In a controlled fusion reactor Deuterium-Tritium The temperature of the plasma is T keV, where k is the fusion is occurring. 10 k Boltzmann constant. The ions' m-3 number density is 2.6 × 10¹8 Moreover (ov) = 10-2²m³s-¹, 3 where o is the reaction cross-section, v is the relative speed of the reacting particles, and represents averaging according to the Maxwell- Boltzmann distribution. = For what value of the confinement time does the reactor achieve the break even point? Enter your answer in seconds to 1 decimal point.

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In a controlled fusion reactor
Deuterium-Tritium
The temperature of the plasma is
T = 10 keV, where k is the
k
Boltzmann constant. The ions'
number density is 2.6×10¹8 m-3.
-22
3
Moreover (ov) = 10-²²m³s-¹,
where o is the reaction cross-section,
v is the relative speed of the reacting
particles, and represents
averaging according to the Maxwell-
Boltzmann distribution.
fusion is occurring.
For what value of the confinement
time does the reactor achieve the
break even point?
Enter your answer in seconds to 1
decimal point.
Transcribed Image Text:In a controlled fusion reactor Deuterium-Tritium The temperature of the plasma is T = 10 keV, where k is the k Boltzmann constant. The ions' number density is 2.6×10¹8 m-3. -22 3 Moreover (ov) = 10-²²m³s-¹, where o is the reaction cross-section, v is the relative speed of the reacting particles, and represents averaging according to the Maxwell- Boltzmann distribution. fusion is occurring. For what value of the confinement time does the reactor achieve the break even point? Enter your answer in seconds to 1 decimal point.
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