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The energy confinement time is simply the time it takes the fusing plasma to expand.

The record for the longest confinement time is around one second, held by the Joint European Torus (Jet) reactor at Culham.

The knowledge of the plasma temperature and density, together with the energy confinement time, is therefore very important for the effective control of the self-sustained fusion reactor.

Therefore, input power time (energy confinement time) is one of the most important parameters of the plasma ignition in tokamaks [1, 2, 3].

The confinement time is measured as before for this condition inside the trap: Fig. 10 End cap of trap fitted with protruding filament in the trap volume.

However, the confinement time is finite due to several reasons that include collisions with the surrounding neutrals, anharmonicities in the trap potential induced by deviations from the ideal geometry of the trap, and in situations involving a large number of charged particles, space charge effects in the trap [5].

Optimal combinations of magnetic shape, temperature and density profiles as well as the confinement time are identified as advanced regimes.

The flat-top of the discharge can last a couple of seconds (i.e. half the diffusive resistive time and twice the energy confinement time), and is limited by the heating of the toroidal field coils.

The maximum energy confinement time can be determined by the microscopic behavior of the plasma such as collisions and microinstabilities.

Finding evolution of (Lambda) and (l_i) form Eqs. (22) and (28), qualitative evolution of the plasma energy confinement time can be found in term of (beta _p) using energy balance Eq. (1).

The number of individuals in solitary confinement/administrative segregation at any given time is not easily ascertained, largely because of the variance in record keeping and reporting among the U.S.'s city, state, and federal prisons, detention facilities, and jails.