plasmaFusion occurring · not self-sustaining
DeuteriumTritiumHeliumNeutron
Temperature12.0 units
Fusion events0
Close encounters0
Fuel remaining180
Energy released0 MeV
Triple product—

Fusion events over time

Energy balance

Particle-energy distribution

Overcoming repulsion

Positive nuclei repel through the Coulomb force. High temperature raises collision energy, while quantum tunnelling gives some close encounters a chance to fuse below the classical barrier.

Three requirements together

Fusion performance depends on density, temperature and energy-confinement time. Raising only one is not enough—the Lawson triple product summarises their combined effect.

Where the energy comes from

Light nuclei can combine into a more tightly bound nucleus. The mass difference appears as kinetic energy according to Q=(mᵢ−m𝒇)c²; energy is transformed, not created.

Model limitation: Collision probabilities are artificially accelerated, dimensionless teaching values rather than reaction cross-sections. The displays do not predict the performance of any real star, tokamak or inertial-fusion facility.