The nuclear fusion reaction that is of principal interest for the purposes of energy production in a magnetically confined thermonuclear plasma is

(1.1) 
Here, D denotes a deuterium nucleus (), T denotes a tritium nucleus (), n denotes a neutron, and
denotes an alpha particle (). At achievable mean plasma temperatures (i.e., less than about 10 keV), a DT fusion reaction has a crosssection that
is approximately 100 times greater than that of a DD fusion reaction (or a TT fusion reaction) [2]. (There is, unfortunately, no HH fusion reaction.) For this reason, DT fusion is considered to be
more practical than DD fusion, despite the fact that there is no natural source of tritium on the Earth. In fact, it is envisaged that DT
fusion reactors will breed the requisite tritium within a blanket that surrounds the plasma via nuclear reactions such as

(1.2) 
Note that makes up 7.6% of terrestrial lithium, which makes up about 0.002% of the Earth's crust.
A DT fusion reaction liberates

(1.3) 
of kinetic energy
that is subsequently carried off by the fusion products [2]. In a thermonuclear plasma, the momenta of the fusion products exceed those of
the fusion reagents by many orders of magnitude, so the fusion reaction effectively takes place in the center of mass frame. Consequently, momentum
and energy conservation require each product to carry off a fraction of the liberated energy that is inversely proportional to its mass (given that the
products are moving nonrelativistically) [22]. Now, the masses of a neutron and an alpha particle are
and
, respectively. Hence, the
kinetic energies of the neutron and the alpha particle generated by a DT fusion reaction are
respectively. In a magnetic confinement device, the alpha particles generated by DT fusion reactions are confined by the magnetic field that permeates the plasma, and subsequently slow down and
heat the deuterium and tritium nucleii, thereby, maintaining the nuclear fusion reactions. On the other hand, the neutrons generated by DT fusion reactions exit the plasma, and are absorbed in the surrounding blanket. The energy absorbed by the blanket is extracted via a conventional heat exchanger, and used to generate
electrical power. As has already been mentioned, the neutrons also breed tritium within the blanket, thereby, replacing the tritium burned up in the fusion reactions.
Figure 1.1:
DT fusion reactivity plotted as a function of the assumed common temperature of the fusion reagents.

Consider a thermonuclear plasma consisting, principally, of electrons, deuterium ions (that are fully stripped of electrons), and (fullystripped) tritium ions. All three species are assumed to have have Maxwellian
velocity distribution functions characterized by a common temperature, . The rate of DT fusion reactions occurring per unit volume within the plasma is [50]

(1.6) 
where is the deuteron number density, the triton number density, the crosssection for DT fusion reactions, the relative
velocity of the reacting species, and
denotes an average over the Maxwellian distributions of the reacting species. In the range of temperatures
– keV, the DT fusion reactivity,
, is accurately fitted by the following formula [2,4]

(1.7) 
where
Here, is measured in units of keV. The parameters – are specified in Table 1.1.
Figure 1.1 plots
for a realistic range of plasma temperatures. It can be seen that
is a rapidly increasing function of increasing temperature, and that
when
keV.
Table:
Parameters for formulae (1.7)–(1.9)
